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The 11th Advanced Accelerator Concepts Workshop Stony Brooks, New York, June 21, 2004
Review of Advanced Accelerator Concepts R & D in Japan
with Asian activities
Yoneyoshi KitagawaInstitute of Laser Engineering,
Osaka University
(1) ILE, Osaka Univ.Y. Kitagawa, K. Kondo
LACPW Laser Accelerator
(2)Utsunomiya Univ. �N. Yugami, Nishida
(12) Hiroshima Univ. A. Ogata
(14) Himeji Inst.Tech.��S. Miyamoto
(11) Ehime Univ.���R. Sugaya
Laser cooling
(5) AIST K. Koyama
VxB Acceleration &THz Generation
Photonic Crystal AcceleratorLaser Cooling
HIB source
RF Photocathode
(6) U.Tokyo M.Uesaka
(9) AETJapan/ Tokyo Inst.Tech. Hiraoka and Horioka
(10) JAERI APRTajima, Daido
(15) Kyoto Univ.H.Tanaka
Medical compact Accelerator
Magnetized Plasma Accelerator
LAC Electron & Ion sources
(7) NIRSS. Yamada
Ion Accelerator, Ultrahigh Field Science
(4) KEK Urakawa(13) Spring-8�Nakamura et al.
(3) KEK Nakajima
(8) CRIEPI K. Menoto
(16) Kyoto Univ.A. Noda, Sakabe
Advanced Accelerator Facilities in Japan
Outline of Talk
[1] Activities of Japanese laboratories• Electron and Ion acceleration:
Kitagawa group, Osaka UniversityUesaka group, University of TokyoKoyama group, National Inst. of Advanced Industrial Science andTechnologyNakajima group, Japan Atomic Energy Research Inst. APR
• Ion acceleration:Tajima and Daido group, Japan Atomic Energy Research Inst. APROgata group, Hiroshima UniversityNemoto group, Central Research Inst. of Electric Power Industry
• LAC and THz Generation:Nishida and Yugami group, Utsunomiya University
• RF photo cathode:Miyamoto group, Himeji Inst. of Technology
• Radiology Application:Uesaka, U. Tokyo and Dobashi, National Institute of Radiology
Science[2] Advanced Compact Accelerator Project (NIRS)[3] Asian AAC activities
Electron and Ion acceleration:Y. Kitagawa,Y. Sentoku,
R. Kodama, K. A. Tanaka, T. Norimatsu, Institute of Laser Engineering, Osaka University,
University of Nevada, Rino
Electron Acceleration to 100 MeV in an Ultra-Intense Laser
Illuminated Capillary
Electron Acceleration to 100 MeV in an Ultra-Intense Laser Illuminated Capillary
10 mm
A
B
Electron Spectra from 1.2 mm and 10 mm-long Capillaries
Elec
tron
s/M
eV/s
tr
108
109
1010
1011
1012
1013
1014
1 10 100
Energy [MeV]
10 mm long
1.2 mm
Detection limit
Bump
Field = 10 GV/m
1
10
100
1000
20 40 60 80100M
axim
um E
nerg
y [M
eV]
Capillary diameter D (µm)
200
PIC EXP
Optimum diameter
PRL Vol.92, No.20 (2004)
Laser Wakefield Excitation in Capillary Plasma
Electrostatic waves at 4.6 psecLongitudinal E-field
Transverse E-field
Div
erge
nce
(rad
)
2-D PIC
5 πmm mrad5.9x1016 cm-3
Ionization shift of laser Spectrum
Resonant to 500 fs pulse width! PRL Vol.92, No.20 (2004)
Medical Application of Capillary Accelerator
External (Far field) Illumination
Capillary (Near field)Injection
Beam Species,Emittance and Spectrum are not required
morTumor
Skin surface
����������
Beam Species,Emittance and Spectrum are required
Proton(HIB)
X-ray
Fast neutron
Electrons
Depth
Tumor
Electron and Ion acceleration:
M. Uesaka,T. Hosakai, K. Kinoshita, A. ZihidkovNERL University of Tokyo
Plasma Cathode Experimentto be presented to the
Workshop
0 20 40 60Electron Energy [MeV]
PIC simulation
Experiment
10-2
10-3
10-4
10-5
e-Spectrum
Ref.T.Hosokai,et al.,Phys Rev.E 67,036407 (2003)
T.Hosokai et al., Phys. Plasmas (In press 2004)
Electron acceleration:K. Koyama and E. Miura,
National Institute of Advanced Industrial Science and Technology
Quasi-mono-energetic electron beam at AIST / Tsukubato be presented to the
Workshop
Quasi-monoenergetic electron beam was obtained at AIST / Tsukuba
Quasi-monoenergetic electron beam was obtained at AIST / Tsukuba
AIST
by focusing a 2-TW laser pulse on a dense-gas jet of ne≈1020cm-3.
