olivier bourgeois institut néel, cnrs grenoble,...
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Olivier Bourgeois NANOCTM Cargèse october 2012
Olivier Bourgeois
Institut Néel, CNRS
Grenoble, France Graduate students :
Christophe Blanc, Hossein Ftouni, Yanqing Liu
Ph D: Jean-Savin Heron
Postdoc: Dimitri Taïnoff, Kunal Lulla
MC Simulations: N. Mingo, A. Rajabpour, S. Volz
Collaborations: A. Barski, E. Hadji, E. Collin, U.
Gennser, D. Kazazis
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Electron, photon, phonon Less controlled Manipulating phonons Building blocks for thermal logic
(thermal rectification, thermal diodes, etc…)
Reducing phonon thermal transport
Reduction of thermal conductance
Suspended structures (membrane, nanowire, etc…)
ZT coefficient
“Position Paper on Nanophotonics and Nanophononics”, Clivia M Sotomayor
Torres and Jouni Ahopelto E-Nano Newsletter (Issue 24) Publishing Date: 2011-12-31 Olivier Bourgeois NANOCTM Cargèse october 2012
ZT= S2Tσ/k K=ke+kph
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Phonon wave length
Mean free path Roughness
Density of state
Group velocity
Olivier Bourgeois NANOCTM Cargèse october 2012
Tk
hv
B
SDom
82.2
for silicon
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Nanostructured Bulk materials
Ebeam lithography
Focus Ion Beam
J. Tang et al. Nano Letters 10, 4279 (2010) and J.K. Yu et al Nature
Nanotechnology 5, 718 (2010)
Olivier Bourgeois NANOCTM Cargèse october 2012
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Nanoparticles
Embedded in a matrix
superlattice
Grown Nanostructured materials
Better control of the size and roughness
Olivier Bourgeois NANOCTM Cargèse october 2012
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Heat
Transport at
the
nanoscale 1 picoJoule (10-15J)
A. Sikora, H. Ftouni, J. Richard, and O.B.,
Rev. Sci. Instrum. 83, 054902 (2012).
NanoLett 2009, PRB 2010
1 attoJoule (10-18J)
1mm
PRL2005
Rev. Sci. Instrum. 81, 053901 (2010)
Nanowatt
Picowatt
Thermodynamic of Small Systems, Institut Néel
Phononic crystal
Thermoelectrics in GeMn
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Olivier Bourgeois NANOCTM Cargèse october 2012
Blocking ballistic phonons in mono-crystalline silicon
nanowire
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Mean free path Lph
LCas=D (Diameter of
the nanowire)
Boundary scattering:
black body radiation
for phonons
Expression for K(T) rB
Vn’
T2
T1 T2 >>
T1
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At low temperature, the dominant
phonon wave length is increasing:
Probability of specular reflection p(dom)
depending on dom (phenomenological parameter)
p(dom)=0 (perfectly rough surface)
dom<<h0 Casimir model
p(dom)=1 (perfectly smooth surface)
dom>>h0
rB
→ n Vn’
Vn
h0 is the root mean square of
the asperity
Olivier Bourgeois NANOCTM Cargèse october 2012
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Ziman-Casimir model
Casphp
pL
L
1
1 where p probability of specular
reflection
hh
h
dePp dom2
2316
)()(Probability distribution
of asperity
If p=0 transport is diffusive (Casimir), if p=1 ballistic transport
Olivier Bourgeois NANOCTM Cargèse october 2012
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Straight nanowire Nanowire with serpentine
Length 10µm and section 100nm by 200nm
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october 2012
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Low temperature experiments
3w method, heat flux along the nanowire
Low frequency measurement
Sensitive to power less than the picoWatt
V1w
Iac
V3w
D. G. Cahill, Rev. Sci. Instrum. 61, 802 (1990)
L. Lu, W. Yi et D. L. Zhang, Rev. Sci. Instrum. 72, 2996 (2001)
O. B. et al., J. Appl. Phys. 101, 016104 (2007)
J. S. Heron, T. Fournier, N. Mingo and O. B., Nano Lett., 9, 1861 (2009)
J. S. Heron, C. Bera, T. Fournier, N. Mingo and O. B., Phys. Rev. B, 82, 155458
(2010) Olivier Bourgeois NANOCTM Cargèse october 2012
• Iac ~ 1w
• Tac ~ I2 ~ 2w
• R ~ T ~ 2w
• V3w~ IacR ~3w
KNbN<<KSi
w
3
4
23
04
V
RIK
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0 1 2 3 4 5 6
0
20
40
60
80
100
120
140
160
K(p
W/K
)
T(K)
K3
K5
K7
K8
Thermal conductance for 4 identical
samples
O. Bourgeois, Th. Fournier, and J. Chaussy, J. Appl. Phys. 101, 016104 (2007) J-S. Heron et al., Journal of Low Temperature Physics , 154, 150 (2009)
h
TkK B
3
22
0
1 10
0.1
1
K/4
KQ
T(K)
K~T3
K~T2
K~T3
Thermal conductance normalized by 4 quanta of conductance
Temperature dependence of
the thermal conductance
Tk
hv
B
SDom
82.2
Olivier Bourgeois NANOCTM Cargèse october 2012
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0 2 4 6
1
10
Lph(µ
m)
T (K)
0 2 4 60.0
0.2
0.4
0.6
0.8
1.0
p
T(K)
Caseffp
pL
L
1
1 111 LL Leffph
Ziman model of phonon transport
3
3/2
33
423
5
2102.3 T
L
S
v
kK
eff
s
BL
Tk
hv
B
SDom
82.2
Olivier Bourgeois NANOCTM Cargèse
october 2012 J.-S. Heron, T. Fournier, N. Mingo and O. Bourgeois, Nano Letters 9,
1861 (2009).
