centre of excellence in smart radios and wireless...

55
SMARAD Activity Report 2011 Centre of Excellence in Smart Radios and Wireless Research Antti Räisänen (editor)

Upload: dangtuong

Post on 16-Mar-2018

242 views

Category:

Documents


2 download

TRANSCRIPT

Page 1: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

SMARAD Activity Report 2011

Centre of Excellence in Smart Radios and Wireless Research Antti Räisänen (editor)

Page 2: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

2

Contents

1 Introduction to SMARAD 2 Research teams 3 Highlights of SMARAD research in 2011 - Future Radio and Antenna Systems - Cognitive Radio - Millimetre Wave and THz Techniques - Sensors - Materials and Energy 4 Participation in European projects 5 SMARAD funding 6 SMARAD personnel during 2011 7 Visitors to SMARAD 8 Visits from SMARAD to foreign institutes 9 Post-graduate degrees 10 Publications 11 Other scientific activities of SMARAD members

Page 3: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

3

1. Introduction to SMARAD Centre of Excellence in Smart Radios and Wireless Research (SMARAD) In 2001 the Academy of Finland appointed SMARAD with the name “Smart and Novel Radios Research Unit” as one of the centres of excellence in research for the period 2002–2007. In 2006 the Academy announced its decision that the renewed SMARAD (“Centre of Excellence in Smart Radios and Wireless Research”) was appointed a Centre of Excellence for years 2008–2013. According to the Academy: “Centres of excellence are research units or researcher training units which comprise one or more high-level research teams that are at or near the international cutting edge of research in their field. They will also share a common set of objectives and work under the same management. Funding for centres of excellence comes not only from the Academy, but also from the host organisations of the units concerned, and possibly from other funding bodies, such as Tekes, business enterprises and foundations. A centre of excellence may be a unit of research teams working at both universities and research institutes.” Currently there are altogether 33 Centres of Excellence: the Academy Board has appointed 18 centres of excellence for the national centre of excellence programme in 2008–2013 and 15 for the years 2012–2017. The current SMARAD was formed in 2006 by the Radio Laboratory, the Electronic Circuit Design Laboratory and the Signal Processing Laboratory of the Department of Electrical and Communications Engineering, Helsinki University of Technology (TKK). After the restructuring of the TKK organization, SMARAD involves research groups from three departments, namely the Department of Radio Science and Engineering, Department of Micro and Nanosciences, and Department of Signal Processing and Acoustics, all within the Aalto University School of Electrical Engineering. SMARAD provides world-class research and education in RF, microwave and millimetre wave engineering, in integrated circuit design for multi-standard radios as well as in wireless communications. In microwave and millimetre wave engineering it is also the only research unit in Finland. SMARAD is a contributor to MilliLab, ESA External Laboratory (a joint institute between VTT and Aalto University School of Electrical Engineering). The total number of employees within the research unit is about 90 including about 30 senior scientists and about 40 doctoral students and several students working on their Master thesis. The unit conducts basic research but at the same time maintains close co-operation with industry. Novel ideas are applied in design of new communication circuits and platforms, transmission techniques and antenna structures resulting also in patents and invention reports. ‘Smart’ in SMARAD’s name refers to adaptability of antennas, radio devices, or materials to RF signals or fields. SMARAD has a well-established network of co-operating partners in industry, research institutes and academia worldwide. It coordinates a few EU projects. The funding sources of SMARAD are also diverse including the Academy of Finland, Tekes, and the Finnish and foreign telecommunications and semiconductor industry. As a by-product of this research SMARAD provides highest-level education and supervision to graduate students in the areas of radio engineering, circuit design and communications through Aalto University and Finnish graduate schools such as GETA. SMARAD Principal Investigators are: Prof. Antti Räisänen, chairman: Millimetre wave and THz techniques Academy prof. Visa Koivunen, vice-chair: Communications and statistical signal processing Prof. Kari Halonen: Electronic circuit design Prof. Sergei Tretyakov: Advanced artificial electromagnetic materials and smart structures Prof. Pertti Vainikainen: RF applications in mobile communications and non-destructive testing

Page 4: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

4

Members of the Scientific Advisory Board of SMARAD are (2011): Prof. Danielle Vanhoenacker-Janvier, Université Catholique de Louvain (UCL), Belgium Prof. Björn Ottersten, Royal Insitute of Technology Stockholm (KTH), Sweden Professor Heli Jantunen, Oulu University Professor, Vice-Rector Heikki Mannila, Aalto University Dr Ritva Dammert, Aalto University Dr Kati Sulonen, Academy of Finland Dr Hannu Kauppinen, Nokia Research Center Dr Jani Ollikainen, Nokia Research Center

2. Research teams 1. Millimetre wave and THz techniques. The research group is led by Prof. Antti Räisänen.

There are 3 other senior researchers with a doctoral degree (Dr. Juha Mallat, Dr. Juha Ala-Laurinaho, and Dr. Dmitri Lioubtchenko) and 6 researchers working towards their doctoral degree. In addition, Prof. Constantin Simovski works part-time in this group.

2. Advanced artificial electromagnetic materials and smart structures. This research group is led by Prof. Sergei Tretyakov. Prof. Constantin Simovski works in this group. The research group includes 3 other senior researchers, and 5 researchers working towards their doctoral degree.

3. RF applications in mobile communications and non-destructive testing. This research group is led by Prof. Pertti Vainikainen. There are 6 other senior researchers with a doctoral degree (Dr. Katsuyuki Haneda, Dr. Jari Holopainen, Dr. Clemens Icheln, Dr. Veli-Matti Kolmonen, Dr. Tommi Laitinen, and Dr. Valeri Mikhnev) and 9 researchers working towards their doctoral degree.

4. Communications and statistical signal processing. The research group is led by Academy prof. Visa Koivunen. Prof. Risto Wichman works full time in this research group. In addition, there are 5 other senior researchers with a doctoral degree in the group. There are 9 researchers working towards their doctoral degree.

5. Electronic circuit design. The research group is led by Prof. Kari Halonen. Prof. Jussi Ryynänen works full time in this research group. The group includes 2 other senior researchers with a doctoral degree and 11 researchers working towards their doctoral degree.

3. Highlights of SMARAD research in 2011 The Centre of Excellence in Smart Radios and Wireless Research, SMARAD, specialises in research into RF, microwave and millimetre wave techniques, integrated circuit design for multi-standard radios as well as wireless communications. Areas of special interest include RF techniques for wireless data communications, radio channel modelling and measurement, new and smart materials and structures, smart (adaptive) antennas, integrated circuit design for multi-standard radios, receiver structures and architectures and the signal processing algorithms they require. The results will have practical application especially in future wireless communication systems. In the following the SMARAD research in 2011 is described under the following titles: Future radio and antenna systems, Cognitive radio, Millimetre wave and THz techniques, Sensors, and Materials and energy.

Page 5: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

3.1 Future demandpropagawhere dtransceismallersome dimproveMIMO,evolutioIn addispectrumwide amechanarea comrates an Antennmethodmobile side of exposurkind of when hthe antemore gantennadesigneelementimproveabsorptstructurbe used

Fig. 1: the pha

Future R

wireless syds continueation to sysdifferent syivers. More, networks

deploymentsed simultan, closed-looon of DVB-ition, futurem use and carea coveranisms to supmmunicatio

nd autoconfi

na shieldind was introd

terminal anthe mobile

re (SAR) lif antenna coolding the menna elemengenerally deas, a shieldeed and evalt is selectede the total ion rate (SAre. At 2000 d also to sign

(a) Fabricantom hand

Radio and

ystems demes to be a stem concepystems coexeover, intermay be sins (e.g. pico

neously giviop MIMO, m-T/H, DVB-e wireless cooperativeage, while pport, e.g., mons combinigurability o

g reduces duced to rentennas at 9e handset thimits are monfigurationmobile termnt, reducingecrease the ed antenna luated (Figd and the oefficiency

AR) in the MHz, the b

nificantly d

ated shieldeand the gen

Antenna

and ever hichallengin

pts. The futuxist in the rference ma

ngle frequeno-cell and ing rise to dmultiuser M-T2 and DVsystems re

e techniquesWLAN h

mobility, neing the mobof WLAN w

interactioneduce the e900 and 20hat points a

more easily mn is far fromminal in bothg the radiati

effect of structure th. 1). Depen

other is actinwith hand head by 81benefits areecrease the

ed antenna pneric SAM h

5

a Systems

igher data rng and widure of wiresame band

anagement ncy networkfemto-cell

different muMIMO, as wVB-NGH. equire new s. So far wihas targeteecessary to wbility and s

would be hig

n between ffect of the

000 MHz. Taway from met and th

m being opth hands to btion efficienthe hand a

hat consists nding on thng as a shiand head b

1% at 900 Me 2.1 dB and

SAR in the

prototype, ahead filled w

rates and wde researchless commu

ds requiringis a majo

ks and netwdeploymen

ultiple antenwell as dive

network tireless cellued short-ranwide area s

services of cghly desirab

user and e hand and Traditional the head (ine antenna ptimal in mabrowse the ncy and cauand head oof two non

he use poseld. It is shby 5.0 dB MHz compad 43%, respe hand.

and (b) meawith tissue-e

wider bandwh topic ranunications ig highly fler issue sin

work planninnts). Spectranna techniqersity transm

topologies cular systemsnge commystems. Syscellular sysble.

mobile terhead of a

antenna elen talk positperformanceany other usinternet, the

using frequen the oper

n-self-resonaition, the b

hown that thand decreasared to the pectively. Th

asurement sequivalent l

widths, and nging from is strongly hexible and nce cell sizng may notal efficienc

ques includimission sch

characterizes have been

munications stem architestems as we

rminal anteuser on th

ements are tion). This e is better. se positionse user's fingency detuniration of mnant antennabetter-perfohe proposedse the maxtraditional

The shieldin

set-up in RAliquid.

meeting thantennas

heterogeneoreconfigura

zes are gettt be feasiblecies shouldng cooperat

hemes for, e

ed by flexin optimized

and it laecture for loell as high d

enna. A nhe operation

placed on tway, radiatHowever,

s. For instangers may cong. In orde

mobile termia elements wrming anted structure

ximum specsingle elemg structure

AMS includin

hese and ous, able ting e in

d be tive e.g.,

ible for

acks ocal data

new n of that tion this nce, over r to inal was nna can

cific ment

can

ng

Page 6: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

Effect oantennadevice astudied efficienaffected7–11 dBpower athe matthe totaclearly the low

Fig. 2: Multi-adifferenthe impdeal withe variof greator two informadiversitimportathe estimnegativdrop ofinfluenceffect oalmost n

of the useras for mobiand their ef

with simuncy, and fard by the preB comparedabsorption itching (detual efficiencyincreased t

wer UHF-ban

Measured

antenna mnt propagaplementationith mutual ciable effect t importanchands at o

ation for mty terminal ance to takemation of the influencef the antence on EDG

of the incidenegligible.

r’s hands ole terminalsffect on the ulations anr-field direcesence of thd to the frein the hand(uning of they of the antthe understand antennas

total efficie

obile termation environ of multi-acoupling thaof the hande, especiallyone time, a

multi-antennis in the

e into accouhe diversity

e on Effectinna radiatioGs due to thent wave pa

on the opers, the interaperformanc

nd measurectional pattehe user’s haee space ca(s) is genere antenna). tenna can evanding of ths.

ency (left) fo

minal diversonment conantenna eleat depends d on the moy with the cas shown ina designersproximity

unt the distoy performanive Diversiton efficienche power imarameters o

6

ration of maction of dice of lowerements of ern of an in

ands. In the ase as showrally more sOn the otheven be imphe effect of

or the brows

sity perfornditions. In

ements in mon the num

obile termincurrent trendn Fig. 3. Ts on termin

to the reaorted radiatince. Accordty Gain (EDcies. b) Thembalance bf the propa

mobile termifferent anter UHF-band

a prototypnternal broaworst case,

wn in Fig. 2severe for ther hand, it w

proved due f the user’s

sing grip (r

mance in nstead of in

mobile termimber of antenal performad of people Therefore, tnal diversityalistic humion patterns

ding to our fDG) which e cross poletween thegation envi

inal antennenna parts w

d antennas ipe antennaadband digi, the antenn2. The resulhe total efficwas also shto the handhands on th

ight) of the p

proximity ncreasing thinals, antenenna elemenance metricholding the

there is a ny performaan hand g

s due to the findings: a) is mostly a

larization rpartial pow

ronment on

nas. Duringwith the usin handhelda. The inpuital televisiona efficiencylts also indciency than

hown that inds of the ushe operation

prototype a

to human he spectral enna designernts, as well cs. The gripe terminal uneed to pro

ance, especigrips. It is

human han The humanattributed tratio value wer gain pan the EDG p

g the designser holding d terminals wut impedanon antenna y decreased

dicated that n the changen certain caser. The resn of especi

antenna.

hands unefficiency wrs also haveas to consi

p of the hanusing either ovide essenially when of paramo

nds beforehn hands havo the dramhas import

atterns. c) Tperformanc

n of the

was nce, are

d by the

e of ses, ults ally

der with e to ider d is one

ntial the

ount hand ve a

matic tant The e is

Page 7: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

Fig. 3: Angulachanneparametdata. Inon the componchannelpropagaThe dencharacteof the Dresults betweenDetailedpropagamore spclearly effect o MIMOongoingone protest systsystem,for syntsize of using th

Multi-ante

ar and shaels. The curterized bas

n practice, mplane wav

nents (SC) cl, i.e., the ation channnse multipaerized by uDMC were showed than 10% and d analysis oation mechapread in theconcentrate

on both the S

O over-the-g. Anechoicomising cantem, the req, has been ethesizing ththe device

he well-kno

nna implem

adowing crrent geomeed on radio

most parameve assumptcapture onlydense multel. ath compon

using the spanalyzed in

at the contri95%, being

of the powanisms of t

e angular doed around tSC and DM

-air testingc chamber andidate for Mquired numbexamined inhe radio prounder test (wn spherica

mentation in

haracteristetry based sto channel peter estimatition. Howey a part of ttipath comp

nents (DMCecular comp

n indoor envibution of tg generally er-angular pthe SC and omain in thehe same an

MC.

g. Developmand fading MIMO-OTAber of probe

n our work. opagation c(DUT) in wal wave theo

7

n a mobile h

tics of dentochastic mparameter eion algorithever, it hasthe propagaponents (D

C) represenponents (SCvironments the DMC tohigher in n

profiles shod DMC have DMC thanngles as in t

ment of Memulator baA testing. Aes for synthWe have p

channel insiwavelengthsory.

handset with

nse multipmultiple-inpu

estimates exhms used to s been repated energy,

DMC), has

nt the part C). In this sbased on e

o the total rnon-line-of-owed that, ve large simn in the SC,the SC. Th

MIMO over-ased multi-

A crucial ashesizing theresented ruide the muls and the un

h different h

path compout multiple oxtracted froparameteriorted that , and that ala significan

of the radiostudy, the pxtensive chreceived po-sight than in all the in

milarities. Ev, the energye shadowin

-the-air (OTprobe test s

spect largely desired fieles for the nlti-probe syncertainty le

hand grip m

onents in output chanom channelize these mo

these so-clso the residnt impact

o channel tpropagation hannel measower can vain line-of-snvestigated

Even thoughy in the DMng objects c

TA) test msystem showy dictating

elds inside tnumber of pystem as a fevel of the

odels.

indoor rannel models l measuremodels are bacalled specudual part of on the ove

that cannotcharacteris

surements. Tary as muchsight scenard scenarios, h the energy

MC is, howevclearly have

methodologywn in Fig. 4the cost of he multi-pr

probes requifunction of field synth

adio are

ment ased ular

f the erall

t be stics The h as rios.

the y is ver, e an

y is 4 is

f the robe ired the

esis

Page 8: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

Fig. 4:

Calibrasystemsdevicespropagafields arprobe simportaproposeThis caprovidethe neavalidateFigure considewhere calibrat

Fig. 5: effects acompen Relays networknovel n

Illustration

ation proces are an ats. Circular ation channrriving fromsystem suffantly, the se a calibratialibration pre the requirear-field anded by compu5(a) show

ered withouthe propos

tion techniq

The z compare include

nsation tech

in wirelessk nodes cannetwork top

n of a MIMO

edure for 2ttractive alt2-D multi-

nel conditiom the horizofers from thscattering frion procedurocedure is ed excitatio

d scattering uter calculas the field

ut applying sed calibratque for parti

(a) ponent of thed (a) withonique.

s communicn be used tpologies. R

Fadingemulat

CommTester BS Em

O-OTA test

2-D MIMOternative fo-probe systeons where tontal plane. he fact thatfrom the neure to partia

based on twon coefficien

effects insations. d inside the

any competion technially compen

he electric fout applying

cation systeto increase Relays can

gtor

unication/

mulator

8

system bas

O over-the-aor MIMO ems providthe incomin The accurat the probeseighbouringally compentwo measurnts for the side the tes

e test zoneensation tecique is connsating the

field in the tg the comp

ems. Relaythroughputbe classifi

Anechoi

ed on multi

air multi-pover-the-air

de a good ng fields toacy of the ps are locateg probes. Tnsate those rement stepsprobes for

st zone. Th

e where bochnique andnsidered. near-field a

test zone wipensation te

s that receivt or extend ied into am

ic chamber

DUT

-probe tech

robe test syr testing omeans for

o the mobillane wave fed in the nThis researc

near-field as and relateenabling th

he proposed

oth near-fied Fig. 5(b)

The resultand scatterin

(ith both the echnique, an

ve and retracoverage o

mplify-and-f

hnology.

ystem. Mulof mobile c

synthesizinle device afield synthe

near field anch work isand the scaed data proche partial cod calibration

eld and theshows the t validates ng effects in

(b) e near-field nd (b) after

ansmit the sof networksforward (A

lti-probe bacommunicatng such radare plane-wesis with mund, even m conducted

attering effecessing, wh

ompensationn procedure

e scatteringtest zone fithe propo

n the test zo

and scatterr applying

ignals betws and facili

AF) relays

ased tion dio-

wave ulti-

more d to ects. hich n of e is

g is field osed one.

ring the

ween tate and

Page 9: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

decode-decode From sibetweeninformatechniquresourctechniquenhance 

Full-dumode, iband) fuand recantennaand thelevels,. does noseveral Full-duptechniqumay opamountcombinbe incorOur resduplex

Fig. 6:interfer Dirty Rwirelessthe hetbandwifocus oamplifienonideaemphassystem mitigati

-and-forwarthe receive

ignal procesn multiple ation in muues for dige sharing bues in muled wireless

uplex commi.e. they do

full-duplex mceive antennas. Implemeeir operationOn the oth

ot require twsystem paraplex MIMues in RF d

ptimize spatt of side infne these tworporated intearch develnetwork no

: Loop intrence.

RF. Buildins systems, iterogeneousdths togeth

on developiner nonlineaalities in A/sis is on th

performancion of RF i

rd (DF) relad signal, enssing point relays, ch

ultihop netwgital filter dbetween traltiple accesnetworks. 

munication not transmmode. The lnas to reduentation cosn range is er hand full

wo channel ameters, e.g

MO transcedomain andtial transmiformation oo approacheto analyticalops concep

odes.

terference

ng flexible, is not straigs radio enher with higng deep un

arities, oscil/D convertee analyticalce in closempairments

ays. The forncode the sig

of view AFannel estimworks. Specdesign. DF ansmit and ss systems.

s. Relays limit and recelatter operat

uce loop-bats of full-dulimited detl-duplex relresources f

g. the symmivers inevd digital bait and receion the channes. In additiol performan

pts and analy

cancellation

compact, hhtforward. vironment

gh data ratenderstandinglator phase rs, effect thl work to c

ed-form, ans.