K.KOYAMA
AIST
Electron Energy Spectrum including quasi-monoenergetic beam
Electron Energy Spectrum including quasi-monoenergetic beam
104
105
106
107
108
0 5 10 15 20 25 30Ele
ctro
n N
umbe
rs (/
MeV
/sr/
shot
)
Electron Energy (MeV)
100
101
102
103
104
600 700 800 900 1000 1100 1200 1300
Inte
nsity
(arb
.uni
t)
Wavelength (nm)
1st-Stokes
Laser Wavelength
Monoenergetic beam was emitted in an narrow divergence angle.
Electron acceleration:K. Nakajima, M. Kando and group
Japan Atomic Energy Research Institute APR
High current electron beam generated
with a short (23fs) laser at a high density regime
to be presented to the Workshop
High current electron beam generatedwith a short (23fs) laser
1.4x1020cm-3
Full powerTeff~2.5 MeV
Teff~7.8 MeV
2.3 x1019 W/cm2 (a0=3.3)
20 TW23 fs
1
2
3
4
5
6
300 320 340 360 380 400 420 440
fc29.out5
Cha
rge
[nC
]
Laser energy [mJ]
Divergence Angle ~ 10deg
Charge ~5 nC/shot
Ion acceleration:Daido, A. Fukumi, K. Matsukado et al.
Japan Atomic Energy Research Institute APR
Ion Generation Experiments @JAERI APR
to be presented to the Workshop
Ion Generation Experiments @JAERI APR
Laser pulse800 nm,50 fs, 200 mJ
Thomsonparabola
CR-39 trackdetectors
0o
θ
Electronspectrometer
Ions
2×1018 W/cm2
Target : Ta 1,3,5 um
Angular distribution of protons
Energy spectra of protons
Prediction of Underdense Plasma Model
6×1018 W/cm2
2×1018 W/cm25×1019 W/cm2
a~5, σ=11~13Emax=10~12 MeVEeff~2 MeVN~108 protons/shot (2 MeV ± 100 keV)
Main pulse
Prepulse
Preformedplasma
Target
Emax (Maximum energy of protons [MeV])χ (Conversion efficiency)
)]m([)]W/cm([1085.0 2/1292 µλI
cmeAae
−×==
λσ cr
L
s ndxn∫= 0
a : Dimensionless amplitude of laser pulse
σ : Normalized density integratedalong the channel axis
xns
ns : Electron densityalong plasmachannel
ncr : Critical densityλ : Laser wavelength
L
Ion acceleration:Ogata group
AdSMAdSM Hiroshima University
Ion production enhancement by rear-focusing and prepulse with foil target.
talk by A. Ogata at High Energy Density Physics and Exotic Acceleration Schemes SUBGROUP
13:25-13:50 Tuesday
In fs-lasers the energies should be scaled byfluence.
Y. Oishi et al., Rev. Laser Engineering,31 (2003) 742.
1017Wcm-2(1TW10µmφ) for 50fs makes only 5x103Jcm-2
out of this figure
0.1
1
10
100
104 105 106 107 108 109
y = 0.00050413 * x^(0.62093) R= 0.90863
Max
Pro
ton
Ener
gy[M
eV]
I λ2t[J cm -2 µm2]
In our experimentT3 laser with a 10-3 prepulse
shift the film target positionfrom the laser waist
energetic ionson both sides
AdSMAdSMHiroshima U.Hiroshima U.
0.1
1
10
100
100 1000 104 105 106 107 108 109
Max
Pro
ton
Ener
gy[M
eV]
I λ2t[J cm -2 µm2]
this work
positioning the target ~1mm before the laser waistunder the existence of prepulses.
50mJ, 50fs, 800nm Ti-sapphire laser. Contrast 10-3.