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1 10
0.1
1
K/4
K0
T(K)
Diffusive transport: classical Casimir
model
Competition between ballistic and diffusive regime: roughness effect
Dominated by the thermal resistance of the wire/reservoir junction (??)
Evidence for the presence of
ballistic phonons
Fitting parameter: •Roughness h4nm
•Speed of sound 9000m/s
•Contribution of the contact
(Chang, C.; Geller, M.
Phys. Rev. B 2005, 71,
125304.)
J.-S. Heron, T. Fournier, N. Mingo and O. Bourgeois, Mesoscopic surface
effects on the phonon transport in silicon nanowire, Nano Letters 9, 1861
(2009).
Olivier Bourgeois NANOCTM Cargèse
october 2012
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Introducing of a serpentine nanostructure in the suspended nanowire (5µm long)
Length scale 200nm Blocking only the ballistic
phonons
Reduce the thermal conductance
Olivier Bourgeois NANOCTM Cargèse october 2012
C. W. Chang, D. Okawa, H. Garcia, A. Majumdar and A. Zettl, Phys. Rev. Lett.
99, 045901 (2007).
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Reduction of up to 40% of
the thermal conductance
Model this system by
transmission function
analysis
Very good agreement
between the model and
the data
Concerning ballistic
phonons the reduction is
of the order of 80%
J-S. Heron, C. Bera, T. Fournier, N. Mingo, and O. Bourgeois,
Blocking phonons via nanoscale geometrical design, Phys Rev
B 82, 155458 (2010)
Olivier Bourgeois NANOCTM Cargèse october 2012
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• Adaptation of the contact between the nanowire (1D)
and the bath (3D)
L. G. C. Rego et G. Kirczenow, Phy. Rev. Lett. 81, 232 (1998)
Y. Chalopin, J.-N. Gillet, S. Volz, Phy. Rev. B 77, 233309 (2008)
1
0.1
1
10
100
K/K
ca
s
T (K)
Straight
C1
C2
C3
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• No effect has been
seen
• No impact of the
thermal resistance
at the interface
• Still below the
universal quantum
of thermal
conductance
Kcas
1
0.1
1
10
100
K/K
ca
s
T (K)
Straight
C1
C2
C3
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Olivier Bourgeois NANOCTM Cargèse october 2012
Reduction of mean free path due to
corrugated surfaces in silicon nanowire
200 nm
10 µm
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Multiple scattering
Backscattering in sawtooth nanowire
Reduction of the mean free path
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Samples made by ebeam lithography
dom=100nm at 1K in silicon very close to the periodicity of the modulation of roughness
Comparison to smooth nanowire
200 nm
10 µm 320 nm d=200 nm
=200nm
d=55 nm
Olivier Bourgeois NANOCTM Cargèse october 2012
Thesis Christophe Blanc
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T
L
S
v
kTK
s
B L
33
423
5
2102.3)(
Casp
pL
L
1
1
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Smooth nanowire have large mean free path
Comparable temperature power law (=2.6)
Mean free path strongly reduced by regular corrugated surfaces
Comparison to smooth nanowire
Olivier Bourgeois NANOCTM Cargèse october 2012
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Presence of
backscattering
Phonon trapped in
the Si teeth
Olivier Bourgeois NANOCTM Cargèse october 2012
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Ali Rajabpour, S. Volz JAP 110, 113529 (2011)
200 nm
10 µm
Olivier Bourgeois NANOCTM Cargèse october 2012
L
L
T
1
1
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• Strong backscattering effect of the corrugation (negative parameter p)
• The corrugation acts like a trap for the phonons • Factor of 10 in the mean free path between smooth
and corrugated wires
Olivier Bourgeois NANOCTM Cargèse october 2012
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Holey silicon nitride (SiN)
Phonon transport in
amorphous SiN
Anderson model in the
Casimir limit ?
New tools for phonon
thermometer
Olivier Bourgeois NANOCTM Cargèse october 2012
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Olivier Bourgeois NANOCTM Cargèse october 2012
K.J. Lulla, M. Defoort, C. Blanc, O. Bourgeois, and E. Collin, Evidence for the crucial role of normal-state electrons in nanoelectromechanical damping mechanisms at very low temperatures, submitted to Physical Review Letters october 2012.
E. Collin, T. Moutonet, J.-S. Heron, O. Bourgeois, Yu. M. Bunkov, and H. Godfrin,, Physical Review B 84, 054108 (2011).
Collaboration with Eddy Collin
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Manipulating phonon: it works !
Strong reduction of mean free path in
corrugated single crystal nanowires
Amorphous materials
Perspectives
Entering in the quantum regime of
thermal transport
2 dimensional electron gas
Olivier Bourgeois NANOCTM Cargèse october 2012
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Thanks to all the members
of the group
Technical pool of Institut
Néel (electronic, Nanofab,
cryogenic facilities)
Collaborations (LITEN, LPN,
Ecole Centrale Paris, INAC,
IC2N (Spain)
Quantherm, QNM
Phononics, COGEETEN
MERGING (FP7, FET)
Olivier Bourgeois NANOCTM Cargèse october 2012