9

rmer ones rgnal again, F relays offemation and ctral shapinrelays, for receive sl

Our resea

ike other weive simultation typical

ack interfereuplex transctermined bylays may imfor receptio

metry of the vitably requaseband, theive filters tnels (left), oon to algorince studies aysis for wir

n in spatia

high-qualityOn one hanand flexib

es would rag, how the noise, mirr

he performacharacterize

nd to develo

etransmit thand transmer interestin

equalizationg of the trone, offer

lots and dearch develo

wireless trananeously in lly requires ence from tceivers are hy transmit amprove syston and trans

traffic betwuire adaptie latter beino mitigate or subtract ithm designas well. reless comm

al domain

y, and yet lnd, re-configble spectruather requir

most essenror frequenc

ance of widee the resultop digital s

he signal wiit. 

ng challengeon and utilransmitted various pos

evelop jointops concept

nsceivers mthe same fa spatial septhe transmihigher than and receiveem through

smission. Gween the netive loop ng outlined loop interfethe estimat

n, the effect

munication s

or subtra

ow-cost radgurable archm use. On

re dedicatedntial analogcy interfereeband multiing distortisignal proce

ithout decod

es in terms lization of signal requssibilities tot encoding ts and anal

may operate frequency beparation beit antennas those of ha

e powers anhput when th

Gains, howevtwork nodesinterferencein Fig.6. T

ference baseted interfereof loop int

systems con

action of e

dio equipmhitecture is n the othed hardware g RF impaience due to iantenna traion and theessing algo

ding DF rel

of cooperatchannel s

uires advano optimize and decod

lysis for re

in half-dupband, or in tween transto the rece

alf-duplex ond interferehe transceivver, depends. e cancellatThe transceied on difference (right)erference m

nsisting of f

estimated lo

ments for futrequired gi

er hand, wsolutions.

irments, powIQ imbalan

ansceivers. Teir effect onorithms for

lays

tion tate

nced the

ding elay

plex (in-

smit eive ones ence vers d on

tion iver rent , or

must

full-

oop

ture ven

wide We wer nce, The n to the

Page 10: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

10

 

Multiantenna systems. The goal is to derive transceivers and transmission schemes that exploit all the degrees of freedom in radio channels to achieve high spectral efficiency, high system throughput, extended range as well as powerful interference cancellation capability. In general, practical multiantenna systems require some channel state information in the transmitter, because otherwise interference between different data streams and users becomes too large in the receiver. The main research problem is then to optimize the tradeoff between the system performance and the required feedback information from receivers to transmitters. In case of cooperative and multipoint MIMO techniques, multiple transmitters simultaneously transmit to a user, which is especially advantageous when the user is located on the edge of the coverage area. With multiuser MIMO techniques the same channel resource is shared with multiple network nodes aiming to further improve the throughput of network. Concerning heterogeneous wireless systems and spectrum sharing, cooperative and multiuser MIMO algorithms should operate in decentralized manner assuming that network nodes possess only limited information on the state of the system. These kind of distributed techniques are further elaborated within wireless sensor networks. Distributed and resource efficient parameter estimation in wireless sensor networks. The objective is to develop distributed detection and estimation schemes for detecting an event and estimating and tracking an unknown common parameter, e.g., temperature, level of water contaminants, or a target position, using multiple displaced sensors. Signal collection through a distributed network of sensor nodes improves robustness of performance and reliability of the network due to redundancy and provides spatial diversity due to multiple viewing angles. In the particular case of sensor networks, the bandwidth and power requirements are closely linked to whether the acquired data is processed in a centralized or a decentralized manner, see Fig. 7. In the former approach, signals from all sensor nodes are processed jointly in one centralized fusion center, thus, facilitating the use of battery operated and low-cost sensors. For a large network, the excessive amount of data can make central processing computationally prohibitive, and may require communications over longer range which leads to reduced battery life. Comparing to the centralized estimation approach, decentralized (or distributed) detection and estimation reduces the amount of data that each estimator needs to process by introducing collaboration between neighboring nodes in the network. Collaboration improves algorithm robustness, e.g., in case of sensor failures; however, it increases bandwidth and power requirements. As an alternative to classical approaches, this research project aims to develop distributed estimation algorithms with sensors that can make discerning use of received data, thereby providing more informative estimates and thriftier use of resources like power and bandwidth. Thus the nodes should update the parameter estimates only when needed and cooperate only when such an action improves awareness. The amount of data transmitted in a sensor network can be effectively reduced via censoring where data is transmitted only if it is informative. Such algorithms will lead to improved performance, prolonged lifetime for the sensor nodes, and improved reliability of the entire network.

Page 11: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

Fig. 7: Optimatechniquelevatiotheir stincorpoarrays developMultianreceiverdevicesbuild anonideathat allofinding,small hused.  Novel odevelopimplemhas beeprototypdemonsdevelopfinding  

Centralized

al signal pues for sens

on and polartatistical prorating the aand azimu

ped methodsntenna systers, wireless

s such as marray configalities and mow applying, to real-wo

handheld dev

optimal andped in th

mentations uen implemepe system strated in a p conformaapplication

d and decen

rocessing fsor arrays orimetric domroperties ararray calibr

uth, elevatios are applicems are be and sensor

mobile interngurations wmutual coug advanced orld arrays vices there

d robust prohis work. using real wented in coo

for trackingood numb

al arrays ofns in azimut

ntralized est

for arbitraof arbitrary mains. Optire establishration data on and polable in moscoming semr networks. net termina

with nice unpling. Conssmart antenwith arbitraare so man

ocedures foAnalytical

world arraysoperation wng other uber of internf arbitrary gth, elevation

11

timation in

ary array cgeometry aimal, robusthed. The mand wavefilarimetric dst arrays andminal part There are m

als and handniform geosequently, tnna algorithary configu

ny design co

or array prol performas in hand-hwith Nokia users carryinational wirgeometry fn and polari

a network w

configuratiare developet and high-r

methods canield modelindata procesd applicatioof future cmany desigdheld TV-rometry. Mothere is a nhms such asuration and onstraints th

cessing usinance studieeld terminaResearch c

ing RF tagreless eventfor beamforimetric dom

with M node

ions. In thied. Signals resolution ten deal witng in an elessing may ns of practi

communicatgn constraineceivers, an

oreover, arrneed for arrs optimal bearray nonid

hat no regul

ng arbitraryes are coals. The procenter. Thergs or mobts. Similar prming and

mains. 

es.

is work sigare processechniques ath array noegant mannbe handle

ical interesttion terminants, especialnd it is rareray elemenray processeamformingdealities. Flar array ge

y array conompleted wototype depere is a highbile phonesprinciples mhigh resolu

gnal processsed in azimuare derived onidealities ner. Conformed. Hence, . als, navigatlly in handhely possiblets suffer fring techniqg and director exampleeometry can

nfigurations with pract

picted in Figh performa

s. It has bmay be usedution direct

sing uth, and by

mal the

tion held e to rom ques tion

e, in n be

are tical g. 8 ance been d to tion

Page 12: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

Fig. 8: arbitrartrivial mmethodapplica MIMOresearchthat proas in trcommutechniquaccurateradars, differeninterferand adaAdditioradar an

 

Fig. 9: createdantenna

Optimal ary array comanipulatio

d: implemenation in dire

O radar anh is MIMO ovide signifiraditional p

unications, ues for targe time syncdifferent wa

nt probing ence cancelaptive and

onal radar rnd detection

Multistaticd using signa. 

and computonfigurationon of input-ntation of 2ection findin

d novel raradars and

ficant perforphased arraspatial div

get detectionchronizatioaveforms msignals in

llation, for eoptimal waelated topicn of vital sig

c, MIMO ranal processi

tationally efns by using -output mat2-D antennang and rang

adar concepwaveform d

rmance gainay systems ersity (indun, high reson for distri

may be launceach anten

example. Naveform decs include mgns using ra

adar configing for desi

12

efficient arrFourier tra

trix model fa array of

ging (Right).

pts. Anothediversity. M

ns over classor they m

uced by raolution locaibuted MIMched from enna provid

Novel methoesign are demulticarrieradar. 

guration usiigning and

ray processiansform of for the arraf arbitrary g.  

er interestinMIMO radarsical radar s

may be wideadar cross alization andMO radar aeach antenndes many bods for paraeveloped anr techniques

ng waveforoptimizing

ing techniqthe array c

ay data. Prageometry in

ng line of rrs are multissystems. Anely distribusection) m

d tracking, are developa, see Fig. 9

benefits in meter estimnd their pes for radar

 

rm diversitythe wavefo

ques may becalibration actical appn a mobile

research fostatic radar ntennas mayuted. Similamay be exp

parameter ped. In co-l9. The posstarget iden

mation, resoerformances

and wireles

y. Virtual apforms launc

e generalizedata and nlication of

e terminal a

ollowed in configurati

y be co-locaarly to MIMploited. Noestimation located MIMibility of usntification urce allocat

s are analyzss ranging

perture mayhed from e

 

e to non-our and

this ions ated MO ovel and MO sing and tion zed. and

y be each

Page 13: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

High-impropertifor obliHIS haradiatiocoupledshows t

Fig. 10: HuygenunidireccomposorientatemployThe anconceptshows tpolariza

Fig. 11polariza Electrosize cylspace msimulatclearly are com

mpedance ies of a muique incidenas been deson pattern, ad to the antethe geometr

: Photo and

ns source actionally ansed of both tion and fee

ying chiral pntennas havt for obtainthe designeation close t

1: Conceptuation.

omagnetic clindrical trameasuremenions. The robserved fr

mpared resul

surface baushroom-typnce and findsigned to uand the secenna with ary and S-par

d S-parame

antennas. Hnd in the id

electric andeding of theparticles (fo

ve been stuning electried and testeto linear in

ual structu

cloaking baansmission-lnts (see Figeduction ofrom the bistlting in goo

ased multi-pe high-impd two orthoutilize bothcond one a

proper courameters of

eters of the d

Huygens sodeal case had magnetic ese dipoles.or circular pudied analytically smalled antenna fthe whole u

ure (left) an

ased on waline cloak o. 12). The cf the total static free spd agreemen

13

-functional mpedance su

ogonal resonh of these m

broadside upling elemf the antenna

designed an

ource antenave perfect

dipoles an. We have dpolarization

ytically, numl antennas for linear pupper half sp

nd realizat

aveguiding operating incloak is de

scattering wpace measurnt with each

antenna. urface (HIS)nant modesmodes. Thepattern. Fuent in ordera.

nd tested an

nnas are elepolarizationd the polaridesigned prn) and omemerically, awith very

polarization.pace.

tion (right)

structuresn the X-bansigned and

width of a mrements. Thh other.

In this proj) using refls. An antenne first mod

urthermore, r to obtain a

tenna.

ectrically smn purity. Thization of raractical realga-particlesand experimuseful radi

. Measured

of a Huy

. The cloakd has been optimized

metal objecthe numerica

oject we haflection-phasna based onde provides

the seconda wide band

mall antennhe propose

radiation is lizations of s (for linearmentally, ciation propdirectivity

ygens anten

king efficienverified wiwith nume

t, enabled bal and exper

ave studied se calculatin a finite-sis a dipole-ld mode candwidth. Fig.

nas that radd antennas defined by

f such antenr polarizatioonfirming erties. Fig. pattern sho

nna for lin

ncy of a finith bistatic frical full-w

by the cloakrimental res

the ions ized like

n be . 10

diate are the

nnas on). this 11

ows

near

nite-free

wave k, is ults

Page 14: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

Fig. 12DLR (G Metal-ptransmioperate cloak sstructurhave bebeen vefrequensimulat

Fig. 13formed 3.2 This rethe radiincludinknowlenetworkspectrumincumbtime, frthe plac

: First comGermany).

plate cloakission-line c

as a dipoletructure its

re retains itseen proposeerified usingncy can be tued and mea

: Photo of by this cloa

Cognitive

search concio is capablng frequencdge of its ok. Cognitivem. Seconda

bent users orequency baces. Hence,

mplete free-s

k as an antecloak capabe antenna. Telf acts as s cloaking ped: a dipole g simulationuned by cha

asured reflec

a metal-plaak structure

e Radio

centrates onle of learnincy, waveformown capabile radio takeary users n

of the frequand and loc one could

space chara

enna at a lble of, for The basic tra

an antennaproperties dantenna an

ns and measanging its gction coeffic

ate cloak ane when fed b

n enabling tng from thems and powlities, statuses an opporneed to enency band. ation. The putilize the

14

acterization

lower frequexample, hansmission-a at a frequdespite of thnd a monoposurements. W

geometry. Ficient.

nd the refleby a coaxial

technologiee radio enviwer. The rads of the spertunistic vie

nsure that nFree spect

primary usespectrum m

n of transmi

uency. Withhiding a larg-line cloak guency well hese modificole antennaWe have alig. 13 show

ection coeffl cable from

es for cogniironment andio has situ

ectrum in thew in agile no harmful trum is a reer may not much more

ission-line c

hin this projge metal sugeometry cabelow the

cations. Tw. The operaso shown hs the cloak/

ficient of anm the bottom

itive radiosnd adjust itsation aware

he neighborhusage of uninterferenc

esource thatneed the spefficiently

cloaks, colla

oject we havupport strucan be modifcloaking f

wo types of cation of theshow the ante/antenna geo

n effective dm.

s. Cognitions transmissieness in a sehood and mnderutilizedce is causet varies deppectrum all

by finding

aboration w

ve found thcture, can afied so that frequency. Tcloak-antense antennas enna resonaometry and

dipole anten

n indicates tion parameense that it

maybe even d parts of raed to primapending on the time in

g idle spectr

with

at a also the

The nnas

has ance

the

nna

that ters has the

adio ary, the

n all rum

Page 15: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

and expusers, sfor cogcompro

Fig. 14: 

Spectrufocuseddistribuand fadperformaddresscooperamultiplefor themspectrumsee Figexploit restless learningoptimizas well coopera

ploiting it fsee Fig. 14. gnitive radomising thei

: Flexible u

um explorad on optimiuted mannerding effects

mance whilesed in this ating seconde potentiallm. Optimizm such that. 15. As a reidentified imultiarm b

g and stochzed jointly.

as flexible ation with P

for data tranIt is also imios so thair performan

use of time-f

ation and izing identir. Distributes. Moreovee using simwork are ddary, optimy scattered

zation is bat sensing is esult, the syidle spectrubandit probhastic optimIn addition,spectrum u

Princeton Un

nsmission wmportant to at battery once. 

frequency-lo

exploitatioification aned detectorsr, user coo

mple individdealing with

mal sensing subbands a

ased on tradfocused on

ystem learnsum. Joint olem. These

mization. P, we have d

usage in devniversity an

15

while contr develop pooperated de

ocation vary

n. Researchnd exploitats provide dioperation fadual detecth decentralipolicies for

as well as oding off be

n subbands ws the dynamoptimizatiolearning m

olicies for developed mvice to devicnd Nokia Re

 

Fig.and sensprovperfachi

rolling the lower efficieevices can

ying underu

h in spectrution of unuiversity gaiacilitates fator structureized detectir distributedoptimizing cetween the where high

mic behavion and acce

methods stemexploring

methods for ce communesearch Cen

15: Tradinexploitati

sing policy vide idle spformance cieved. 

level of intent and high

operate f

utilized spec

um exploraused spectrun since they

ast multibanes. The conion of primd detection cooperativeexplorationquality sper of the spessing of idl

m from statand accessmodeling a

nications. Thnter. 

ng off betwion. Develallocates s

pectrum perclose to i

terference ch fidelity imfor a long

 ctrum. 

ation and exum in a coy can mitignd sensing ncrete rese

mary users by multipl

e spectrum n and explectrum is idectrum and dle bands ististical infersing the speand managinhis work ha

ween spectruloped gresensing to rsistently aideal sensi

caused to otmplementati

time with

xploitation ooperative gate shadow

and improarch probleby a group

le sensors oaccess policoitation of

dle persistencan maxima

s modeled arence, machectrum canng interfereas been don

um exploratedy spectrsubbands tnd as a reing policy

ther ions hout

has and

wing oves ems p of over cies the

ntly, ally as a hine n be ence e in

tion rum that

esult is

Page 16: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

16

Implementation issues in spectrum sensing and exploitation. The quality of the spectrum sensor decisions and decision statistics, and the decision frequency are the key parameters in optimization of the spectrum utilization and the overall performance of the cognitive radio system. The most important properties of a single detector entity are, firstly the ability to make the decisions quickly and reliably, and secondly the ability to observe a wide frequency range and multiple primary systems simultaneously. In addition, the implementation must be optimized such that the change of primary signal under detection has as small as possible effect on the receiver front-end parameters. Reconfiguring the front-end takes time and slows down the hopping between different bands and signal types. Spectrum sensing applications also set high requirements for RF hardware (wide bandwidth, wide tuning range, high dynamic range, high linearity), which is a limiting factor in current implementations. Sensing algorithm should be selected so that it enables the flexible configuration of the sensor parameters with software. In order to enable the sensing of multiple systems simultaneously, the functionality of the DSP implementation should be independent of the sampling rate and signal bandwidth of the system to be detected. While targeting a battery operated application it is of utmost importance to minimize the power consumption of the sensor both at circuit and architectural level. Therefore, in the implementation of a simultaneous multisystem spectrum sensor, one should lead up to a solution in which the amount of hardware does not increase linearly with the number of systems under detection (or even with number of transmit/modulation parameters in a single system). In addition to spectrum sensing functionalities, DSP may have to implement support functions such as additional filtering and gain control. As the functional requirements on the DSP domain increase, it becomes more and more important to optimize the energy and cost efficiency of the realized circuits. While performing spectrum sensing, it might also be beneficial to obtain additional information for example about the adjacent channels and their power levels. For example in some cases, presence of a strong signal on the channel adjacent to the one under detection could affect the reliability of the detection results. In addition, this knowledge could be to adjust RF functions in the receiver. In hardware side the development of cognitive radio has focused on developing energy efficient RFICs and demonstrating sensing algorithms in various different environments. The demonstrations have focused on defining the limitations of the RF hardware to the detection and detector performance. The over-the-air measurements and the measurements in the controlled environment show that the different nonlinearities in the RF hardware can easily decrease the reliability of the spectrum sensor. In some extent the developed feature detectors can impove the detection reliability when compared to energy detectors. However, still advances in impoving the linearity at RF and analog parts must be made to increase the reliability of the spectrum measurements. In the detector side a comprehensive study on diffetent algorithms has been done in addition with algorithm development to find optimal algorithms suited for mobile environment. The focus on algorithm implementation has been on finding implementations that lead to small implementation size together with low power consumption. In RFICs the focus has been on finding solutions that improve the aforementioned RF linearity and also support wide variety of different frequency bands. Fig. 16 illustrates demonstarion board that enables over the air measurements. White spaces. Secondary usage of TV white-spaces is an emerging application of cognitive radio techniques, where unutilized or underutilized spectrum reserved for digital terrestrial television is allocated to wireless communications. Spectrum sensing can be used to determine the level of TV signals in a specific location, but sensing alone is not able to provide information on the frequency planning of the network, i.e., it is not possible to know whether a particular TV frequency is planned for use in the measured location. Thus, sensing must be complemented with a geo-location database. We develop techniques to improve the secondary usage of TV white spaces by combining the information from geo-location database and radio propagation modeling with measurements from white-space devices.

Page 17: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

Fig.16: Integra2010. Tmeasurebasebanbands: 160MH

Fig. 17:

Detector fo

ated multibThe seconded during 2nd circuits L-band, C

Hz and 50MH

: Implemet

or spectrum

band receivd version o2011. The and analog

C-band and Hz. The AD

ted SAR rec

sensing

ver for SARof integratecomplete in

g-to-digital X-band, a

DC has 4 dif

eiver.