Ion Acceleration:Nemoto group
Central Research Institute of Electric Power Industry
Energetic particle generation using Ultra-short pulse laser
Energetic particle generation using Ultra-short pulse laser
Laser beam
Tape target ~ µ
Accelerated Proton beam
Proton beam pattern(Half angle)
Energetic Ion acceleration
0
1000
2000
3000
4000
0 50 100 150 200 250 300PET 70um (<100keV)
Al 30um
Cu 5umPolyimido 7.5um
Cu 30um
Polyimido 7.5um
Zr 5um
Cu 5um
Cu 30um
100fs, 1.1e19W/cm270fs, 8.3-8.7e18W/cm2
Max
imum
Pro
ton
Ene
rgy
(keV
)
Terget thickness density
T-cube laser system20TW, 1J, 50fs, 10Hz
Maximum proton energy
Simple iso-thermal plasma expansion model well describes the experimental results
( )2
2max 1ln2
++≈− efpiefpipp ttZUE ωω
Eq.(1)
RF Generation:
N. Yugami, Y.Nishida et al., Utsunomiya University
51 GHz radiations from magnetized short-pulse laser
plasmasto be presented to the
Workshop
Experimental Setup
Observed radiation Pulse
1st Peak
Cut-off freq.fc = 31.4 GHz
B0 = 5.44 kGN2 4.5 Torr Laser power 0.5TW
Pulse width(FWHM)1st Peak 185 ps
Radiology Application:M. Uesaka, A. Fukasawa et al., U. Tokyo
K. Dobashi, NIRS J. Urakawa, KEK
Compact Laser-Compton Hard X-ray source based on X-band linac
Compact Hard X-ray source based on X-band linac
Final target for medical useX-band accelerating structure
X-band Klystron
X-band pow
er supply
Patient
Monochromatic hard X-ray
Moving arm2D X-ray detector
Laser system
Dynamic imageof coronary artery
Moving stage(bed)
<5 m
<3m
Intravenous injection of contrast agent
Lasercirculation
system
1010-1011photons/s
Thermionic cathodeX-band RF-gun(2.6cell)
Compact Hard X-ray source�based on X-band linac (under constructing)
Alpha Magnet
Thermionic cathode X-band RF-gun
X-band Accelerating Structure
X-bandPower Source
Q-Sw
itch N
d:YA
G L
aser
Hard X-ray(33keV)
Q-Magnet
Bending MagnetLaser Dump
Collision Point
Lens
Thin mirror(in vaccume)
TimingSystem
Multi-bunch Electron Beam
Laser light(1064 nm)
Beam Dump
Mirror
Polarized beam splitter
PockelscellX-ray yield:1.7x108photons/s
-500
-400
-300
-200
-100
0
100
-2 0 2 4 6 8
Vk(
kV)
Time(µs)
X-band RF source50MW 50pps
RF photo cathode:Miyamoto group
Himeji Inst. of Technology
Plane and Needle Photocathode
Plane and Needle Photocathode
10µm
(b)
(d)
(c)
Tungsten needle
substrate (tungsten tip)
(a)
introduce
carbon heater
manipulation arm (Molybdenum)
Laser and CCD monitor
LaserInjection
Tuner
RFGunAcc.
Needle Cathode(W)
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Plane Cathode(LaB6)
3mm
Field emission current vs. RF Power
[2] National Institute of Radiological Sciences Project
Advanced and Compact Accelerator
Development PROJECT
PROJECT organization
I. Compact Synchroton for proton and heavy Ion
• Laser ion sourceJAERI APR, U. Tokyo, Hiroshima U.• Beam storage and coolingKyoto U.• Synchrotron ringKEK• FFAG acceleratorNIRS
II. Compact hard X-ray radiation source
• Intense and short pulse radiation source:Laser electron source
U. Tokyo, Osaka U., AIST• X-band electron beam linacU. Tokyo• High flux radiation sourceKEK
[3] Asian AAC activities
to be presented by Kazuhisa Nakajima, KEK
Asian Advanced Accelerator Community
is organized at APAC2004
Asian Advanced Accelerator Community
is organized at APAC2004
The largest number of labs are involved in Advanced Accelerator R&D in Asia.
JapanKoreaChinaTaiwanIndiaIsraelUkraine
Chair: Kazuhisa NAKAJIMA
Acknowledgment
We acknowledge the organizing committee, Japanese community member and all the the workshop participants for the given chance of presentation.
Thank you very much for listening to my talk.