17

R applicated receiverntegrated S(ADC) con

and the bafferent mod

tions. The fr for SAR SAR receivenverter. Tseband has

des, from 8 b

first prototyapplication

er, Fig. 17,he RF-fron

s two diffebits mode to

ype chip wan was imp, includes Rnt-end has erent cut-ofo 5 bits mod

as measuredplemented RF- front ethree differff frequencde.

d in and end, rent

cies:

Page 18: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

Intensivbasebantuning. EuropeaMeasurby ESAtempera-25° C, the projuse the The cirFourth Applica ProcedIf the fdegradastudy. IexperimmorphicFour dmanufagrips, slocationhand. Dcouplinusing athat the

Fig. 18: 3.3 Millimeamplifieoutput p

10

40

11

40

10

15

ve measuremnd and ADCThe circuitan Solid Starement of thA. For L-bature, 0° C 45° C and

ject has beedesigned in

rcuit designInternation

ations (AMI

dures againforeseeable ation of theInteraction bmental studcally shaped

different capactured. Thesee Fig. 18n can affectDifferences ng element ba multi-elem probability

: Effect of th

Millimetr

etre wave ier was desipower at 90

CCE1

6

CCE3

xz

y

ments haveC) were mets design anate and Cirche whole reband receive

and 45° C)70° C) was

en deliveredntegrated ren and the mnal WorkshICSA)” whi

nst impedanuser effect

e performanbetween a m

dy using cad hand phanpacitive co

e difference8. It was ct significant

of severalbased antenment antenny of interact

he user’s ha

re Wave a

integrated igned and s

0 GHz with

15

40

40

15

410

e been perfoeasured sepand measuremcuit Confereeceiver was er, the chip). Measurems performedd on 22nd Seceiver in a f

measurementhop on Anich will be h

nce detunints are taken

nce in real umobile termapacitive cntoms. oupling elees of the peronfirmed wtly the perfo dB in tota

nnas with tyna structure tion with the

ands on the

and THz

circuits. Asuccessfullya standard

CCE2

610

106

4

CCE4

18

formed on tarately to vment resultsence (ESSCdone in ac

p has beenment in 5 dd for the receptember 20future projet results fornalog and held on 26 -

ng of mobiln into accouse cases c

minal antenncoupling el

ement antenrformances

with measuormance of al efficienc

ypical hand e with antene index fing

operation o

Techniqu

An extendedy measured1.2 V suppl

4

6

6

4

the second verify their fs of the base

CIRC) in Hecordance w

n measureddifferent temceiver in C-b011 at ESA-ect by a Gerr the wholeMixed Sig- 28 August

le terminalount alreadycan be avoidna and a hanlement ante

nnas, showof the ante

rements thathe antenna

cy were obgrips. Part

nna switchiger is minim

of mobile te

ues

d version of d. The amply and occu

chip. All tfunctionalityeband and A

elsinki on Sewith the comd in 3 diffemperatures band mode.ESTEC, wh

rman compae receiver wgnal Integrat 2012 at ES

l antennas y in the anded, which nd of a userennas and

wn in Fig. ennas were at antenna a in a mobilserved betwof the handng. Shaping

mized is wor

erminal ante

f the power lifier achiev

upies an acti

the individuty and to seADC has beeptember 20

mpliance speerent tempe(room temp. The final phere also thany was diswill be presated CircuSA-ESTEC

in the vicinntenna desig was demor was invest

homogene

18, were studied witelement sh

le handset hween differd effect can g the antenrthwhile as

ennas.

combining ves +14.5 ive area of

ual blocks (etup the correen reported011. ecificationseratures (roperature, 0°presentation

he possibilitycussed. sented in “Tits For Sp.

nity of a usgn, part of nstrated in tigated with

eous anthro

designed th several hhape, size held in a usrent capacitbe avoided

nna elementwell.

CMOS powdBm satura0.17 mm2. T

(the rect d in

set oom ° C, n of y to

The pace

ser. the the

h an opo-

and hand

and er’s tive

d by t so

wer ated The

Page 19: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

amplifiethe voltprotectiA 100-simplifirealiseddoublerdB fromIn additmanufaMeasurmicrogr

Fig. 19mm2 an

Fig. 20:0.65 mm

Fig. 21area is

er is implemtage swing ion. The miGHz balancied schemad with an onr is 16 dB um 42 to 55 Gtion, 165 an

actured usinred on-waferaph of one

: Chip micnd the active

: A schemam x 0.42 mm

: Chip mi2.0 mm2 (2.

mented in 6limitations crograph ofced frequentic and a chn-chip spirausing an inpGHz. nd 183 GHzg a 100-nm

er performanof the 165-

crograph of e area is 0.1

atic and a chm.

icrograph of.0 mm x 1.0

65 nm CMOof the tran

f the power ncy doublerhip microgral balun. Atput power o

z low noise m gate length

nce shows 1-GHz low n

f the 90-GH17 mm2.

hip microgr

of the 165-G0 mm).

19

OS process nsistor. Theamplifier isr was desigraph are pr

At 100 GHz of +5 dBm.

amplifiers h metamorp19-27 dB of

noise amplif

Hz CMOS po

raph of the

GHz metam

taking into chosen ams presented gned in 65-resented in the measur

. The funda

were reporphic high elef gain and lfiers is prese

ower amplif

100-GHz C

morphic HEM

o account remplifier topo

in Fig. 19. nm CMOSFig. 20. Th

red conversamental sup

ted. The amectron mobilowest noiseented in Fig

fier. The are

CMOS frequ

MT low no

eliability isology also p

S technologyhe widebansion loss ofppression is

mplifier circility transiste figure val

g. 21.

rea, includin

uency doubl

oise amplifi

sues relatedprovides ES

y as well. Tnd balancingf the freque

better than

cuits have btor technoloues of 4 dB

ng pads is 0

er. Chip siz

er. The circ

d to SD-

The g is ncy

n 25

been ogy. B. A

0.42

ze is

cuit

Page 20: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

CharacESA-refor spacincludeexperimapplicatResults jig weredesigneadaptivThe recreceivedheating pulsed dDevelopThe mahas beethe-art developAccuratimportameasurethe thruwith ercalibrat

Fig. 22matchinGHz. Millimewith a steeringis a perphase pboundarinducinelement

cterisation,elated SMARce and othes various cl

mental resultions in the from the n

e reported. ed for subhae for newescent break-d much attrelated effe

diode measupment of S

anufactured n verified toresults we

ped new comte on-waferant at subements at su-reflect-linrrors causedtion techniq

2: a) Excepng design. b

etre wave MEMS-bas

g mechanismriodic array

properties ofry condition

ng reconfiguts of the M

, modellingRAD and Mer THz applosely relatelts in a confield.

novel characIn addition

armonic mixst diodes by-through intention. Thects in submurements ha

Schottky diodemonstrato produce ere obtainedmpact outpur scattering bmm-wave submm-wavne (TRL) ord by cross-tque based on

a) eptionally wb) On-wafer

beam steersed high imm is based oy of unit cef the unit cens. MEMS

urable surfaMEMS varac

, and appliMilliLab resplications hed mutually ncrete way,

cterisation mn to the jig xer diode te

y various man THz Schoe novel me

micron-sizedas been starode-based dtors includeexceptionalld with a vut matching

parameter frequencie

ve frequencr line-reflectalk due ton the 16-term

wide-band r vector netw

ring with ampedance suon the princ

ells with dimell structuretuneable H

ace impedanctor array.

20

ications of nsearch activhave been cy complemen, benefitting

method of Sfor fundam

esting is unanufacturersottky diodeethod takesd diodes. A rted. demonstrato

e a monolithly wide-banvery small g and filterin

measuremees (Fig. 2ies is a chact-reflect-m

o imperfect m error mod

(75-140 GHwork analyz

a MEMS-burface (HISciple of a pmensions me are analysHIS can be nce via appA simplifie

nonlinear 2ities for the

continued. Tnting activig both acad

Schottky dimental mixender develops is in targete series ans holisticallnew step, a

ors has prohic Schottkynd operation

chip-size dng structureents with a 22b). Howeallenging ta

match (LRRgrounding

del.

GHz) triplerzer measure

based high S) has beenhase gradie

much smalleed by usingused for ellying differed model o

2 terminal e characterisThis researcties that targdemic resea

iodes by usir operationpment. A flt. d thermal ly into accoan accompan

oduced excey diode basen covering 7design, an

(see Fig. 22vector netw

ever, calibask. Standar

RM) calibratof the port

b)r circuit baements of Sc

impedancen studied inent array. Mer than a wg a simplifielectronic refrent bias vof a surface

millimetre sation of Scch and devget to combarch as wel

ing a univen, also a newlexibly usab

resistance ount also i

anying study

ellent wideed frequenc75–140 GHzachievemen2a). work analyz

bration of rd methods tion often h

rts. We inve

) ased on co

Schottky-dio

e surface. n W band (

MEMS-basedwavelength. ed model wflective bea

oltage to dif with 40 im

wave devicchottky devivelopment abine theory ll as indust

ersal mixer w universalble jig to be

extraction important sy including

-band devicy tripler whz. The state-nt based o

zer (VNA) the on-wautilizing, e

have probleestigate a n

ompact outdes at 100-3

Beam steer(80 GHz). Td tuneable HThe reflect

with appropram steeringfferent rowsmpedance s

ces. ices area and trial

test l jig eing

has self-fast

ces. hich -of-n a

are afer e.g., ems new

tput 300

ring The HIS tion riate g by s of strip

Page 21: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

lines ofpattern of normis progr

Fig. 23:which is

Periodiwide radevelopengineetransmiinductorules, tcontinusuggestScatteritheoretiThe preperiodicfrequenelementtransmithe loadpositionwavelen

Fig. 24CRLH t Dielectrtransmi

f 0.35 x 0.3of a strip co

mal and oblirammed to s

: The norms programm

ic structurange of appped very wering and ission line wor we obtainthis transmuously radiated in Fig. ing parametical reflectioecision of dc leaky-wav

ncy approacts are stronission line. Fding elemenn within thngth). These

a) : a) Unit ctransmissio

ric rod wavitting an mm

35 mm2 unionsisting ofque incidensteer the bea

malized radimed for a be

es for leakplications. S

well over thscientific

with the coun coupled r

mission line ated into th

24b). A mters measuron of the an

design proceve antennasching millimngly influenFurthermorents interact

he unit cell e effects are

cell of perion line, and

veguide (DRm-wave pow

0

-60

-90

it cells is usf elements wnce. Fig. 23am to direct

ation patteream at the d

ky-wave anStarting withe time sinclife, possibunterparts oright/left-han

becomes he space amicrostrip rement showntenna sampedures prevs is proving meter wave

ncing overale, the evanewith each o(be it unit

e currently u

odically loadc) comparis

RW) componwer. DRW

-100

-30

21

sed for demwith differenshows the stion of 0° w

rn at 80 GHdirection of

ntennas (LWh filters, thce 1940’s. bilities notof its constianded transm

leaky, i.e. above the sbased leakwn in Fig.

ple which isviously suggg to have stres and higll performanescent fieldsother and tht cell smallunder resea

b) ded transmson of simu

nents. Dielehas an adv

-20

0

monstratingnt impedansimulated ra

while the ang

Hz with incidf 0°.

WA). The phe theory ofWith onsett considereitutive partsmission line

the wave structure (e

ky-wave ant24c displa

s out of balagested by varongly deterher. The pnce of the s excited at heir performler or large

arch and to b

ission line, lation and m

ectric rod wvantage ove

30Equal Im

Full tuni

Limited

the beam sce is analyzadiation patgle of illum

dent angle f

periodic struf the periodt of metamed before s, i.e. by sere (see Fig. propagatin

e.g. for platenna was ys the com

ance. arious textbriorating ac

parasitic comcomposite rthe discont

mance stroner than the be described

b) continuomeasuremen

waveguide ier conventio

60

9

mpedance

ing range

tuning range

steering abized numericttern for the

mination is 4

from 45° for

uctures candic transmis

materials intoemerged. Bries capacit24a). With

ng along thanar transm

designed amparison of

books on mccuracy withmponents oright/left hatinuities arengly depend

one tenth d in the futu

c) ously radiatnt for unbal

is a promisonal metal

90

ility. Radiatcally for beae surface wh45°.

r the surfac

n be utilizedssion lines wo the practBy loadingtor and para

proper deshe structure

mission lineand measurmeasured

etamaterialsh the operatof the loadanded (CRL

e so strong, tds also on th

of the guiure.

ting microslanced LWA

sing device waveguides

tion ams hich

e

d in was tical g a allel sign e is e as red. and

s or tion ding LH) that heir ded

trip A.

for s of

Page 22: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

lower dadvantaintegratRecentlantennarectangua desigmeasureUsing aphased electricloaded w

Fig. 25sensor structur Integrabeam-stlens antpolarizashapingthe mearay-tracmeasurereductio

Fig. 26b) meas Millimemillimeand it

dielectric losage is the pting variously the DRWa is its comular metal w

gn of a boles the amouan array of D

antenna arally small with a ferro

5: a) Schemstructure i

re integrate

ated lens anteering withtennas was ation and mg was develoasurement rcing simulaements at 7on of intern

6: a) A phosured norma

etre wave eter-wave imis fabricate

sses comparpossibility os componen

W antenna fompact size waveguideslometer powunt of poweDRW antenrray. A phadipoles wh

oelectric var

a) matical viewintegrated ied with the D

ntennas foh high direcstudied. Th

mutual couoped and teresults are sation progra77 GHz. Th

nal reflection

a) otograph of alized radia

reflectarramaging apped on a sil

red to metaof using stants into it. or 220 – 325compared t. The schemwer sensor r travelling

nnas with intase shifter ihich are perractor to con

w of the DRinto a DRWDRW antenn

r beam stectivity. Redhe reflectionupling. A v

sted with anshown in Fiam. The behe new shapns was dem

f the designeation pattern

ay. A 120-Gplications isicon wafer

22

al losses, espandard micr

5 GHz was to other di

matic imageintegrated in the DRW

ntegrated phintegrated iriodically pntrol the ph

RW antennW, and c) na.

eering. An duction of inns are know

very effectivntenna meaig. 26. The eam-steeringaped lens w

monstrated w

ed extendedns at 77 GH

GHz reflecs being devr. The 3700

pecially at frofabricatio

fabricated irective ante of the ante

into a DRW. ase shiftersinto DRW printed on thase of the p

b) a, b) schemschematica

integrated nternal reflewn to cause ve reflectiosurements. lens was de

g propertieswas comparewith simulati

d hemispherHz.

ctarray for mveloped. Th0 elements

frequencies n and semi

and tested. ennas and

enna is showRW is prese

, it is possibis shown inthe DRW s

propagating

matical viewl view of t

lens antennections in lohigh side l

on reductionThe designeesigned usins were tested to a clasions and me

b)rical lens w

mm-wave ihe reflectarr

of the ref

above 100 iconductor

The advanta good ma

wn in Fig. 2ented. The

ble to createn Fig. 25c.side wall. Ewave.

w of the bothe phase s

na provides ow permittilobes and in

on method ned lens andng an in-hoted with radssical lens deasurements

) with shaped

identificatioray has 138flectarray c

GHz. Anottechniques

tage of suchatching wit

25a. In Fig. 2power sen

e a controlla. It consistsEach dipole

c) lometer powshifting dip

the means ivity integrancreased crobased on l

d an exampleouse develodiation pattdesign and s.

extension, a

on (MMID)8-mm diameompensate

ther for

h an th a 25b nsor

able s of e is

wer pole

for ated oss-lens e of ped tern the

and

) or eter the

Page 23: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

sphericafew mecoplanaintroducMEMS capaciti90°, short-ci

Fig. 27MEMS-3-m dis

Three dfocusinthe reflresultinnear-fiecompar

Fig. 28aside atreflecta Materianalyseimportaand lossample the recttransmi

al phase froeters from ar waveguidces the requ

phase shifive shunt sw180°, and ircuited CPW

: a) Reflec-actuated phtance.

different tyg to 0.5 m aectarrays ar

ng phase shield measurerison to simu

8: a) Measut 3 m, and b

array with a

al measurer. The extant topic of s tangent inid placed i

tangular waission S-par

ont from thethe reflect

de (CBCPWuired compfters. In thewitches loc270°. BefW stub as th

tarray geomhase shifter

ypes of stataside from re fed with ift pattern inement rangulation as w

a)

ured (solid)b) phase of

an open-end

rement in traction of f investigation the frequeinside a shoaveguide corameters are

e feed in suctarray. The

W) structure.pensation. Te MEMS, tcated so thafore the acthe phase sh

a) metry. The rrs. b) Phase

tic reflectarboresight atan offset on case of ree at 120 G

well as the n

) and simulaf the S11-parded wavegui

the frequematerial paon. A fast, ency range ort section onnected to e measured

23

ch a way, threflectarra

. There, a paThe reflectathe phase sat the normtive, static r

hifter.

reflectarraye-shift patte

rrays are faat 3 m, and 3of 27° at deflectarray 2GHz. Figurenear-field ph

lated (dasherameter meaide.

ency rangarameters aaccurate anof 75 to 32

of an enclostwo ports o

d in the freq

hat the fielday elementsatch antenn

array is beinshift arises

malized reflereflectarray

y is offset feern for a ref

abricated: 13) focusing

distance of 02. The statie 28 showhase of the r

ed) beam paasured at 1

e of 75−3at millimetrnd easy to u25 GHz hassed transmiof a vector nquency ban

d is refocuses are baseda is coupledng develope

from shortection phaseys are fabric

b) ed and it canflectarray fo

1) focusing to 3-km di

0.3 m (Fig. ic reflectarrs the measreflectarray

attern for r-mm distan

25 GHz ue waveleng

use method s been deveission line. network ana

nd of 75 to

ed at a desird on a cond to a phaseed for activting a cople in differecated with

n be activelfocusing to

g to boresigstance at bo27a). Fig.

rays are chasured beamy.

b)

reflectarray nce from the

using a vegths is an i

to determineloped wheThe line walyzer. The325 GHz t

red locationnductor-bace shifter, whve control wlanar line wnt states is open-ended

ly focused w0.5-m offse

ght at 3 m,oresight. Al27b shows

aracterized im patterns w

focused 0.5e surface of

ector netwointeresting ne permittivre the mate

was a sectione reflection to estimate

n, at ked

hich with with

0°, d or

with et at

, 2) ll of the

in a with

5 m f the

ork and vity erial n of and the

Page 24: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

permitticommersimulatsample For Tedifferencoefficiphase rmethodpermitti

Fig. 29simulat ExtractIn conneffectivmethodmateriabased odoes nosamplestechniqueffect o 60 GHztechniqudesigneuse of mefficienfrequenMEMS transmiwith difmanufaradiatiomeasurethe -10

ivity and lorcial full-wed results. Aof unknown

eflon and unt values oients using results obta

d, the best ivity of the

: a) Measurted transmis

tion of elecnection to thve material ds suffer froal. In this pron the classot involve ans thicker thue. The pro

of thermal n

z membranues to over

ed and manumicromachi

ncy and gooncies. The sa

switches. ission lines fferent phas

actured anteon pattern ement systedB matchi

oss tangent wave simulaAs a referenn polymer. unknown pof the dieleleast squareained from fit is obtaiunknown p

a) red and simssion coeffic

ctromagnethe previous parametersom an intrroject we hasical Nicolsny branch s

han λ/2, a moposed derioise on the

ne antennarcome the ufactured foining to remod radiationame manufa

However, were used

se shift valuennas were m

measuremem located iing criterion

of the matator (HFSS)nce case thi

olymer, thectric conste error fittin

the measuned for pe

polymer is o

mulated trancient phase f

tic materiasubject, wefrom meas

rinsic limitaave proposeson-Ross-Wseeking and measure thaivative of thextracted m

a array for high path

or the 60 GHmove the sun properties

facturing proin this w

to demonstues and singmeasured u

ments were in the Orangn and the m

24

terial under) and compis has been d

e simulatedtant and lo

ng method. urement anermittivity oobtained to b

nsmission cofor unknow

al paramete have also tsured reflecation relateed a novel w

Weir (NRWis therefore

at would oththe NRW ematerial para

r beam steeloss at 60 Hz frequen

ubstrate mats comparedocess couldwork passivtrate beam gle antenna using a prop

performedge labs, la T

maximum m

r test. Similarison is thdone first fo

d reflectionoss tangentFig. 29 sho

nd simulatioof 2.0 and be 2.4 and l

oefficient phwn polymer.

ters from rtheoreticallyction and tred to the eway to over

W) techniquee capable ofherwise cauxtraction teameters.

ering applicGHz. A tw

ncy band usiterial underd to a bulkd be used to ve phase steering. Thelements (F

pe station and with th

Turbie, Franmeasured re

ar situationhen made beor Teflon (P

n and transt are compows the tranon. Using lloss tangenoss tangent

b)hase for Tef

reflection-try studied alransmissionelectrical thcome this li

e, the propof extracting use problemechnique ha

cations. Bewo elementing micromr the antennk silicon pro

manufacturshifters usihe prototypFig. 30). Thnd a vector he 3D on-nce. The maalized gain

n is also simetween the PTFE), and

smission cpared with nsmission coleast squarnt 0.003 fot 0.06.

) eflon and b)

ransmissiolgorithms fon coefficienhickness of imitation. Aosed extrac

g material pams in the Nas been use

eam steeringt antenna a

machining tena elementsocess at m

ure phase shing differe

pes include he input imp

network an-wafer radanufactured n is 6.0 dBi

mulated witmeasured after that fo

oefficients the measu

oefficient (Sre error fittor Teflon. T

measured a

n coefficienor extractionts. The knothe measu

Although bection techniarameters frRW extract

ed to study

g is one of array has bechnology. Ts provides hillimeter w

hifters basedent lengths antenna arr

pedances of nalyzer and diation patt

antennas fu. The anten

th a and

for a

for ured S21) ting The

and

nts. n of own ured eing que rom tion the

f the been The high

wave d on

of rays f the

the tern ulfil nnas

Page 25: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

25

were designed in co-operation with University of Nice-Sophia-Antipolis, France and the prototypes were manufactured in LAAS-CNRS, University of Toulouse, France.

Fig.30: A photo of the manufactured antenna prototype. 3.4 Sensors Microwave visualization of objects buried in non-transparent media. Subsurface radar sensing is aimed at detection, localization and identification of versatile objects in non-metallic media. Among those tasks, detection of pipes, voids, mines in soil, rebars and cracks in civil engineering structures, tumours in biological tissues are worth noting. A new signal processing approach based on expanding the subsurface radar data into separate B-scans for amplitude and phase and their subsequent assembly in the common image using transformations of signal amplitude → intensity of the pixel and signal phase → color of the pixel has been proposed. The idea of the method is based on the fact that amplitude of the wideband signal reflected from the buried object indicates presence of the object at some depth while the phase shift at the act of reflection depends on the contrast of dielectric properties between the object and surrounding medium and therefore can characterize it. Thus, the image where intensity of the pixel is related to amplitude of reflected signal and color to its phase can be used for both detection of the objects and their discrimination. Some results of microwave visualization of objects buried in sandbox using frequency-swept signals in the range of 1.3 to 6.5 GHz and UWB tapered-slot antennas are shown in Fig. 31. As seen in Fig. 31, both detection and differentiation of buried objects is possible with the use of the proposed method.

Fig. 31: a) Void in the sandbox, b) anti-personnel plast mine (PMN) simulant in the sandbox. Ground surface is seen at zero depth, bottom of the box at the depth of 40 cm, objects have been buried at 10 cm.

 

1 mm

ground surface ground surface

void mine simulant

bottom of the box bottom of the box

Page 26: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

Design particlecan funHowevefully rethat thenecessalens syspossibleconjuga

Fig. 32balance MEMSThe blohybrid readoutelectroselementoutput oexpectegeneratThe senchip is supply measurenon-linethe EurmeasureJournal

of an idees. In our eanction as aer, the knowalize the req

e ideal phasary propertiestem. The pe experimeating particl

2: The coned modulato

S acceleromock diagramtopology wt is implemstatic dampt. The ratioof the ADCed to have nor, DSP and

nsor chip hashown in Fis 1 mA. Thement resulearity of 0.1ropean Soliement resulof Solid St

eal phase-carlier work

a perfect lewn experimquired idealse conjugates of nonlinphysical priental realizales consistin

nceptual desor; LPF= lo

meter. The m of the senwhich combmented withping is usedometric outpC is inverselno supply dd analog buas been impFig. 34. Thehe sensor inlts and it a18 % at thed State Cirlts together tate Circuits

onjugatingwe have th

ens, focusinmental approl phase conjting surfacenear and noinciple of thations are ng of two an

sign of paow-pass filte

acceleromensor is showines the oph a charge d to damp put is convely proportiodependency,uffer. plemented ine chip area interface is achieves SN input rangecuits Confewith deep t

s July 2012

26

g surface aheoretically ng propagaoaches basejugation boe is in princonreciprocahe lens opeoutlined. F

ntennas con

rticles former.

eter has beenwn in Fig. 3pen-loop rea

balancing the high querted to the

onal to the s, in theory.

n a 0.35 µmis 6.66 mm2

able to dampNR of 91 dB

e of ±1.15 gerence (ESStheoretical bissue.

as an arrashown that

ating wavesed on thin undary conciple physil particles weration wasFig. 32 illunnected via a

ming an id

n designed 33. The senadout and e

topology wuality facto

e digital domsupply volta

The chip h

m CMOS pr2 and the nop the high QB at 200 Hg. The resulSCIRC) 20background

y of nonlint a pair of ps and enhansheets of ndition. In thcally realizwhich can b

analysed inustrates cona non-linear

deal phase-c

during the tnsor interfaelectrostatic which has or Q of themain by a Dage, the digihas on board

rocess. The ominal currQ of the senz BW. Thelt of the sen12. The papof the chip

near and phase conjugancing evannonlinear mhis project wzable and inbe used to bin detail andnceptual der circuit.

conjugating

time periodace is imple damping. ratiometric

e micromecDelta-sigmaital output od voltage re

e micrographrent consumnsor elemene sensor shonsor has beeper present

p has been a

nonreciprogating surfanescent wav

materials canwe have shonvestigated build a perfd directions

esign of ph

g array. BM

d of 2010-20emented witThe open-lo

c output. Tchanical sena ADC. As of the sensoegulator, cl

h of the senmption at 3.6nt confirmedows maximen presenteding the furtccepted for

ocal aces ves. nnot own the

fect s of hase

M=

011. th a oop The nsor the

or is ock

nsor 6 V

d by mum d in ther the

Page 27: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

Fig. 33: Fig. 34: MEMSMEMS group wEnded TseparatelimitingresonatoOne of drive sithis comThis sotweakinamplituadditionconsum

Fig. 35:

: Block dia

: Microgra

S frequencyfrequency

within OMFTuning Fore oscillatorsg circuitry. or element othe implemignal is meamparison, thlution is ve

ng the referude has to bnal amplific

mption).

: Simplified

agram of the

aph of the ac

y referencereference a

FRI project rk) voltage s implemenIt is critic

operating inmented oscill

asured and he loop gairsatile in a rence volta

be relativelycation stage

d block diag

e accelerom

cceleromete

e. The desigalso continuwere focuscontrolled

nted on the al to keep n the linear lator loops ucompared tn is regulatsense that t

age of the y high to enes which in

gram of the

27

meter chip.

er chip.

gn of the inued in 201sed on deveresonators.interface Athe drive sregime. uses continuto an externted with thethe controllePI controllnsure accurncrease ove

implemente

nterface for1. The reseeloping an i

Two approASIC. Each

signal amp

uous level cnally referee help of a ed amplitudler. A poterate operatioerall resourc

ed voltage c

r the tempeearch activitintegrated inoaches inveof them fealitude well

control, Figence value.

PI (proportde can be mential drawbon of the coce utilizatio

controlled r

erature comties in the nterface to estigated, reatures a uni

controlled

g. 35. The amBased on ttional-integ

modified durback is thaontrol loopon (chip ar

resonators.

mpensation oCircuit DesSETF (Sing

esulting in tique amplit

d to ensure

mplitude of the outcomegral) controlring runtimeat the detec. This requea and curr

of a sign gle-two tude

the

f the e of ller. e by cted

uires rent

Page 28: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

Anotherhas alsoamplitupart of turn conThis apmay no

Fig. 36: Both tovoltage be chalshown MEMS+straight

Fig.37:

r approach,o been inv

ude instead the signal pntrols the g

pproach allot be as accu

: Implemen

opologies hCMOS pro

lenging, whin Fig. 37. + softwaretforward inc

SEM pictu

requiring lestigated. Tof continuoperiod when

gain of loopows to implurate as the

nted interfac

have been iocess. The mhile the bigOne step t

e, which alclusion of th

ure of imple

ess componThe structurously contron amplitude

p amplifier tlement ampcontinuous

ce ASIC for

implementemeasuremenggest obstactaken to imllows modehe models in

emented ME

28

nents and abre is a syn

olling its vae is higher thus realizi

plitude limitcontrol solu

r MEMS osc

ed in an intnts on the Mcle was the

mprove the merately precnto circuit s

EMS fork res

ble to operanchronous halue. It uses

than a desing a hard-ltation with ution.

cillators.

terface ASIMEMS osci

lack of promodelling wcise modelsimulation t

sonator.

te with lowhard-limiter

a comparatired value. Timiter for tlower amo

IC (Fig. 36llator protooper model was to initialing of theools.

wer drive sigr which simtor which tuThe compathe resonatoount of reso

6) in AMS otype, howe

for the MEalize the use MEMS s

gnal amplitumply limits urns on for

arator outpuor drive signources howe

0.35mm hver, showedEMS resonase of Covenstructures,

udes the the

ut in nal. ever

high d to ator ntor and

Page 29: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

3.5 Univermanageregulatobandgapbe usedthe novharvesteultra-lowstart-upenergy harvestehas bee

Fig. 38:

Fig. 39:regulato Electrothis fieltransitiolayer wthe con

Materials

sal power ement systeor, shown inp voltage re

d for verifyivel voltageer types, inw power de

p, voltage bstorage. Coers and supn submitted

: The block

: The blockor and the b

omagnetic cld was doneon layer wh

was postulatencept of ex

s and Ene

managemem was comn Fig. 38, ueference using the func reference.

ncluding phoevices, e.g. boost and vollaborationpercapacitord for manuf

k diagram of

k diagram obandgap vo

characterize in 2011. Fhich left uned equal to xcess surfa

ergy

ent systemmpleted. Tused for acced for provctionality ch

As shownotovoltaic, tsensors, fle

voltage reguwith Tamp

rs, both realfacturing.

of the charge

of the systemltage refere

zation of pFirst, the prenexplained t

the lattice ace current

29

m for energThe present curately reg

viding accurharacterizinn in Fig. 3thermal, RF

exible displaulation. Thepere Univerlized in flex

ge pump reg

m to be desience.

planar and eviously intthe thickneperiod) wawhich co

gy harvestsystem co

gulating therate referencng the perfo39, the sysF radiation,ays, or comme system usrsity of Techxible printed

gulator.

igned. The f

bulk metatroduced coess of this ls replaced bmpressed t

ters. The fiomprises ofe output volce to be useormance of stem will in

kinetic andmunication ses supercahnology is dd electronic

first design

amaterials. oncept of a slayer (the thby a more athe transitio

first design f a charge ltage of theed in the rethe voltagenterface did fuel cell hdevices pro

apacitors fodone for obcs technolog

includes th

A strong cso-called Dhickness ofadvanced coon layer to

of the powpump volt system, an

egulator. It we regulator ifferent eneharvester, woviding syst

or filtering btaining enegy. The des

e charge pu

contributionDrude-Simovf the transitoncept. Thio an effect

wer tage nd a will and

ergy with tem and

ergy sign

ump

n in vski tion is is tive

Page 30: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

metasur(monolaeither ngrids wThis minducedsolar cePrevioufinite theffectiv Isotropstudied index inand peramorphinclusiothe latticenteredthe wed

Fig. 40distribustructurnegativ MetaminternatPlasmondue to tis 43%)antirefleARC gabsorbinCuInxGcoverin

rface. Secoayers of res

non-resonanwithout any model allowed bianisotroells: it giveus explanatihickness. T

ve layer.

pic negativa historica

n the inter-brmeability ahous Si andons: individice dispersid ones and

dges (see Fi

a) : a) – A new

ution of the re comprisie refraction

material fortional patenn enhancemthe introduc) is given aecting coati

gives nearlyng layer is

Ga1-xSe2 (CIngs do not

Silicon

Silver Ag

ond, the cosonant part

nt grids andsubstrate. Ted us to thpy. This res

es the only ions of the This resulte

ve refractioally 1st desiband regionare negatived silver cordual, collection for the finally simug. 40).

w constituenelectric fie

ing a simpln of the beam

r plasmon-nt applicatioment of thinction of the as a comping (ARC).

y the same s much smaIGS), or Ghelp, too.

oncept of thicles) has b

d resulted inThe developheoretically sult fits dataknown selfPlasmon en

ed in an un

on index frign solutionn (between te there. It ire. We haveive in a placases of al

ulated the n

nt of the negeld vector ale cubic latm. The abso

-enhanced on of a newn-film solarplasmonic

parison withCalculationeffect. The

aller than tGaAs). The

We unders

30

he electrombeen develon first-orderped theory c

reveal an a known frof-consistentnhancemennphysical d

from plasmn of a metathe visible is the lattice done a d

anar array, all possible negative ref

gative-refrat 360 THz wttice of sucolute value

solar cellw material r cells. In ananostructuh the solar ns show thae exceptionthe diffusioen the ARCstood the re

magnetic choped. The pr modificaticonsiders reimportant

om the literat explanatio

nt replaced dispersion o

monic nanoamaterial wand near IR

ce of core-sdetailed studand collectivcubic lattic

fraction in 3

b)

action-indexwhen the G

ch particlesof the refra

s. We havthat theoretall known pure on top o

cell withouat in these rn is the cason length oC does noeason of th

haracterizatipreviously kions of Fresesonant gridphysical efature on so-on of their a plasmoniof the retri

oparticles. with the isotR ranges). Bshell particldy of the ove in cubic

ces: simple,3D arrays of

x isotropic mGaussian bea

. This simuction index

ve suggestetically allowpublicationsof a solar ceut the nanoreported case when the

of carriers (t help, how

his and sug

tion of realknown modsnel formulds on arbitrffect we ca-called Plasanti-reflect

ic grid by aieved perm

We have tropic nega

Both effectivle with sheloptical resp lattices. W, body-centf these parti

metamaterieam illuminaulation is this less than

ed, studied ws the signs the strong

ell (the best ostructure ases the introe thickness (e.g. 100-2wever kno

ggested to

l metasurfadels concerlas or resonrary substraalled substrasmon-enhanting properta bulk layer

mittivity of

suggested ative refractve permittivll of crystalponses of s

We have studered and faicles shaped

al; b) - Spaates the wehe evidencen unity.

and filed nificant oveg enhancemreported re

and withoutoduction of

of the pho00 nm for wn plasmoimplement

aces rned nant ates. ate-

nced ties. r of this

and tion vity l or uch

died ace-d as

atial dge e of

the erall ment

sult t an f the oto-

Si, onic

the

Page 31: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

coverinstrong qcell (barange (bstarted i

Fig. 40solar clead toconcent300 nmdistribuconcent(29% co Metamphotovothermoeincreasethe midfew tencomparsignific

Fig. 42:space gmediumnormalilimitatioabsencecorresp

ng as an arrquadrupole

ased on CIGbased on siin 2011 wit

: (left) – Thcell. The uppo the energtration of th

m thick CIGution at the trated outsiompared to

material fooltaic systeelectric cele of the head-infrared rans of nanomred to the cant increase

: (a) and (b)gap which

m); (c) – theized to thaons). Red ce. The oneponds to the

ray of new response. T

GS). Prelimiilicon). A pth the purpo

The electric fper layer isgy losses. he field in iGS (the bo

upper inteide the met the solar c

r prospecems (NF Tlls operate at transfer cange it pracmeters. Ththermoelec

e of the gap

b) – possibleis small en

e spectrum oat carried curve corree-order gaie photon tun

nanoantennThese new inary resultspre-seed proose of the ex

field spatias the polymThe intermit leads to tttom electr

erface of thetal elementsell without A

tive thermTPVS) conusing the

compared toctically hold

his restrictioctric systemp e.g. from 1

e arrangemenough to suof the radiaby propag

esponds to tin comparennelling acro

31

nas which pcoverings

s were also oject fundedxperimental

al distributioer superstra

mediate laythe energy

rode below e photo-abss. This featARC and 1

mo-photovonverting thso-called po the valueds only whon makes Nms. We ha100 nm to 1

ent of nanotupport the ative heat trgating wavethe presenced to the boss 1 µm ga

possess bothwere simulobtained fo

d by Aalto C demonstrat

on at 370 THate. The con

yer is the conversionit is not s

sorbing layture results1% compar

oltaic systee heat intophoton tunn restricted b

hen the gap NF TPVS

ave suggest µm keepin

tubes in thephoton tun

ransfer acroes only (obce of nanotblack-body ap.

h substrate-lated in 201or a solar ceCenter of Etion of our e

THz in the cencentration100 nm th. The lowershown); (riyer. It is cles in the strored to the ca

ems. So-cao electricitneling whicby the backbetween twtoo expens

ted a metang the same

(c) e system (d1 nnelling frooss one micbeying thertubes, dashe

transfer i

-induced bia11 for an inell operatingEntrepreneueffect (see F

entral crossn of the fieldhick p-doper layer is wight) – Theear that therong overalase when AR

alled near-ty more efch leads tok-body limiwo media issive and noamaterial th

level of the

is the 20-5om nanotubcron gap. Trefore to ted black cuin absence

anisotropy nter-band sog in the visi

urship has bFig. 41).

s section of d in it does ed CIGS.

weakly n-dope same spae hot spots l enhancemRC is presen

-field thermfficiently to the dramit. Howevers as small aot competithat allows e heat transf

0 nm thick fbes to the cThe spectrumthe black-burve – to th

of nanotu

and olar ible

been

f the not The ped

atial are

ment nt).

mo-than

matic r, in as a tive the

fer.

free cold m is ody heir ubes

Page 32: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

32

Our metamaterial does not support neither electron nor phonon heat transfer which could suppress the photovoltaic conversion in the cold medium. The micron gap can be implemented in a relatively inexpensive way with precision 50 nm over the area 1 mm2. Such cells can be unified in a large panel. The implementation of our idea can result in a breakthrough in the thermo-photovoltaics, especially if we manage to obtain similar results in the near IR range, where the micron-gap thermo-photovoltaic systems comprising our material will make possible the waste heat conversion with the same overall efficiency as that of near-IR solar cells (i.e. up to 20-25%). Presently, the best micron-gap thermo-photovoltaic systems based on Ge or CdTe demonstrate the efficiency 3% (alone) or 6% (combined with wafer solar cells). The idea and corresponding results are illustrated by Fig. 42.

4. Participation in European projects Co-ordination: TUMESA SMARAD (Aalto University Department of Radio Science and Engineering) was the coordinator of project TUMESA (MEMS Tuneable Metamaterials for Smart Wireless Applications), which was funded by the European Community within Seventh Framework Programme, Information and Communication Technologies theme. Prof. Antti Räisänen was the Chairman of the Governing Board and Dr. Dmitry Chicherin was the Project Manager until April 2011, and during the remaning time Dr. Juha Ala-Laurinaho was the Project Manager. In addition to Aalto University, the project partners were KTH - Royal Institute of Technology, University of Rennes I, Autocruise S.A. and MicroComp Nordic AB. The objective of the project was to develop components and sub-systems based on microelectromechanical systems (MEMS) in order to provide a cost-efficient and high-performance technology platform for millimetre-wave automotive and industrial radar and future high-capacity communication systems. More precisely, the main goals of the project were: to develop novel on-chip phase shifting and beam-steering devices based on MEMS tuneable high-impedance surfaces; to integrate developed phase shifting components in novel space-efficient antenna arrays on a single chip; to elaborate novel concepts of implementation the beam-steering devices and antenna arrays in cost-efficient radar sensor and future high-capacity wireless communication systems and evaluate fabricated prototypes at a system level. Most of the projects goals were achieved. Duration of the project was 3 years and 4 months, from 1 June 2008 to 30 September 2011. The project website is http://radio.tkk.fi/tumesa. Participation: METACHEM From September 2009, SMARAD has been active in the FP7 Research Project METACHEM, Nano-chemistry and self-assembly routes to metamaterials for visible light. Prof. Simovski is responsible for the theoretical part of WP1 of this project and represents the contribution of Aalto into it. WP1 is considered as a step towards a 3D-isotropic metamaterial, operating in the visible range and demonstrating epsilon-near-zero, mu-near-zero, and negative refraction properties without strong spatial dispersion. ARTEMOS From April 2010, SMARAD has been active in ENIAC research project ARTEMOS (Agile RF Transceivers and Front-Ends for Future Smart Multi-Standard Communications Applications). This project aims at developing architecture and technologies for implementing agile radio frequency

Page 33: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

33

(RF) transceiver capacities in future radio communication products. These new architecture and technologies will be able to manage multi-standard (multi-band, multi-data-rate, and multi-waveform) operation with high modularity, low-power consumption, high reliability, high integration, low costs, low PCB area, and low bill of material (BOM). Prof. Jussi Ryynänen, is reponsible of developing direct delta-sigma receiver in WP4 of this project. RODIN From 2010, SMARAD has been active in the FP7 Reseach Project RODIN (Suspended Graphene Nanostructures). The RODIN-project is organized around the concept of suspended single-and few-layer graphene nanostructures and annealed diamond-like carbon films. In particular project focuses on engineering and measuring the mechanical and electromechanical properties. Prof. Jussi Ryynänen, is reponsible of evaluating electrical performance of developed mechanical resonators.

5. SMARAD funding In 2011 SMARAD funding was as follows: RAD SA MNT Total Univ. budget (incl. extra funding for CoE) 1.216.000 404.000 511.000 2.131.000 External (competitive) funding 1.940.000 965.000 1.613.000 4.518.000 Total 3.156.000 1.369.000 2.124.000 6.649.000 External funding from the following sources:

- Academy of Finland (CoE) 351.000 136.000 79.000 566.000 - Academy of Finland 519.000 481.000 421.000 1.421.000 - TEKES 418.000 68.000 309.000 795.000 - GETA 83.000 25.000 67.000 175.000 - ESA 40.000 - - 40.000 - EU 305.000 1.000 98.000 404.000 - Finnish industry and other domestic 224.000 254.000 639.000 1.117.000

6. SMARAD personnel during year 2011 In the Department of Radio Science and Engineering: Ala-Laurinaho, Juha, D.Sc. (Tech.) Senior scientist Albooyeh, Mohammad, M.Sc. Doctoral student from February 9th Alitalo, Pekka, D.Sc. (Tech.) Post-doctoral researcher Amin, Amee, B.Sc. Research assistant from June 1st to August 31st Bin Abdullah Al-Hadi, Azremi, M.Sc. Doctoral student Chicherin, Dmitry, Lic.Sc. (Tech.) Doctoral student until April 30th Dahlberg, Krista, Lic.Sc. (Tech.). Doctoral student Du, Zhou, M.Sc. Doctoral student Ermolov, Kirill, Mr. Research assistant from June 1st to August 31st Generalov, Andrey, M.Sc. Doctoral student Geng, Suiyan, Lic.Sc. (Tech.) Doctoral student from September 1st to October 31st Haapiainen-Laine, Sari, B.Sc. Project secretary Haimakainen, Johannes, Mr. Research assistant from June 1st to October 31st

Page 34: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

34

Haneda, Katsuyuki, D.Sc. Post-doctoral researcher Hashemi, Seyedmohammade, M.Sc. Stipendiate from October 17th Hernandez Zamora, Bruno, B.Sc. Erasmus stipendiate from October 17th Holopainen, Jari, D.Sc. (Tech.) University teacher Huang, Yi, B.Sc. Research assistant from June 1st to August 31st Icheln, Clemens, D.Sc. (Tech.) Senior lecturer Ilvonen, Janne, M.Sc. (Tech.) Doctoral student Järveläinen, Jan, M.Sc. (Tech.) Doctoral student Kahra, Eino, Mr. Laboratory technician Kari, Henri, Mr. Research assistant from June 1st to August 31st Karilainen, Antti, M.Sc. (Tech.) Doctoral student Karttunen, Aki, Lic.Sc. (Tech.) Doctoral student Khanal, Subash, B.Sc. Research assistant from June 1st Khatun, Afroza Mst, M.Sc. Doctoral student Kiuru, Tero, M.Sc. (Tech.) Doctoral student until November 27th Kivekäs, Outi, D.Sc. (Tech.) Post-doctoral researcher until May 22nd Kolmonen, Veli-Matti, D.Sc. (Tech.) Post-doctoral researcher Kyrö, Mikko, Lic.Sc. (Tech.) Doctoral student Laakso, Lauri, Mr. Laboratory technician Laitinen Tommi, D.Sc. (Tech.) Senior scientist Lindberg, Stina, B.Sc. (Econ.) HR Secretary Lioubtchenko, Dmitri, Ph.D. Academy research fellow Luukkonen, Olli, D.Sc. (Tech.) Post-doctoral researcher until May 31st Maksimovitch, Yelena, Dr. Researcher from June 16th to July 22nd and from November

24th to December 22nd Mallat, Juha, D.Sc. (Tech.) Senior university lecturer Medina Acosto, Gerardo, B.Sc. Erasmus stipendiate until January 19th Meriläinen Mikko, Mr. Research assistant from January 13th to May 31st Mikhnev, Valeri, Dr. Senior scientist from June 13th Morits, Dmitry, M.Sc. Doctoral student Mylläri, Tuula, Ms. Secretary Mäkelä, Sampo, Mr. Research assistant from June 1st Nefedov, Igor, Dr.Sc. Senior scientist Niemi, Teemu, B.Sc. (Tech.). Research assistant Olkkonen, Martta-Kaisa, M.Sc. (Tech.)Doctoral student Parveg, Dristy, M.Sc. Doctoral student Planman, Irma, Ms. HR Secretary Pousi, Patrik, D.Sc. (Tech.) Post-doctoral researcher until June 30th Podlozny, Vladimir, Ph.D. Project manager and senior scientist Popovic, Delia, Ms. Project secretary from August 1st Poutanen, Juho, M.Sc. (Tech.) Doctoral student until January 16th Rasilainen, Kimmo, B.Sc. Research assistant Robertson, Jean-Baptiste, M.Sc.Eng Project coordinator until March 31st Räisänen, Antti, D.Sc. (Tech.) Professor, Head of the department Salo, Sampo Research assistant from June 1st to August 31st Schmuckli, Lorenz, Mr. Laboratory technician Sibakov, Viktor, M.Sc. (Tech.) Laboratory manager Simovski, Constantin, Dr.Sc. Visiting professor Song, Jinsong, B.Sc. Research assistant from January 24th Tamminen, Aleksi, Lic.Sc. (Tech.) Doctoral student

Page 35: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

35

Takizawa, Kenichi, Dr. Visiting researcher from August 17th Tretyakov, Sergei, Dr.Sc. Professor Vahdati, Ali, M.Sc.(Tech.) Doctoral student from January 26th to July 31st Valkonen, Risto, M.Sc. (Tech.) Doctoral student Vainikainen, Pertti, D.Sc. (Tech.) Professor Vehmas, Joni, B.Sc. (Tech.) Research assistant Virk, Usman, B.Sc. Research assistant from February 1st Zvolensky, Tomas, M.Sc. Doctoral student In the Department of Signal Processing and Acoustics: Aho, Janne, B.Sc. (Tech.) Research assistant from August 3rd Aittomäki, Tuomas, M.Sc. (Tech.) Doctoral student Balakrishnan, Arun, Mr. Stipendiate until August 31st Bica, Marian, B.Sc. Research assistant Bysany D., Satish, B.Sc. Research assistant from March 21st Chaudhari, Sachin, M.Sc. Doctoral student Cierny, Michal, M.Sc. Doctoral student Dhamala, Ujjwal, B.Sc. Research assistant Eriksson, Jan, D.Sc. (Tech.) Senior scientist Haghparast, Azadeh, M.Sc. Doctoral student until July 27th Hynninen, Jussi, M.Sc. (Tech.) Computer administrator Jacob Mathecken, Pramod, M.Sc. Doctoral student Jänis, Pekka, M.Sc. (Tech.) Doctoral student Kashyap, Neelabh, B.Sc. Research assistant from January 12th Koivisto, Tommi, M.Sc. (Tech.) Doctoral student Koivunen, Visa, D.Sc. (Tech.) Academy professor Le, Vieth-Anh, M.Sc. Doctoral student from October 10th Lemetyinen, Mirja, Ms. HR secretary Lundén, Jarmo, D.Sc. (Tech.) Post-doctoral researcher Oborina, Alexandra, M.Sc. Doctoral student Ojaniemi, Jaakko, M.Sc. Doctoral student from December 5th Oksanen, Jan, M.Sc. Doctoral student Ollila, Esa, D.Sc. (Tech.) Academy research fellow Pereira Da Costa, Mario, M.Sc. Doctoral student Pölönen, Keijo, M.Sc. (Tech.) Doctoral student Rajasekharan, Jayaprakash, M.Sc. Doctoral student Razavi, Seyed Alireza, D.Sc. (Tech.) Post-doctoral researcher from September 1st Riihonen, Taneli, M.Sc. (Tech.) Doctoral student Richter, Andreas, D.Sc. Professor Saeed, Umar, B.Sc. Research assistant Salmi, Jussi, D.Sc. (Tech.) Post-doctoral researcher Schober, Karol, M.Sc. Doctoral student Sikander, Ulla, Ms. Project secretary Simonen, Tarmo, M.Sc. (Tech.) Computer administrator Werner, Stefan, D.Sc. (Tech.) Academy research fellow Wichman, Risto, D.Sc. (Tech.) Professor In the Department of Micro and Nanosciences: Aaltonen, Lasse, Lic.Sc. (Tech.) Doctoral student Gronicz Jakub, M.Sc. (Eng.) Doctoral student

Page 36: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

36

Halonen, Kari, D.Sc. (Tech.) Professor, Head of the department Kalanti, Antti, M.Sc. (Tech.) Doctoral student Kaltiokallio, Mikko, M.Sc. (Tech.) Doctoral student Kärkkäinen, Mikko, Lic.Sc. (Tech.) Doctoral student Laulainen, Erkka, Mr. Research assistant Nieminen, Tero, M.Sc. (Tech.) Doctoral student Pulkkinen, Mika, B.Sc. Research assistant Rapinoja, Tapio M.Sc. (Tech.) Doctoral student Ryynänen, Jussi, D.Sc. (Tech.) Professor Saari, Ville, Lic.Sc. (Tech.) Doctoral student until 30 April Stadius, Kari, Lic.Sc. (Tech.) Senior researcher Söderman, Lea, Ms. Secretary Tikka, Tero, M.Sc. (Tech.) Doctoral student Turunen, Vesa, M.Sc. (Tech.) Doctoral student Varonen, Mikko, Lic.Sc. (Tech.) Post-doctoral researcher Viitala, Olli, M.Sc. (Tech.) Doctoral student Xu, Liangge, M.Sc. (Tech.) Doctoral student Yucetas, Mikail, M.Sc. (Tech.) Doctoral student

7. Visitors to SMARAD in 2011 Visiting Professors: Ass. Prof. Takahiro Aoyagi, Tokyo Institute of Technology, Japan, 1 week Prof. Olga Glukhova, Saratov State University, Russia, 2 weeks Prof. Gregorio Fernando, Universidad Nacional del Sur, Argentina, 2 weeks Prof. Marcello de Campos, Universidad Federal do Rio de Janeiro, Brazil, 1 week Prof. Sergiy Vorobyov, University of Alberta, Kanada, 1 week Prof. Sumit Roy, University of Washington, USA, 1 week Prof. Vincent H. Poor, Princeton University, USA, 1 week

Visiting Researchers: B.Sc. Bruno Hernandez Zamora, Universidad Autonoma de Madrid, Spain, 4 months B.Eng. Soichi Saito, Tokyo Denki University, Japan, 2 months M.Eng. Daisuke Sugizaki, Tokyo Denki University, Japan, 1 month B.Eng. Kenshiro Tsutsuki, Tokyo Denki University, Japan, 1 month M.Sc. Seyedmohammad Hashemi, Iran University of Science and Technology, Iran, 3 months Dr Constantinos Valagiannopoulos, University of Athens, Greece, 12 months M.Sc. Amin Enayati, IMEC, Katholieke Universiteit Leuven, Belgium, 7 months Dr Yelena Maksimovich, Institute of Applied Physics, Minsk, Belorussia, 2 months Dr Kenichi Takizawa, National Institute of Information and Communications Technology, Japan,

5 months M.Sc. Inigo Liberal, Public University of Navarra, 4 months

8. Visits from SMARAD to foreign institutes in 2011 Dr Pekka Alitalo, German Aerospace Center, Wessling, Germany, 2 months Dr Katsuyuki Haneda, University of Southern California, Los Angeles, USA, 2 weeks Dr Katsuyuki Haneda, Tokyo Denki University, Japan, 2 weeks

Page 37: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

37

Prof. Constantin Simovski, ITMO, St. Petersburg, 2 weeks M.Sc. Tomas Zvolensky, Queen's University, Belfast, UK, 1 month Dr Marko Kosunen, University of California, Berkeley, USA 3 months Dr Mikko Varonen, JPL California Institute of Technology, USA, 11 months Academy prof. Visa Koivunen, Princeton University, USA, 2 months Dr Jarmo Lunden, Princeton University, USA, 8 months M.Sc. (Tech.) Jan Oksanen, Princeton University, USA, 2 months Dr Esa Ollila, Princeton University, USA, 8 months Dr Jussi Salmi, University of Southern California, USA, 1 month

9. Post-graduate degrees Doctor of Science (Technology) degrees in 2011: Jari Holopainen Compact UHF-band antennas for mobile terminals: focus on modelling,

implementation, and user interaction Thesis defence: 29 April 2011 Opponents: Prof. Dirk Manteuffel, Christian-Albrechts-Universität, Kiel, Germany, and Dr Kevin Boyle, EPCOS, UK Ltd, U.K. Preliminary examiners: Prof. Ph.D. Koichi Ito, Chiba University, Japan, and Dr Ping Hui, Nokia Corporation, Canada Supervisor: Prof. Pertti Vainikainen

Ville Saari Continuous-time low-pass filters for integrated wideband radio receivers Thesis defence: 29 April 2011 Opponent: Prof. Mohammed Ismail, The Ohio State University, USA Preliminary examiners: Assoc. Prof. Andrea Baschirotto, University of Milano-Bicocca, Italy, and Dr Kimmo Koli, ST-Ericsson, Finland Supervisor: Prof. Jussi Ryynänen

Juho Poutanen Geometry-based radio channel modelling: Proopagation analysis and concept development Thesis defence: 13 May 2011 Opponents: Dr Jonas Medbo, Ericsson Research, Sweden, and Prof. Martine Lienard, University of Lille, France Preliminary examiners: Prof. Mir Ghoraishi, Tokyo Institute of Technology, Japan, and Dr Tricia Willink, Communication Research Centre, Canada Supervisor: Prof. Pertti Vainikainen

Suiyan Geng Millimeter wave and UWB poropagation for high throughput indoor communications Thesis defence: 2 November 2011 Opponent: Fredrik Tufvesson, Lund University, Sweden Preliminary examiners: Dr Chia-Chin Chong, NTT Dokomo Labs, Palo Alto, USA, and Prof. Hirokazu Sawada, Tohoku University, Sendai, Japan Supervisor: Prof. Pertti Vainikainen

Tero Kiuru Characterization, modelling, and design for applications of waveguide impedance tuners and Schottky diodes at millmeter wave lengths Thesis defence: 12 December 2011 Opponent: Prof. Jan Stake, Chalmers University of Technology, Gothenburg, Sweden

Page 38: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

38

Preliminary examiners: Dr Thomas Crowe, Virginia Diodes Inc., Charlottesville, USA, and Dr Imran Mehdi, Jet Propulsion Laboratory, Pasadena, USA Supervisor: Prof. Antti Räisänen

Dmitri Chicherin Studies on microelectromechanically tuneable high-impedance surface for millimetre wave beam steering Thesis defence: 2 December 2011 Opponent: Prof. Didier Lippens, Université des Sciences et Technologie de Lille, France Preliminary examiners: Prof. Wolfgang Menzel, University of Ulm, Germany, and Dr Tauno Vähä-Heikkilä, VTT Technical Research Centre of Finland Supervisor: Prof. Antti Räisänen

Licentiate of Science (Technology) degrees in 2011: Krista Dahlberg Mixer test jig for millimeter wave Schottky diodes (Testialusta milimetri-

aaltoalueen Schottky-diodeille) Graduation date: 7 February 2011

Supervisor: Prof. Antti Räisänen External examiner: Dr. Jyrki Louhi, Nokia Siemens Networks

Aleksi Tamminen On developments in submillimeter-wavelength imaging

(Alimillimetriaaltoalueen kuvantamismenetelmien kehittämisestä) Graduation date: 6 October 2011 Supervisor: Prof. Antti Räisänen External examiner: Dr Ville Viikari, VTT Technical Research Centre of Finland

10. Publications 10.1 Articles in scientific journals with peer-review

[1] M. Albooyeh, D. Morits, and C. Simovski, “Electromagnetic characterization of substrated metasurfaces,” Metamaterials, vol. 5, no. 3, pp. 93–111, 2011.

[2] M. Albooyeh and C. Simovski, “Substrate-induced bianisotropy in plasmonic grids,” Journal of Optics A, vol. 13, no. 2, p. 105102, 2011.

[3] P. Alitalo, A. O. Karilainen, T. Niemi, C. R. Simovski, and S.A. Tretyakov, “Design and realisation of an electrically small Huygens source for circular polarization,” IET Microwaves, Antennas & Propagation, vol. 5, no. 7, pp. 783–789, 2011.

[4] P. Alitalo and S. Tretyakov, “Broadband electromagnetic cloaking realized with transmission-line and waveguiding structures (invited paper),” Proceedings of the IEEE, vol. 99, no. 10, pp. 1646–1659, 2011.

[5] D. Baranov, A. Vinogradov, C. Simovski, I. Nefedov, and S. Tretyakov, “On the electrodynamics of an absorptive uniaxial non-positively definite (indefinite) medium,” Journal of Experimental and Theoretical Physics, vol. 141, no. 9, pp. 1–9, 2011.

[6] L. Bergamin, P. Alitalo, and S. Tretyakov, “Nonlinear transformation optics and engineering of the Kerr effect,” Physical Review B, p. 205103, 2011.

Page 39: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

39

[7] A. Bin Abdullah Al-Hadi, J. Ilvonen, R. Valkonen, J. Holopainen, O. Kivekäs, C. Icheln, and P. Vainikainen, “Coupling element –based dual-antenna structures with hand effects,” Int. J. of Wireless Information Networks, vol. 18, no. 3, pp. 146–157, 2011.

[8] A. Bin Abdullah Al-Hadi, V. Papamichael, and P. Vainikainen, “Multi-antenna mobile terminal diversity performance in proximity to human hands under different propagation environment conditions,” Electronics Letters, vol. 47, pp. 1214–1215, 2011.

[9] D. Chicherin, M. Sterner, D. Lioubtchenko, J. Oberhammer, and A.V. Räisänen, “Analog-type millimeter-wave phase shifters based on MEMS tunable high-impedance surface and dielectric rod waveguide,” Int. J. of Microwave and Wireless Technologies, vol. 3, no. 5, pp. 533–538, 2011.

[10] F. Costa, O. Luukkonen, C. Simovski, A. Monorchio, S. Tretyakov, and P. de Maagt, “TE surface wave resonances on high-impedance surface based antennas: Analysis and modeling,” IEEE Trans. on Antennas and Propagation, vol. 59, no. 10, pp. 3588–3596, 2011.

[11] J. Holopainen, O. Kivekäs, J. Ilvonen, R. Valkonen, C. Icheln, and P. Vainikainen, “Effect of the user's hands on the operation of lower UHF-band mobile terminal antennas: Focus on digital television receiver,” IEEE Trans. on Electromagnetic Compatibility, vol. 53, no. 3, pp. 831–841, 2011.

[12] J. Ilvonen, O. Kivekäs, J. Holopainen, R. Valkonen, K. Rasilainen, and P. Vainikainen, “Mobile terminal antenna performance with the user's hand: Effect of antenna dimensioning and location,” IEEE Antennas and Wireless Propagation Letters, vol. 10, pp. 772–775, 2011.

[13] J. Ilvonen, R. Valkonen, O. Kivekäs, P. Li, and P. Vainikainen, “Antenna shielding method reducing the interaction between user and mobile terminal antenna,” Electronics Letters, vol. 47, no. 16, pp. 896–897, 2011.

[14] A.O. Karilainen, P.M.T. Ikonen, C.R. Simovski, S.A. Tretyakov, A.N. Lagarkov, S.A. Maklakov, K.N. Rozanov, and S.N. Starostenko, “Experimental studies on antenna miniaturisation using magneto-dielectric and dielectric materials,” IET Microwaves, Antennas & Propagation, vol. 5, no. 4, pp. 495–502, 2011.

[15] A.O. Karilainen, P.M.T. Ikonen, C.R. Simovski, and S A. Tretyakov, “Choosing dielectric or magnetic material to optimize the bandwidth of miniaturized resonant antennas,” IEEE Trans. on Antennas and Propagation, vol. 59, no. 11, pp. 3991–3998, 2011.

[16] A.O. Karilainen, J. Vehmas, O. Luukkonen, and S.A. Tretyakov, “High-impedance-surface-based antenna with two orthogonal radiating modes,” IEEE Antennas and Wireless Propagation Letters, vol. 10, pp. 247–250, 2011.

[17] T. Kiuru, J. Mallat, A.V. Räisänen, and T. Närhi, “Schottky diode series resistance and thermal resistance extraction from S-parameter and temperature controlled I–V measurements,” IEEE Trans. on Microwave Theory and Techniques, vol. 59, no. 8, pp. 2108–2116, 2011.

[18] O. Kozina, I. Nefedov, L. Melnikov, and A. Karilainen, “Plasmonic coaxial waveguides with complex shapes of cross-sections,” Materials, vol. 4, pp. 104–116, 2011.

[19] O.N. Kozina, L.A. Melnikov, and I.S. Nefedov, “Strong field localization in subwavelength metal-dielectric optical waveguides,” Optics and Spectroscopy, vol. 111, no. 2, pp. 241–247, 2011.

[20] M. Kyrö, K. Haneda, J. Simola, K. Nakai, K.-i. Takizawa, H. Hagiwara, and P. Vainikainen, “Measurement based path loss and delay spread modeling in hospital environments at 60 GHz,” IEEE Trans. on Wireless Communications, vol. 10, no. 8, pp. 2423–2427, 2011.

[21] I. Liberal, I. S. Nefedov, I. Ederra, R. Gonzalo, and S.A. Tretyakov, “Electromagnetic response and homogenization of grids of ferromagnetic microwires,” J. of Applied Physics, vol. 110, no. 6, p. 064909, 2011.

[22] I. Liberal, I. Nefedov, I. Ederra, R. Gonzalo, and S. Tretyakov, “On the effective permittivity of arrays of ferromagnetic wires,” J. of Applied Physics, vol. 110, p. 104902, 2011.

Page 40: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

40

[23] O. Luukkonen, S.I. Maslovski, and S.A. Tretyakov, “A stepwise Nicolson-Ross-Weir -based material parameter extraction method,” IEEE Antennas and Wireless Propagation Letters, vol. 10, pp. 1295–1298, 2011.

[24] A. Miroshnichenko, I. Maksymov, A. Davoyan, C. Simovski, P. Belov, and Y. Kivshar, “An arrayed nanoantenna for broadband light emission and detection,” Physica Status Solidi - Rapid Research. Letters, vol. 3, no. 3, pp. 347–349, 2011.

[25] D. Morits and C. Simovski, “Isotropic negative effective permeability in the visible range produced by clusters of plasmonic triangular nanoprisms,” Metamaterials, vol. 5, no. 4, pp. 162–168, 2011.

[26] S. Myllymäki, R. Valkonen, J. Holopainen, A. Huttunen, V.K. Palukuru, M. Berg, H. Jantunen, and E. Salonen, “Capacitive-sensor-induced losses in 900-, 1800-, and 1900-MHz antennas,” IEEE Antennas and Wireless Propagation Letters, vol. 10, pp. 330–333, 2011.

[27] I.S. Nefedov and S.A. Tretyakov, “Ultrabroadband electromagnetically indefinite medium formed by aligned carbon nanotubes,” Physical Review B, vol. 84, p. 113410, 2011.

[28] I.S. Nefedov and S.A. Tretyakov, “Effective medium model for two-dimensional periodic arrays of carbon nanotubes,” Photonics and Nanostructures - Fundamentals and Applications, vol. 9, no. 4, pp. 374–380, 2011.

[29] I. Nefedov and C. Simovski, “Giant radiation heat transfer through micron gaps,” Physical Review B, vol. 84, p. 195459, 2011.

[30] P. Padilla, J.P. Pousi, A. Tamminen, J. Mallat, J. Ala-Laurinaho, M. Sierra-Castaner, and A.V. Räisänen, “Experimental determination of DRW antenna phase center at mm-wavelengths using a planar scanner: comparison of different methods,” IEEE Trans. on Antennas and Propagation, vol. 59, no. 8, pp. 2806–2812, 2011.

[31] J. Poutanen, J. Salmi, K. Haneda, V.-M. Kolmonen, and P. Vainikainen, “Angular and shadowing characteristics of dense multipath components in indoor radio channels,” IEEE Trans. on Antennas and Propagation, pp. 245–253, 2011.

[32] C. Schmidt, T. Laitinen, and T. Eibert, “Hybrid fast Fourier transform-plane wave based near-field far-field transformation for “body of revolution” antenna measurement grids,” Radio Science, p. 004640, 2011.

[33] C. Simovski, “On electromagnetic characterization and homogenization of nanostructured metamaterials,” Journal of Optics, vol. 13, no. 1, p. 013001, 2011.

[34] M. Sterner, N. Somjit, U. Shah, S. Dudorov, D. Chicherin, A.V. Räisänen, and J. Oberhammer, “Microwave MEMS devices designed for process robustness and operational reliability,” Int. J. of Microwave and Wireless Technologies, vol. 3, no. 5, pp. 547–563, 2011.

[35] S. Steshenko, F. Capolino, P. Alitalo, and S. Tretyakov, “Effective model and investigation of the near-field enhancement and subwavelength imaging properties of multilayer arrays of plasmonic nanospheres,” Physical Review E, vol. 84, no. 1, p. 016607, 2011.

[36] J. Toivanen, T. Laitinen, V.-M. Kolmonen, and P. Vainikainen, “Reproduction of arbitrary radio-channel environment,” IEEE Trans. on Instrumentation and Measurement, vol. 60, no. 1, pp. 275–281, 2011.

[37] S. Tretyakov, “Bianisotropic materials optimized for strong interactions with electromagnetic fields,” Problems of Physics, Mathematics, and Technics (Special issue on the occasion of the centenary of F.I. Fedorov, invited paper), vol. 2, no. 7, pp. 49–51, 2011.

[38] C. Valagiannopoulos, “The influence of electromagnetic scattering from a permeable sphere on the induced voltage across a rotating eccentric coil,” Journal of Electromagnetic Analysis and Applications, vol. 3, no. 1, p. 6, 2011.

[39] C. Valagiannopoulos, “Electromagnetic scattering of the field of a metamaterial slab antenna by an arbitrarily positioned cluster of metallic cylinders,” Progress in Electromagnetic Research, vol. 114, p. 16, 2011.

Page 41: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

41

[40] C.A. Valagiannopoulos and N.K. Uzunoglu, “Simplified model for EM inverse scattering by longitudinal subterranean inhomogeneities exploiting the dawn/dusk ionospheric ridge,” IET Microwaves, Antennas & Propagation, vol. 5, no. 11, pp. 1319–1327, 2011.

[41] C.A. Valagiannopoulos, “Electromagnetic propagation into parallel-plate waveguide in the presence of a skew metallic surface,” Taylor & Francis Electromagnetics, vol. 31, no. 8, pp. 593–605, 2011.

[42] C.A. Valagiannopoulos, “High selectivity and controllability of a parallel-plate waveguide component with a filled rectangular ridge,” Progress in Electromagnetic Research, vol. 119, pp. 497–551, 2011.

[43] J. Vehmas, P. Alitalo, and S.A. Tretyakov, “Transmission-line cloak as an antenna,” IEEE Antennas and Wireless Propagation Letters, vol. 10, no. 1, pp. 1594–1597, 2011.

[44] A. Vinogradov, A. Ignatov, A. Merzlikin, S. Tretyakov, and C. Simovski, “Additional effective medium parameters for composite materials (excess surface currents),” Optics Express, vol. 19, no. 7, pp. 6699-6704, 2011.

[45] K. Yamamoto, K. Haneda, H. Murata, and S. Yoshida, “Optimal transmission scheduling for a hybrid of full- and half-duplex relaying,” IEEE Communication Letters, vol. 15, no. 3, pp. 305–307, 2011.

[46] T. Zvolensky, D. Chicherin, A.V. Räisänen, and C. Simovski, “Leaky-wave antenna based on micro-electromechanical systems-loaded microstrip line,” IET Microwaves, Antennas & Propagation, vol. 5, no. 3, pp. 357–363, 2011.

[47] L. Aaltonen, A. Kalanti, M. Pulkkinen, M. Paavola, M. Kämäräinen, and K. Halonen, “A 2.2 mA 4.3 mm2 ASIC for a 1000 degrees/s 2-axis capacitive micro-gyroscope,” IEEE Journal of Solid-State Circuits, vol. 46, no. 7, pp. 1682–1692, July 2011.

[48] V. Turunen, M. Kosunen, S. Kallioinen, A. Pärssinen, and J. Ryynänen, “Spectrum sensor hardware implementation based on cyclostationary feature detector,” Majlesi Journal of Electrical Engineering, vol. 5, no. 1, pp 32–37, March 2011.

[49] F. Gregorio, J. Cousseau, S. Werner, T. Riihonen, and R. Wichman, “Predistorter with IQ imbalance and crosstalk compensation for broadband MIMO OFDM transmitters,” EURASIP Journal on Advances in Signal Processing, 2011, pp. 1–15, July 2011.

[50] F. Gregorio, S. Werner, J. Cousseau, J. Figueroa, and R. Wichman, “Receiver-side nonlinearities mitigation using an extended iterative decision-based technique,” Signal Processing, vol. 91, pp. 2042–2056 March 2011.

[51] M. Husso, J. Hämäläinen, R. Jäntti, J. Nieminen, T. Riihonen, and R. Wichman, “Performance of on-off scheduling strategy in the presence of transmit beamforming,” Physical Communication, vol. 4, no. 1, pp. 3–12, March 2011.

[52] P. Jänis, C. Ribeiro, and V. Koivunen, “Interference aware radio resource management for local area wireless networks,” EURASIP Journal on Wireless Communication and Networking, vol. 2011, article ID 921623, pp. 1–15, 2011.

[53] P. Mathecken, T. Riihonen, S. Werner, and R. Wichman, “Performance analysis of OFDM with Wiener phase noise and frequency selective fading channel,” IEEE Trans. on Communications, vol. 59, pp. 1321–1331, May 2011.

[54] M. Novey, E. Ollila, and T. Adali, “On testing the extent of noncircularity,” IEEE Transactions on Signal Processing, vol. 59, no. 11, pp. 5632–5637, 2011.

[55] E. Ollila, J. Eriksson, and V. Koivunen, “Complex elliptically symmetric random variables - generation, characterization and circularity tests,” IEEE Trans. on Signal Processing, vol. 59, no. 1, pp. 58–69, 2011.

[56] R.-A. Pitaval, H.-L. Määttänen, K. Schober, O. Tirkkonen, and R. Wichman, “Beamforming codebooks for two transmit antenna systems based on optimum Grassmannian packings,” IEEE Trans. on Information Theory, vol. 57, no. 10, pp. 6591–6602, October 2011.

Page 42: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

42

[57] Man-On Pun, V. Koivunen, and H.V. Poor, “Performance analysis of joint opportunistic scheduling and receiver design for MIMO-SDMA downlink systems,” IEEE Trans. on Communications, vol. 59, no. 1, pp. 268–280, 2011.

[58] J. Remes, T. Starck, J. Nikkinen, E. Ollila, C. Beckmann, O. Tervonen, V. Kiviniemi, and O. Silven, “Effcts of repeatibility measures on results of fMRI sICA: a study on simulated and real resting-state effects,” NeuroImage, vol. 56, no. 2, pp. 554–569, 2011.

[59] T. Riihonen, S. Werner, and R. Wichman, “Hybrid full-duplex/half-duplex relaying with transmit power adaptation,” IEEE Trans. on Wireless Communications, vol. 10, pp. 3074–3085, Sept. 2011.

[60] T. Riihonen, S. Werner, and R. Wichman, “Mitigation of self-interference in full-duplex MIMO relays,” IEEE Transactions on Signal Processing, vol. 59, pp. 5983–5993, Dec. 2011.

[61] T. Riihonen, R. Wichman, and J. Hämäläinen, “Performance analysis of maximum SNR scheduling with an infrastructure relay link,” Wireless Personal Communications, vol. 56, no. 2, pp. 277–299, Jan. 2011.

[62] J. Salmi and A.F. Molisch, “Propagation parameter estimation, modeling and measurements for ultrawideband MIMO radar,” IEEE Trans. on Antennas and Propagation, vol. 59, no. 11, pp. 4257–4267, 2011.

[63] C. Schmidt, J. Figueroa, J. Cousseau, R. Wichman, and S. Werner, “Nonlinearities modeling and post-compensation in continuous-time sigma-delta modulators,” IET Microwaves, Antennas & Propagation, vol. 5, pp. 1796–1804, Dec. 2011.

[64] J.F. Schmidt, J.E. Cousseau, R. Wichman, and S. Werner, “Bit loading using imperfect CSIR for prediction based resource allocation in mobile OFDMA,” IEEE Trans. on Vehicular Technology, vol. 60, pp. 4082–4088, Oct. 2011.

[65] J.F. Schmidt, J.E. Cousseau, R. Wichman, and S. Werner, “Low-complexity channel prediction using approximated recursive DCT,” IEEE Trans. on Circuits and Systems I, vol. 58, pp. 2520–2530, Oct. 2011.

10.2 Articles in conference proceedings and in other edited works

[1] A. Karttunen, J. Ala-Laurinaho, R. Sauleau, and A.V. Räisänen, “Optimal eccentricity of a low permittivity integrated lens for a high-gain beamsteering antenna,” in Proc. of the 5th European Conference on Antennas and Propagation, EuCAP2011, Rome, Italy, 11-15 April, 2011.

[2] A.V. Räisänen, J. Ala-Laurinaho, A. Karttunen, J. Mallat, P. Pousi, and A. Tamminen, “Recent activities on antenna measurements at mm- and submm-wavelengths at Aalto University,” in Proc. of the 5th European Conference on Antennas and Propagation, EuCAP2011, Rome, Italy, 11-15 April, 2011.

[3] R. Sauleau, O. Biro, J. Stiens, Z. Sipus, A.V. Räisänen, L.-P. Schmidt, C.A. Fernandes, J. Mosig, V. Fusco, S. Maci, A. Neto, A.I. Nosich, A.V. Boriskin, “Newfocus research networking program,” in Proc. of the 5th European Conference on Antennas and Propagation, EuCAP2011, Rome, Italy, 11-15 April, 2011.

[4] J.P. Pousi, D.V. Lioubtchenko, and A.V. Räisänen, “High permittivity rectangular dielectric rod waveguide for 110-325 GHz,” in Proc. of the Millimetre Wave Days: The 6th ESA Workshop on Millimetre-Wave Technology and Applications, and The 4th Global Symposium on Millimeter Waves GSMM2011, May 23-25, 2011, Espoo, Finland.

[5] Z. Du, D. Chicherin, and A.V. Räisänen, “Beam steering with MEMS-based HIS on a lossy sillicon substrate at 80 GHz,” in Proc. of the Millimetre Wave Days: The 6th ESA Workshop on Millimetre-Wave Technology and Applications, and The 4th Global Symposium on Millimeter Waves GSMM2011, May 23-25, 2011, Espoo, Finland.

[6] K. Dahlberg, T. Kiuru, J. Mallat, A.V. Räisänen, and T. Närhi, “Mixer test jig for millimeter wave Schottky diodes,” in Proc. of the Millimetre Wave Days: The 6th ESA Workshop on

Page 43: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

43

Millimetre-Wave Technology and Applications, and The 4th Global Symposium on Millimeter Waves GSMM2011, May 23-25, 2011, Espoo, Finland.

[7] A. Enayati, G.A.E. Vandenbosch, W. De Raedt, and A.V. Räisänen, “Multilayer PCB technology for antenna-in-package solution at millimetrewave frequencies,” in Proc. of the Millimetre Wave Days: The 6th ESA Workshop on Millimetre-Wave Technology and Applications, and The 4th Global Symposium on Millimeter Waves GSMM2011, May 23-25, 2011, Espoo, Finland.

[8] A.A. Generalov, D.V. Lioubtchenko, J. Mallat, V. Ovchinnikov, and A.V. Räisänen, “Novel RF power sensor on Si rod waveguide,” in Proc. of the Millimetre Wave Days: The 6th ESA Workshop on Millimetre-Wave Technology and Applications, and The 4th Global Symposium on Millimeter Waves GSMM2011, May 23-25, 2011, Espoo, Finland.

[9] R. Sauleau, O. Biro, J. Stiens, Z. Sipus, A.V. Räisänen, L.-P. Schmidt, C.A. Fernandes, J. Mosig, V. Fusco, S. Maci, A. Neto, A.I. Nosich, and A.V. Boriskin, “Newfocus research networking program,” in Proc. of the Millimetre Wave Days: The 6th ESA Workshop on Millimetre-Wave Technology and Applications, and The 4th Global Symposium on Millimeter Waves GSMM2011, May 23rd – May 25th, 2011, Espoo, Finland.

[10] A. Tamminen, J. Ala-Laurinaho, J. Häkli, P. Koivisto, J. Säily, A. Luukanen, and A.V. Räisänen, “Reflectarray design for 120-GHz MMID application: simulation results,” in Proc. of the Millimetre Wave Days: The 6th ESA Workshop on Millimetre-Wave Technology and Applications, and The 4th Global Symposium on Millimeter Waves GSMM2011, May 23-25, 2011, Espoo, Finland.

[11] T. Kiuru, A. Gonzalez Garcia, and T. Närhi, “MMIC subharmonic mixer for 94 GHz,” in Proc. of the Millimetre Wave Days: The 6th ESA Workshop on Millimetre-Wave Technology and Applications, and The 4th Global Symposium on Millimeter Waves GSMM2011, May 23-25, 2011, Espoo, Finland.

[12] A. Karttunen, J. Ala-Laurinaho, R. Sauleau, A.V. Räisänen, “Reduction of internal reflections in low permittivity integrated lens antennas,” in Proc. of the Millimetre Wave Days: The 6th ESA Workshop on Millimetre-Wave Technology and Applications, and The 4th Global Symposium on Millimeter Waves GSMM2011, May 23-25, 2011, Espoo, Finland.

[13] A. Enayati, S. Brebels, G.A.E. Vandenbosch, W. Deraedt, and A.V. Räisänen, “Antenna-in-package solution for 3D integration of millimeterwave systems using a thin-film MCM technology,” in IEEE MTT-S Microw. Symp. Dig., Baltimore, Maryland, USA, June 5-10, 2011, 4 p.

[14] K. Dahlberg, T. Kiuru, J. Mallat, A.V. Räisänen, and T. Närhi “Generic jig for testing mixing performance of millimeter wave Schottky diodes,” in Proc. of the 41st European Microwave Conference, European Microwave Week 2011, Manchester, Oct. 10 – 14, 2011, pp. 922-925.

[15] T. Zvolensky, D. Chicherin, A. Räisänen, C. Simovski, H. Hakojärvi, M. Sterner, and J. Oberhammer, “Leaky-wave antenna at 77 GHz,” in Proc. of the 41st European Microwave Conference, European Microwave Week 2011, Manchester, Oct. 10 – 14, 2011, pp. 1039-1042.

[16] Z. Du, D. Chicherin, and A.V. Räisänen, “Millimeter wave beam steering with a MEMS-based high impedance surface,” in Proc. of the 41st European Microwave Conference, European Microwave Week 2011, Manchester, Oct. 10 – 14, 2011, pp. 1043-1046.

[17] A. Enayati, W. Deraedt, G.A.E. Vandenbosch, and A.V. Räisänen, “Antenna-in-package solution for millimeter-wave applications implemented in a microwave-compatible multilayer PCB technology,” in Proc. of the 41st European Microwave Conference, European Microwave Week 2011, Manchester, Oct. 10 – 14, 2011, pp. 1061-1064.

[18] T. Kiuru, K. Dahlberg, J. Mallat, A.V. Räisänen, and T. Närhi, “Comparison of low-frequency and microwave frequency capacitance determination techniques for mm-wave

Page 44: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

44

Schottky diodes,” in Proc. of the 6th European Microwave Integrated Circuits Conference, European Microwave Week 2011, Manchester, Oct. 10 – 14, 2011, pp. 53-56.

[19] T. Kiuru, J. Mallat, A.V. Räisänen, and T. Närhi, “Compact broadband MMIC Schottky frequency tripler for 75 - 140 GHz,” in Proc. of the 6th European Microwave Integrated Circuits Conference, European Microwave Week 2011, Manchester, Oct. 10 – 14, 2011, pp. 108-111.

[20] A. Enayati, W. Deraedt, G.A.E. Vandenbosch, and A.V. Räisänen, “Antenna-in-package solution for millimeter-wave applications implemented in a microwave-compatible multilayer PCB technology,” in Proc. of the 6th European Microwave Integrated Circuits Conference, European Microwave Week 2011, Manchester, Oct. 10 – 14, 2011, pp. 600- 603.

[21] A. Luukanen, J. Ala-Laurinaho, D. Gomes Martins, J. Häkli, P. Koivisto, P. Pursula, P. Rantakari, J. Säily, A. Tamminen, R. Tuovinen, and M. Sipilä, “Rapid beamsteering reflectarrays for mm-wave and submm-wave imaging radars,” in Passive Millimeter-Wave Imaging Technology XIV (D. A. Wikner and A. R. Luukanen, eds.), Orlando, Florida, USA, SPIE, April 25-29, 2011.

[22] P. Alitalo, C. A. Valagiannopoulos, and S. A. Tretyakov, “Simple cloak for antenna blockage reduction,” in IEEE International Symposium on Antennas and Propagation and USNC/URSI National Radio Science Meeting (AP-S/URSI 2011), Spokane, USA, 3-8 July, 2011.

[23] P. Alitalo, C. A. Valagiannopoulos, and S. A. Tretyakov, “Low-reflection millimeter-wave composite lens,” in Proc. of the Millimetre Wave Days: The 6th ESA Workshop on Millimetre-Wave Technology and Applications, and The 4th Global Symposium on Millimeter Waves GSMM2011, May 23-25, 2011, Espoo, Finland.

[24] P. Alitalo, J. Vehmas, and S. A. Tretyakov, “Reduction of antenna blockage with a transmission-line cloak,” in 5th European Conference on Antennas and Propagation (EuCAP 2011), Rome, Italy, Apr. 11-15, 2011, pp. 2399-2402.

[25] A. O. Karilainen, P. Alitalo, and S. A. Tretyakov, “Chiral antenna element as a low backscattering sensor,” in 5th European Conference on Antennas and Propagation (EuCAP 2011), Rome, Italy, Apr. 11-15, 2011, pp. 1983-1986.

[26] C. A. Valagiannopoulos, P. Alitalo, and S. A. Tretyakov, “Analytical model for coupling of waves between a homogeneous medium and a volumetric transmission-line network,” in IEEE International Symposium on Antennas and Propagation and USNC/URSI National Radio Science Meeting (APS/ URSI 2011), Spokane, USA, July 3-8, 2011.

[27] J. Vehmas, P. Alitalo, and S. A. Tretyakov, “Cloaking performance of a transmission-line cloak in free space and in the near field of a horn antenna,” in Metamaterials 2011: The Fifth International Congress on Advanced Electromagnetic Materials in Microwaves and Optics, Barcelona, Spain, Oct. 10-13, 2011.

[28] L. Bergamin and S. Tretyakov, “Non-linear transformation optics,” in Metamaterials 2011: The Fifth International Congress on Advanced Electromagnetic Materials in Microwaves and Optics, Barcelona, Spain, Oct. 10-13, 2011, pp. 275-277.

[29] A. Bin Abdullah Al-Hadi, M. Costa, V. Koivunen, and P. Vainikainen, “Ambiguity analysis of isolation-based multi-antenna structures on mobile terminal,” in 5th European Conference on Antennas and Propagation (EuCAP 2011), Rome, Italy, Apr. 11-15, 2011, pp. 576-580.

[30] A. Bin Abdullah Al-Hadi, K. Haneda, and P. Vainikainen, “Site-specific evaluation of a MIMO channel capacity for multi-antenna mobile terminals in proximity to a human hand,” in 5th European Conference on Antennas and Propagation (EuCAP 2011), Rome, Italy, Apr. 11-15, 2011, pp. 562-566.

[31] J. Ilvonen, O. Kivekäs, A. Bin Abdullah Al-Hadi, R. Valkonen, J. Holopainen, and P. Vainikainen, “Isolation improvement method for mobile terminal antennas at lower UHF band,”

Page 45: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

45

in 5th European Conference on Antennas and Propagation (EuCAP 2011), Rome, Italy, Apr. 11-15, 2011, pp. 1307-1311.

[32] D. Titz, M. Kyrö, F. Ferrero, S. Ranvier, C. Luxey, P. Brachat, G. Jacquemod, and P. Vainikainen, “Measurement setup and associated calibration methodology for 3d radiation pattern of probe-fed millimeterwave antennas,” in IEEE Loughborough Antennas and Propagation Conference (LAPC), Loughborough, UK, Nov. 14-15, 2011, 5 p.

[33] F. Costa, O. Luukkonen, C. Simovski, A. Monorchio, S. Tretyakov, and P. de Maagt, “Accuracy of homogenization models for finite high-impedance surfaces located in the proximity of a horizontal dipole,” in Metamaterials 2011: The Fifth International Congress on Advanced Electromagnetic Materials in Microwaves and Optics, Barcelona, Spain, Oct. 10-13, 2011, pp. 143-145.

[34] M. Dashti, A. Khatun, T. Laitinen, K. Haneda, J.-i. Takada, and P. Vainikainen, “Impact of antenna pattern on UWB time-based ranging,” in 5th European Conference on Antennas and Propagation (EuCAP 2011), Rome, Italy, Apr. 11-15, 2011, pp. 2812-2816.

[35] P. Vainikainen, E. Vitucci, V. Degli-Esposti, T. Laitinen, V.-M. Kolmonen, and J. Poutanen, “Use of realistic propagation channel information in MIMO antenna system evaluation,” in 5th European Conference on Antennas and Propagation (EuCAP 2011), Rome, Italy, Apr. 11-15, 2011, pp. 2712-2715.

[36] I. Fedosov, I. Nefedov, B. Khlebtsov, and V. Tuchin, “Measurements of laser induced temperature fields in gold colloids using light microscopy,” in Proceedings of III International Symposium Topical Problems of Biophotonics, IAP RAS, N.Novgorod. 2011 – 363, St.Petersburg – N.Novgorod, July 16-22, 2011, p. 140.

[37] V. Grimalsky, I. Nefedov, and Y. Rapoport, “2D electron dynamics in single layer graphene metamaterial,” American Institute of Physics (AIP), Bad Honnef, October 26-28, 2011, pp. 138-140.

[38] C. Gustafson, F. Tufvesson, S. Wyne, K. Haneda, and A. F. Molisch, “Directional analysis of measured 60 GHz indoor radio channels using SAGE,” in 2011 IEEE Vehicular Technology Conference (VTC2011- Spring), Budapest, Hungary, May 15-18, 2011, 3 p.

[39] K. Haneda, J. Poutanen, V.-M. Kolmonen, L. Liu, F. Tufvesson, P. Vainikainen, and C. Oestges, “Validation of the COST2100 channel model in indoor environments,” in NEWCOM++ / COST 2100 Joint Workshop on Wireless Communications, Paris, France, March 1-2, 2011.

[40] K. Haneda, A. Richter, and P. Vainikainen, “Experimental identification of an image source distribution on an indoor map,” in 5th European Conference on Antennas and Propagation (EuCAP 2011), Rome, Italy, Apr. 11-15, 2011, p. 17.

[41] K. Haneda, F. Tufvesson, S. Wyne, M. Arlelid, and A. F. Molisch, “Feasibility study of mm-wave impulse radio using measured radio channels,” in 2011 IEEE Vehicular Technology Conference (VTC2011- Spring), Budapest, Hungary, May 15-18, 2011, 3 p.

[42] J. Poutanen, L. Liu, K. Haneda, and T.-F. V. P. Oestges, Claude, “Parameterization of the COST 2100 MIMO channel model in indoor scenarios,” in 5th European Conference on Antennas and Propagation (EuCAP 2011), Rome, Italy, Apr. 11-15, 2011, p. 06-2.

[43] S. Pivnenko, J. M. Nielsen, O. Breinbjerg, T. Laitinen, and T. B. Hansen, “Comparison of two high-order probe correction techniques for spherical near-field antenna measurements,” in 33rd ESA Antenna Workshop, Noordwijk, The Netherlands, October 18-21, 2011.

[44] R. Valkonen, J. Ilvonen, K. Rasilainen, J. Holopainen, C. Icheln, and P. Vainikainen, “Avoiding the interaction between hand and capacitive coupling element based mobile terminal antenna,” in Proc. of the 5th European Conference on Antennas and Propagation, Rome, Italy, Apr. 11-15, 2011, pp. 2781-2785.

Page 46: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

46

[45] A. Vinogradov, A. Ignatov, A. Merzlikin, S. Tretyakov, and C. Simovski, “Additional effective medium parameters for composite materials (excess surface currents),” in Days on Diffraction 2011, St. Petersburg, Russia, 30 May - 3 June, 2011, pp. 181-182.

[46] A. O. Karilainen and S. A. Tretyakov, “Zero-backscattering self-dual object from two chiral particles,” in Metamaterials 2011: The Fifth International Congress on Advanced Electromagnetic Materials in Microwaves and Optics, Barcelona, Spain, Oct. 10-13, 2011, pp. 405-407.

[47] A. Khatun, T. Laitinen, and P. Vainikainen, “Cubical surface scanning for near-field antenna measurements using spherical wave expansion,” in Antenna Measurement Techniques Association, Denver, CO, USA, Oct. 16-21, 2011, p. 11-0107.

[48] M. Kyrö, D. Titz, V.-M. Kolmonen, S. Ranvier, P. Pons, C. Luxey, and P. Vainikainen, “5 x 1 linear antenna array for 60 GHz beam steering applications,” in 5th European Conference on Antennas and Propagation (EuCAP 2011), Rome, Italy, Apr. 11-15, 2011, pp. 1327-1331.

[49] T. Laitinen, S. Pivnenko, J. Nielsen, and O. Breinbjerg, “On the sensitivity of probe-corrected spherical near-field antenna measurements with highorder probes using double phi-step theta-scanning scheme against various measurement uncertainties,” in 5th European Conference on Antennas and Propagation (EuCAP 2011), Rome, Italy, Apr. 11-15, 2011, pp. 1933-1937.

[50] T. Laitinen and S. Pivnenko, “Separation of radiation from two sources from their known radiated sum field,” in XXX URSI General Assembly and Scientific Symposium of International Union of Radio Science, Istanbul, Turkey, Aug. 13-20, 2011.

[51] T. Laitinen and S. Pivnenko, “On the truncation of the azimuthal mode spectrum of high-order probes in probe-corrected spherical near-field antenna measurements,” in Antenna Measurement Techniques Association, Denver, CO, USA, October 16-21, 2011, p. 11-0105.

[52] T. Laitinen, J. Toivanen, and P. Vainikainen, “Toward accurate antenna measurements using multi-probe systems,” in XXX URSI General Assembly and Scientific Symposium of International Union of Radio Science, Istanbul, Turkey, Aug. 13-20, 2011.

[53] M. Olkkonen, T. Laitinen, and P. Vainikainen, “Non-destructive RF moisture measurement of a bio material web,” in 9th International Conference on Electromagnetic Wave Interaction with Water and Moist Substances (ISEMA 2011), Kansas City, USA, May 31 - June 3, 2011, pp. 30-36.

[54] S. Pivnenko, J. M. Nielsen, O. Breinbjerg, T. Laitinen, and T. B. Hansen, “Comparison of two high-order probe correction techniques for spherical near-field antenna measurements,” in 33rd ESA Antenna Workshop, Noordwijk, The Netherlands, October 18-21, 2011.

[55] C. Schmidt, T. Laitinen, and T. Eibert, “Hybrid fast Fourier transform-plane wave based near-field far-field transformation for “body of revolution” antenna measurement grids: the cylindrical case,” in IEEE International Symposium on Antennas and Propagation and USNC/URSI National Radio Science Meeting (AP-S/URSI 2011), Spokane, USA, 3-8 July, 2011, pp. 1628-1631.

[56] V. Semkin and T. Laitinen, “Ultra wideband antenna for the near-field multi-probe system of scanning,” in The 5th International Conference on Electromagnetic Near-field Characterization and Imaging (ICONIC), Rouen, France, November 30 - December 2, 2011.

[57] O. Luukkonen, S. Maslovski, and S. Tretyakov, “An approach to finding the correct branch from the forest of possible solutions for extracted effective material parameters (invited),” in XXX URSI General Assembly and Scientific Symposium of International Union of Radio Science, Istanbul, Turkey, Aug. 13-20, 2011, p. 5.

[58] C. Simovski and O. Luukkonen, “Edge waves and their use for the broadband field concentration,” in Days on Diffraction, St. Petersburg, Russia, 30 May - 3 June, 2011, pp. 168-169.

Page 47: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

47

[59] C. Simovski and O. Luukkonen, “Metamaterials for efficient and broadband transition from wave beams to evanescent packages,” in Metamaterials 2011: The Fift International Congress on Advanced Electromagnetic Materials in Microwaves and Optics, Barcelona, Spain, October 10-13, 2011, pp. 874-876.

[60] S. Tretyakov, S. Maslovski, and O. Luukkonen, “On retrieval of electromagnetic parameters of complex optical materials from reflection and transmission measurements (invited),” in 10th Mediterranean Workshop and Topical Meeting “Novel Optical Materials and Applications”, Cetraro, Italy, 5-11 June, 2011.

[61] S. Maslovski, Y. Rapoport, and S. Tretyakov, “Perfect lensing with phaseconjugating surfaces: approaching practical realization (invited),” in Days on Diffraction 2011, St. Petersburg, Russia, 30 May - 3 June, 2011, pp. 143-144.

[62] S. Maslovski, Y. Rapoport, and S. Tretyakov, “Perfect lens based on ideal phase conjugating surfaces (invited keynote talk),” in Metamaterials 2011: The Fifth International Congress on Advanced Electromagnetic Materials in Microwaves and Optics, Barcelona, Spain, October 10-13, 2011, pp. 627- 629.

[63] D. Morits and C. Simovski, “Negative effective permeability at optical frequencies produced by clusters of plasmonic particles,” in Days of Diffraction, St. Petersburg, Russia, 30 May - 3 June, 2011, pp. 145-146.

[64] D. Morits and C. Simovski, “Thin-film solar cell enhanced by broadband plasmonic nanoantennas,” in Metamaterials 2011: The Fifth International Congress on Advanced Electromagnetic Materials in Microwaves and Optics, Barcelona, Spain, October 10-13, 2011, pp. 519-521.

[65] D. Morits and C. Simovski, “On electromagnetic characterization of nanoclustered metamaterials,” in The 3rd International Topical Meeting on Nanophotonics and Metamaterials (Nanometa 2011), Seefeld, Austria, Jan. 3-6, 2011, p. 9.

[66] C. Simovski and D. Morits, “On plasmonic light-trapping for tandem thinfilm solar cells,” in International Conference on Electrodynamics of Complex Materials for Advanced Technologies, PLASMETA'11, Samarkand, Uzbekistan, Sept. 21-27, 2011, pp. 52-53.

[67] I. Nefedov and Y. Rapoport, “Stop light and electrical control of the carbon nanotube-graphene structure,” in Metamaterials 2011: The Fifth International Congress on Advanced Electromagnetic Materials in Microwaves and Optics, Barcelona, Spain, Oct. 10-13, 2011, pp. 766- 768.

[68] I. Nefedov and C. Simovski, “Giant enhancement of the thermal radiation heat transfer through the gap between two bodies, carried by hyperbolic media,” in Next Generation Solar Energy From Fundamentals to Applications, Erlangen, Germany, December 12-14, 2011.

[69] I. Nefedov and C. Simovski, “Radiative heat transfer assisted by carbon nanotubes,” in Metamaterials 2011: The Fifth International Congress on Advanced Electromagnetic Materials in Microwaves and Optics, Barcelona, Spain, October 10-13, 2011, pp. 1012-1014.

[70] I. Nefedov, S. Tretyakov, and C. Simovski, “Arrays of carbon nanotubes as ideal backward wave terahertz metamaterials,” in Europhysics Conf. Abstracts, Vol. 35 A, Seefeld, Tirol, Austria, EPS, 3 - 6 January, 2011, p. mon2o.2.pdf.

[71] I. Nefedov and S. Tretyakov, “Effective medium model for a periodic array of metallic carbon nanotubes and eigenwaves propagating in a finitethickness carbon nanotube slab,” in Physics, Chemistry and Applications of Nanostructures (V. E. Borisenko, S. V. Gaponenko, V. S. Gurin, and C. H. Kam, eds.), Singapore, World Scientific Publishing, 2011, pp. 267-269.

[72] I. Nefedov and S. Tretyakov, “Backward waves in arrays of aligned carbon nanotubes,” in Optics Days Book of abstracts (A. Popov, A. Bykov, J. Lauri, and M. Kauppinen, eds.), Tampere, University of Oulu, Finland, May 12-13, 2011, p. 42.

[73] I. Nefedov, “Effects of electromagnetic interaction in periodic arrays of single-wall metallic carbon nanotubes,” in 14th Int. Workshop on New Approaches to High-Tech: Nano-Design,

Page 48: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

48

Espoo, Finland, Aalto University, School of Science, Dept. of Applied Physics, August 22-26, 2011, p. 29.

[74] I. Nefedov, “Eigenwaves propagating in finite-thickness slabs of aligned metallic carbon nanostructures,” in 5-th Finnish-Russian Photonics and Laser Symposium Technical Digest, Saint-Petersburg, Russia, October 18- 20, 2011, pp. 33-34.

[75] I. Nefedov, “Electromagnetic wave properties of carbon nanotube films in the mid infrared range,” in Days on Diffraction 2011, St. Petersburg, Russia, 30 May - 3 June, 2011, pp. 147-148.

[76] S. Tretyakov, I. Nefedov, and C. Simovski, “Towards optimized metamaterial performance: Choosing the optimal geometry and the best raw material” in ICMAT 2011, Singapore, 26 June - 1 July 2011, p. 18.

[77] C. Valagiannopoulos and C. Simovski, “Conversion of evanescent waves into propagating modes by passing through a metamaterial prism: an iterative approximation method,” in 5th European Conference on Antennas and Propagation (EuCAP 2011), Rome, Italy, Apr. 11-15, 2011.

[78] C. Valagiannopoulos, “On adjusting the characteristics of a low-index slab antenna with a finite set of metallic pins,” in 5th European Conference on Antennas and Propagation (EuCAP 2011), Rome, Italy, Apr. 11-15, 2011.

[79] N. Kashyap, S. Werner, and Y.-H. Huang,“Event-triggered multi-area state estimation in power systems,” The Fourth International Workshop on Computational Advances in Multi-Sensor Adaptive Processing (CAMSAP), San Juan, Puerto Rico, Dec. 2011.

[80] P. Mathecken, T. Riihonen, S.Werner, and R.Wichman,“Accurate characterization and compensation of phase noise in OFDM receiver,” 45th Annual Asilomar Conference on Signals, Systems, and Computers (ACSSC), Pacific Grove, California, Nov. 2011.

[81] T. Riihonen, S. Werner, and R. Wichman, “Transmit power optimization for multiantenna decode-and-forward relays with loopback self-interference from full-duplex operation,” 45th Annual Asilomar Conference on Signals, Systems, and Computers (ACSSC), Pacific Grove, California, Nov. 2011.

[82] F. Vitiello, T. Riihonen, J. Hämäläinen, and S. Redana, “On buffering at the relay node in LTE-Advanced,” Proc. IEEE 74th Vehicular Technology Conference (VTC-Fall), San Francisco, California, Sept. 2011.

[83] M. Cierny, C. Ribeiro, R. Wichman, and O. Tirkkonen, “Inter-cell interference management in OFDMA TDD downlink using sounding/silencing protocol,” IEEE International Symposium on Personal, Indoor and Mobile Radio Communications (PIMRC), Toronto, Canada, Sept. 2011.

[84] B. Raaf, W. Zirwas, K.-J. Friederichs, E. Tiirola, M. Laitila, P. Marsch, and R. Wichman, “Vision for beyond 4G broadband radio systems,” IEEE International Symposium on Personal, Indoor and Mobile Radio Communications (PIMRC), Toronto, Canada, Sept. 2011, invited paper.

[85] K. Schober, R. Wichman, and T. Koivisto, “MIMO adaptive codebook for closely spaced antenna arrays,” European Signal Processing Conference (EUSIPCO), Barcelona, Spain, Aug. 2011.

[86] G. González, F. Gregorio, J. Cousseau, S. Werner, and R. Wichman, “Cyclostationary autocorrelation based CFO estimators,” European Signal Processing Conference (EUSIPCO), Barcelona, Spain, Aug. 2011.

[87] F. Gregorio, J. Cousseau, S. Werner, T. Riihonen, and R. Wichman, “Compensation of IQ imbalance and transmitter nonlinearities in broadband MIMO-OFDM,” IEEE International Symposium on Circuits and Systems ISCAS, Rio de Janeiro, Brazil, May 2011.

Page 49: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

49

[88] K. Schober, H.-L. Määttänen, O. Tirkkonen, and R. Wichman, “Normalized covariance matrix quantization for MIMO broadcast systems,” European Wireless, Vienna, Austria, April 2011.

[89] M. Cierny, C. Ribeiro, R. Wichman, and O. Tirkkonen, “SINR prediction versus reverse reporting for soft reuse and interference management,” European Wireless, Vienna, Austria, April 2011.

[90] M. Cierny, P. Jänis, R. Wichman, and C. Ribeiro, “Exclusion regions via handshaking protocol for inter-cell interference management,” Conference on Information Sciences and Systems (CISS), Baltimore Maryland, USA, March 2011.

[91] T. Riihonen, A. Balakrishnan, K. Haneda, S. Wyne, S. Werner, and R. Wichman, “Optimal eigenbeamforming for suppressing self-interference in full-duplex MIMO relays,” Conference on Information Sciences and Systems (CISS), Baltimore, Maryland, USA, March 2011.

[92] J. F. Schmidt, J. E. Cousseau, R. Wichman, and S. Werner, “Prediction based resource allocation in OFDMA,” Conference on Information Sciences and Systems (CISS), Baltimore, Maryland, USA, March 2011.

[93] M. Kaltiokallio, V. Saari, S. Kallioinen, A. Parssinen, and J. Ryynanen, “Wideband 2 to 6GHz RF front-end with blocker filtering,” in Proceedings of 37th European Solid-State Circuits Conference (ESSCIRC2011), Helsinki, Finland, 12-16 Sept. 2011, pp. 539-542.

[94] S. Kallioinen, M. Vääräkangas, P. Hui, J. Ollikainen, I. Teikari, A. Pärssinen, V. Turunen, M. Kosunen, and J. Ryynänen , ”Multi-mode, multi-band spectrum sensor for cognitive radios embedded to a mobile phone,” in Proc. Int. Conf. Cognitive Radio Oriented Wireless Networks and Communications, Osaka, Japan, June 2011, pp. 236-240.

[95] M. Vääräkangas, S. Kallioinen, A. Pärssinen, V. Turunen, and J. Ryynänen, “Trade-offs in primary detection using a mobile phone as a sensing device,” in Proc. Int. Conf. Cognitive Radio Oriented Wireless Networks and Communications, Osaka, Japan, Jun. 2011, pp. 241-245.

[96] S. Kiminki, V. Saari, A. Pärssinen, V. Hirvisalo, A. Immonen, J. Ryynänen, and T. Zetterman, “Design and performance trade-offs in parallelized RF SDR architecture,” in Proc. Int. Conf. Cognitive Radio Oriented Wireless Networks and Communications, Osaka, Japan, June 2011, pp. 156-160.

[97] M. Kaltiokallio and J. Ryynänen, “A 1 to 5GHz adjustable active polyphase filter for LO quadrature generation,” IEEE Radio Frequency Integrated Circuits Symposium (RFIC), Baltimore, USA, June 2011, 4 p.

[98] K. Stadius, M. Kaltiokallio, J. Ollikainen, T. Pärnänen, V. Saari, and J. Ryynänen, “A 0.7-2.6 GHz high-linearity RF front-end for cognitive radio spectrum sensing,” 2011 IEEE International Symposium on Circuits and Systems, Brazil, 15-18 May 2011, pp. 2181-2184.

[99] T. Rapinoja, L. Xu, K. Stadius, and J. Ryynänen, “Implementation of all-digital wideband RF frequency synthesizers in 65-nm CMOS technology,” IEEE International Symposium on Circuits and Systems, Brazil, 15-18 May 2011, pp. 1948–1951.

[100] M. Varonen, M. Kärkkäinen, D. Sandström, and K. Halonen, “A 100-GHz balanced FET frequency doubler in 65-nm CMOS,” 6th European Microwave Integrated Circuits Conference, Manchester, UK, October 2011, pp. 105-107.

[101] M. Yücetas, L. Aaltonen, M. Pulkkinen, J. Salomaa, A. Kalanti, and K. Halonen, ”A charge balancing accelerometer interface with electrostatic damping,” European Solid-State Circuits Conference, Helsinki, Finland, September 2011, pp. 291-294.

[102] R. Jayaprakash, J. Eriksson, and V. Koivunen, “Cooperative game theory and auctioning for spectrum allocation in cognitive radios,” 22nd IEEE International Symposium on Personal Indoor and Mobile Radio Communications, Toronto (PIMRC), Canada, Sep. 2011.

[103] T. Aittomäki and V. Koivunen, “Resource allocation for target detection in distributed MIMO radars,” in Asilomar Conference on Signals, Systems and Computers (ACSSC), Nov. 2011.

Page 50: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

50

[104] T. Aittomäki and V. Koivunen, “Widely distributed MIMO radar beamforming for detecting targets with slow RCS Fluctuations,” in IEEE International Conference on Acoustics, Speech and Signal Processing (ICASSP), May 2011, pp. 2792-2795.

[105] K. Pölönen and V. Koivunen, “Reduced complexity space-time coding in single-frequency networks,” in Proc. IEEE Wireless Commun. Netw. Conf. (WCNC), Cancún, Mexico, Mar. 2011, pp. 1523-1528.

[106] J. Lundén, V. Koivunen, S. R. Kulkarni, and H. V. Poor, “Exploiting spatial diversity in multiagent reinforcement learning based spectrum sensing,” in Proc. 4th IEEE Int. Workshop Computational Advances in Multi-Sensor Adaptive Processing (CAMSAP 2011), San Juan, Puerto Rico, Dec. 13-16, 2011, pp. 325-328.

[107] J. Lundén, V. Koivunen, S. R. Kulkarni, and H. V. Poor, “Reinforcement learning based distributed multiagent sensing policy for cognitive radio networks,” in Proc. 5th IEEE Int. Symp. New Frontiers in Dynamic Spectrum Access Networks (DySPAN 2011), Aachen, Germany, May 3-6, 2011, pp. 642-646.

[108] S. Chaudhari, J. Lundén, and V. Koivunen, “BEP walls for cooperative spectrum sensing,” in Proc. 36th IEEE Int. Conf. Acoustics, Speech, and Signal Processing (ICASSP 2011), Prague, Czech Republic, May 22-27, 2011, pp. 2984-2987.

[109] S. Chaudhari, J. Lundén, and V. Koivunen, “Effects of quantization on BEP walls for soft decision based cooperative sensing,” in Proc. 12th IEEE Int. Workshop Signal Processing Advances in Wireless Communications (SPAWC 2011), San Francisco, CA, USA, Jun. 26-29, 2011, pp. 106-110.

[110] S. Chaudhari, J. Lundén, and V. Koivunen, “Performance limitations for cooperative spectrum sensing with reporting channel errors,” in Proc. 22nd IEEE Int. Symp. Personal, Indoor, and Mobile Radio Communications (PIMRC 2011), Toronto, Canada, Sep. 11-14, 2011, pp. 337-342.

[111] P. Jänis, C. Ribeiro, and V. Koivunen, “On the performance of flexible UL-DL switching point in TDD wireless networks,” in The 2nd IEEE GLOBECOM Workshop on Femtocell Networks, Houston USA, 2011, 6 p.

[112] J. Salmi, S. Sangodoyin, and A. F. Molisch, “High resolution parameter estimation for ultra-wideband MIMO radar,” in The 44nd Asilomar Conference on Signals, Systems, and Computers, Pacific Grove, CA, Nov. 7-10, 2010. Published in 2011.

[113] E. Ollila, V. Koivunen, and H. V. Poor, “A robust estimator and detector of circularity of complex signals,” in IEEE Int. Conf. Acoustics, Speech and Signal Processing (ICASSP'11), Prague, Czech republic, May 22-27, 2011, pp. 3620-3623.

[114] A. Oborina, V. Koivunen, and T. Henttonen, “Effective SINR distribution in MIMO OFDM systems,” in Proc. 44th Asilomar Conference on Signals, System and Computers, Nov. 2010, pp. 511-515. Published 2011.

[115] E. Ollila, V. Koivunen, and H. V. Poor, “Complex-valued signal processing - essential models, tools and statistics,” in 2011 Information Theory and Applications Workshop, San Diego, CA, USA, Feb 6-11, 2011.

[116] E. Ollila and H.-J. Kim, “On testing hypothesis of mixing vectors in the ICA model using FastICA,” in IEEE Int. Symp. Biomedical Imaging (ISBI'11), Chicago, USA, Mar. 30 - Apr. 2, 2011, pp. 325 - 328.

[117] K. Nordhausen, P. Ilmonen, A. Mandal, H. Oja, and E. Ollila, “Deflation-based FastICA reloaded,” in 19th European Signal Processing Conference (EUSIPCO'11), Barcelona, Spain, Aug. 29 – Sep. 2, 2011, pp. 1854 - 1858.

[118] K. Nordhausen, E. Ollila, and H. Oja, “On the performance indices of ICA and blind source separation,'” in 12th IEEE Int. Workshop on Signal Processing Advances for Wireless Communications (SPAWC'11), San Fransisco, CA, June 26-29, 2011, pp. 461 - 465.

Page 51: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

51

[119] M. Costa, A. Richter, and V. Koivunen, “Model order selection in sensor mrray mesponse modeling,” in 45th IEEE Asilomar Conference on Signals, Systems, and Computers, Pacific Grove, California, USA, Nov. 2011.

10.3 Published monographs

No monographs published in 2011 10.4 Other scientific publications

[1] D. Chicherin, “Studies on microelectromechanically tuneable high-impedance surface for millimetre wave beam steering,” No. 127/2011 in Aalto University publication series DOCTORAL DISSERTATIONS, Aalto University, Espoo, Finland, 2011.

[2] S. Geng, “Millimeter wave and UWB propagation for high throughput indoor communications,” No. 97/2011 in Aalto University publication series DOCTORAL DISSERTATIONS, Aalto University, Espoo, Finland, 2011.

[3] J. Holopainen, “Compact UHF-band antennas for mobile terminals: Focus on modelling, implementation, and user interaction.,” No. 28/2011 in Aalto University publication series DOCTORAL DISSERTATIONS, Aalto University, Helsinki, 2011.

[4] T. Kiuru, “Characterization, modeling, and design for applications of waveguide impedance tuners and schottky diodes at millimeter wavelengths,” No. 133/2011 in Aalto University Publication Series DOCTORAL DISSERTATIONS, Aalto University, Espoo, Finland, 2011.

[5] J. Poutanen, “Geometry-based radio channel modeling: Propagation analysis and concept development,” No. 37/2011 in Aalto University publication series DOCTORAL DISSERTATIONS, Aalto University, Helsinki, 2011.

[6] V. Saari, “Continuous-time low-pass filters for integrated wideband radio receivers,” No. 23/2011 in Aalto University publication series DOCTORAL DISSERTATIONS, Aalto University, Helsinki, 2011.

[7] A. Räisänen (ed.): SMARAD, Centre of Excellence in Smart Radios and Wireless Research, Activity Report 2008-2010. Aalto University, Department of Radio Science and Engineering, Science+Technology Report no. 31, December 2011, 88 p.

10.5 Text books and other books related to scientific research

[1] A. Räisänen and A. Lehto: Radiotekniikan perusteet (Fundamentals of Radio Engineering, in Finnish). Otatieto, Helsinki, Finland, 13th edition, 2011, 286 p.

10.6 Chapters in books

[1] N. Tsitsas and C. Valagiannopoulos, “Mathematical modeling of spherical microstrip antennas and applications,” in InTech Microstrip Antennas Book, Open source e-book, 2011, 22 p.

[2] K. Nordhausen, H. Oja, and E. Ollila, “Multivariate models and the first four moments,” in Nonparametric Statistics and Mixture Models, Eds. D. Hunter, D. Richards, and J. L. Rosenberger, pp. 267-287, Singapore: World Scientific, 2011.

[3] H. Kokkinen, J. Henriksson, and R. Wichman, “TV White Spaces in Europe,” in R.A. Saeed, S.J. Shellhammer (ed.). "TV White Space Spectrum Technologies: Regulations, Standards and Applications" CRC Press, October 2011.

Page 52: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

52

11. Other scientific activities of SMARAD members University Boards: Kari Halonen Member, Steering group of Aalto School of Electrical Engineering Member, Doctoral Programme Committee of Aalto School of Electrical Engineering Member, Board of Directors of MilliLab Department Head, Department of Micro and Nanosciences Visa Koivunen Vice-leader, SMARAD CoE Jussi Ryynänen Head of Electronics and Electrical Engineering (EST) study programme Vice Chair, EST degree programme committee Member, Aalto Bachelor study renewal committee Antti Räisänen Chairman, Doctoral Programme Committee of Aalto School of Electrical Engineering Member, Steering group of Doctoral Education of Aalto University Member, Steering group of Aalto School of Electrical Engineering Department head, Department of Radio Science and Engineering Leader, SMARAD CoE Chairman, Board of Directors of MilliLab Participation in Organization of Scientific Conferences and Membership in Expert Boards Kari Halonen TPC Member, European Solid-State Circuits Conference TPC Member, IEEE International Solid-State Circuits Conference TPC Chair and member of Organizing Comittee of ESSCIRC 2011 Conference in Helsinki Member, Management Group of NORCHIP Conference Member, Management Group of PRIME workshop Associate Editor, IEEE Journal of Solid-State Circuits Member, Editorial board of Springer International J. of Analog Integrated Circuits and Signal

Processing Visa Koivunen Fellow, IEEE Associate Editor, Signal Processing Associate Editor, IEEE Transactions on Signal Processing Associate Editor, EURASIP Journal of Wireless Communications and Networking IEEE Signal Processing Society, Industrial Liason board Member and industry liason, IEEE Signal Processing for Communications Technical

Committee (SPCOM-TC) Member, IEEE Sensor Array and Multichannel Signal Processing Technical Committee (SAM-

TC)

Page 53: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

53

KTH advisory board, ICT area COST IC902 Cognitive Radios, Finland representative Jussi Ryynänen TPC Member, European Solid-State Circuits Conference ESSCIRC 2011 TPC Member, European Conference on Circuit Theory and Design, ECCTD 2011 Workshop chair ESSCIRC 2011 Antti Räisänen Fellow, IEEE Edmond S. Gillespie Fellow, AMTA Member of the Board of Directors, Member of the General Assembly, European Microwave

Association (EuMA) Chairman of the EuMA Awards Committee Member, Steering Committee of the European School of Antennas Member, Steering Committee, ESF NEWFOCUS Member of the TPC, 5th European Conference on Antennas and Propagation, EuCAP2011

(Rome, Italy, 11-15 April, 2011) Co-Chair of the Steering Committee, 4th Global Symposium on Millimeter Waves, GSMM2011

(Espoo, Finland, May 23–25, 2011) Member of the TPC, 14th European Microwave Week, EuMW2011 (Manchester, UK, 9-14

October, 2011) Member of the TPC, 6th ESA Workshop Workshop on Millimetre-Wave Technology and

Applications (Espoo, Finland, May 23-25, 2011) Member of the TPC, 33rd Annual Antenna Measurement Techniques Association (AMTA)

Symposium (Denver, USA, 16-21 October, 2011) Sergei Tretyakov Fellow, IEEE Fellow, Electromagnetics Academy President, the Virtual Institute for Artificial Electromagnetic Materials and Metamaterials Member, Steering Committee of the European Doctoral Programme on Metamaterials Deputy member, URSI Finnish National Committee General chair, 5th International Congress on Advanced Electromagnetic Materials in

Microwaves and Optics (Barcelona, Spain, October 2011) Member of the TPC, Optics & Optoelectronics Congress on 18-22 April 2011 in Prague Member of the TPC, SPIE Optics + Photonics, Metamaterials: Fundamentals and Applications

IV, 21-25 August 2011, San Diego, California, USA Member of the TPC, 2011 International Conference on Problems of Interaction of Radiation

with Matter, October 26-28, 2011, Gomel, Belarus Member of the TPC, Loughborough Conference on Antennas and Propagation, 14-15 Nov.

2011, UK Member, Expert Advisory Group for Nanosciences, Nanotechnologies, Materials and New

Production Technologies (European Commission, 7th Framework Programme) Risto Wichman Offical Member, URSI Finnish National Committee, Radiocommunication Systems and Signal

Processing

Page 54: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

54

Local liaison office, EURASIP TPC Member IEEE Globecom Steering Group Member, COST IC0803 RF/Microwave Communication Subsystems for

Emerging Wireless Technologies Review Activities Kari Halonen Reviews for IEEE Journal of Solid-State Circuits, IEEE Transactions on Circuits and Systems I

and II, IEEE Transactions on Microwave Theory and Design, Int. Journal of Analog Integrated Circuits and Signal Processing

Reviews for NORCHIP Conference, European Solid State Circuits Conference, IEEE International Solid-State Circuits Conference, IEEE Symposium on Circuits and Systems, European Conference on Circuit Theory and Design, PRIME workshop

Visa Koivunen Reviews for journals: IEEE Transactions on Signal Processing, IEEE Signal Processing

Magazine, IEEE Journal of Selected Areas in Communications, IEEE Transactions on Antennas and Propagation, IEEE Jornal of Selected Topics in Signal Processing

Reviews for conferences IEEE ICASSP, IEEE SPAWC, IEEE SAM, IEEE PIMRC, IEE ICC Jussi Ryynänen Reviews for IEEE Transactions on Circuits and Systems-Part I, IEEE Journal of Solid-State

Circuits, Integration, the VLSI Journal, IEEE European Solid State Circuits Conference, and IEEE International Symposium on Circuits and Systems ISCAS 2011

Review for research proposal, NWO, The Netherlands Organisation for Scientific Research Antti Räisänen Editorial Board Member, Experimental Astronomy Evaluation for ERC Evaluations for IEEE Fellow Committee, USA Evaluations for ESF Research Networking Programme Evaluation for Agence Nationale de la Recherche, France Evaluation for a faculty position in Information and Communication Technology: Chalmers

University of Technology, Sweden Reviews for Applied Physics Letters, IEEE Proceedings, IEEE Transactions on Microwave

Theory and Techniques, IEEE Transactions on Antennas and Propagation, IEEE Transactions on Instrumentation and Measurement, IEEE Microwave andWireless Components Letters, IEEE Antennas and Propagation Letters, IEEE Transactions on Electron Devices, IEEE Transactions on Electromagnetic Compatibility, IEEE Transactions on Components, Packaging and Manufacturing Technology, IEEE Transactions on Instrumentation and Measurement, IEEE/ASME Journal of Microelectromechanical Systems, IET Electronics Letters, IET Microwaves, Antennas & Propagation, Progress in Electromagnetics Research, Journal of Electromagnetic Waves and Applications, Int. Journal of Microwave, and Wireless Technologies,

Conference paper reviews: EuCAP2011, EuMW2011, ESA Workshop on Millimetre Wave Technology 2011, GSMM 2011, 33rd AMTA Symposium

Page 55: Centre of Excellence in Smart Radios and Wireless Researchsmarad.aalto.fi/en/publications/smarad_activity_report_2011.pdf · 3 1. Introduction to SMARAD Centre of Excellence in Smart

55

Constantin Simovski Reviews for Nature Materials, Nature Communications, IEEE Trans. on Antennas and

Propagation, IEEE Trans. on Microwave Theory and Technique, IEEE Antennas and Wireless Propagation Letters, Physical Review B, Physical Review E, Physical Review Letters, Journal of Optics (Pure and Applied), Optics Letters, Journal of Applied Physics, Applied Physics Letters, Metamaterials, Optics Express, Optics Communications, Journal of Lightwave Technology. Optics and Spectroscopy

Sergei Tretyakov Editorial Board Member, Progress in Electromagnetics Research, Problems of Physics,

Mathematics, and Technics Reviews for Science, Nature Photonics, Nature Materials, Nature Communications, IEEE

Trans. on Antennas and Propagation, Physical Review, Physical Review Letters, Journal of the Optical Society of America A and B, Optics Letters, Journal of Applied Physics, Metamaterials, Optics Express, Optics Communications, IET Proceedings, New Journal of Physics, etc.

Pertti Vainikainen Reviews for IEEE Transactions on Instrumentation and Measurement, IEEE Transactions on

Antennas and Propagation,, IET Electronics Letters, IEEE Antennas and Wireless Propagation Letters

Risto Wichman Reviews for IEEE Trans. on Vehicular Technology, IEEE Trans. on Signal Processing, IEEE

Communication Letters, Springer Wireless Networks, EURASIP Journal on Wireless Communications and Networking

Evaluation of project proposals for Czech Science Foundation and Austrian Science Foundation