coherent radiation from high-current electron beams of a linear accelerator and its applications
DESCRIPTION
Coherent Radiation from High-Current Electron Beams of a Linear Accelerator and Its Applications. S. Okuda 1987-2002 ISIR, Osaka Univ. 2002- Research Institute for Advanced Science and Technology (RIAST), Osaka Prefecture Univ. Coworkers: - PowerPoint PPT PresentationTRANSCRIPT
Coherent Radiation from High-Current
Electron Beams of a Linear Accelerator
and Its Applications
S. Okuda
1987-2002 ISIR, Osaka Univ. 2002- Research Institute for Advanced Science and Technology (RIAST), Osaka Prefecture Univ. Coworkers: Osaka Pref. Univ. R. Taniguchi, T. Kojima Osaka Univ. M. Nakamura, M. Takanaka, R. Kato Kyoto Univ. T. Takahashi Kangwon Univ. S. Nam
High-current electron linear accelerator (linac)
High-current thermionic gun
3 SHBs
Coherent radiation from electron beams
Free-electron lasers
Coherent radiation with a broad spectrum
Applications of the radiation
Electron bunch shape monitor
Absorption spectroscopy
38 MeV L-band linac at Osaka Univ.
Single-bunch electron beam parameters
Repetition rate 120 pps
Energy 27 (38 max.) MeV
Energy spread 1-2.5% FWHM
Maximum Charge 91 nC/bunch
Micropulse length 20-30 ps
Normal. rms emittance 70-200 mm mrad
High-current thermionicelectron gun
Osaka Argonne X-ray SASE (2002) (2002)
Gun, Injector thermionic photocathode photocathode
SHPBs rf (half cell)
rf frequency (MHz) 1300 1300
Repetition rate (pps) 120
Energy (MeV) 27 (38 max.) 14
Energy spread (% FWHM) 1-2.5
Charge (nC/bunch) 91 100 a few
Micropulse length (ps) 20-30 15-40 10
Normalized rms emittance
(mm mrad) 70-200 1700 2
Estimated
Measured
High-current and high-brightness beams
Operational modes of the linac
Density modulation and coherent radiation
Free-electron lasers (FELs)
Features of FELs Tunability Subpicosecond short pulse High peak power (MW)
Single passage (no cavity mirror)High gainX-ray FEL
SASE (Self-amplified spontaneous emission) FEL
First lasing: 1991
Oscillation FEL
Output power of FEL light
Wavelength: 40 mOutput power: 800 J/macropulse
First lasing: 1994
FEL facility at Osaka Univ.
FEL facilities
IR-FIR user facilities
Visible-UV Storage ring FELs
High power IR FELs
Superconducting linacs
X-ray SASE projects
×N (~ 1011)
Coherent radiation from an electron bunch
Phys. Rev. Lett. 1991
Our observation of coherent radiation
High intensity in a submillimeter to millimeter range (THz – 100 GHz)Continuous spectrumCoherencePico-second short pulseSynchronization with the electron bunch
Absorption spectroscopyAnalysis of transient phenomenaImagingCoherent excitationPump and probe analysis
Characteristics of CR
Applications of CR
Applications of the radiation
Electron bunch shape monitor
Far-infrared light source
for absorption spectroscopy
Bunch form factors for various bunch shapes
Gaussian
RectangularIsosceles triangular
Wavelength is normalized by the FWHM bunch length.
Bunch sape monitoring system
Coherenttransition radiation
L-band LINAC
Bunch compressorAl foil
Al Mirror
Interferometer
Detector
Streak camera
Shielding wall
Detector
Electron beam
Cherenkov radiation
Streak measurement Time resolution 0.9 psMeasurement of the coherent transition radiation Wavelength range 0.4-2 mm Wavenumber resolution 0.2 cm-1 Interferometer: Martin-Pupplet type Detector: Liquid-He-cooled Si bolometer
Time resolution 0.9 psInterference filter 478.5 nm (B. W.: 11.3 nm)
Martin-Pupplet interferometer
Beam splitter
Fixed mirror
Detector for measuring interferogram
Detector for monitoring beam intensity
Movablemirror
Coherenttransition radiation
Beam splitter : wire grid with a wire spacing of 25 m
-60 -40 -20 0 20 40 60-10
-8
-6
-4
-2
0
2
4
Sig
nal (
arb.
unit)
Optical path difference (mm)
Bunch compression with a bunch compressor
0 20 40 60 80 100 120
0.0
0.2
0.4
0.6
0.8
1.0
29ps (FWHM)
Nor
mal
ized
In
tens
ity
Time (ps)
0 20 40 60 80 100 120
0.0
0.2
0.4
0.6
0.8
1.0
29ps (FWHM)
Nor
mal
ized
In
tens
ity
Time (ps)0 20 40 60 80 100 120
0.0
0.2
0.4
0.6
0.8
1.0
18ps (FWHM)
Rel
ativ
e In
tens
ity
Time (ps)
0 20 40 60 80 100 120
0.0
0.2
0.4
0.6
0.8
1.0
18ps (FWHM)
Rel
ativ
e In
tens
ity
Time (ps)
4 pole chicane-type bunch compressor
Magnetic field 0.105 T
Deflection angle 0.27 rad
Electron beamElectron beam
Single-bunch beam parameters Energy 27 MeV Energy spread 1.1 % (FWHM) Charge/bunch 13.5 nC
Bunch shapes measured with a streak camera
B.C. on
Spectra of CR and bunch form factors
0 5 10 15 20 25
10-7
10-6
10-5
10-4
Lon
gitu
din
al F
orm
Fac
tor
Wavenumber (cm-1)
Coherent radiationTriangular bunch (29ps)
0 5 10 15 20 25
10-7
10-6
10-5
10-4
Lon
gitu
din
al F
orm
Fac
tor
Wavenumber (cm-1)
0 5 10 15 20 25
10-7
10-6
10-5
10-4
Lon
gitu
din
al F
orm
Fac
tor
Wavenumber (cm-1)
Coherent radiationTriangular bunch (29ps)Coherent radiationTriangular bunch (29ps)
0 5 10 15 20 25
10-7
10-6
10-5
10-4
Lon
gitu
din
al f
orm
fac
tor
Wavenumber (cm-1)
Coherent radiationTriangular bunch (18ps)
0 5 10 15 20 25
10-7
10-6
10-5
10-4
Lon
gitu
din
al f
orm
fac
tor
Wavenumber (cm-1)
0 5 10 15 20 25
10-7
10-6
10-5
10-4
Lon
gitu
din
al f
orm
fac
tor
Wavenumber (cm-1)
Coherent radiationTriangular bunch (18ps)Coherent radiationTriangular bunch (18ps)
Bunch form factor at =1 mm: 10-6 → 10-5
1 10 100
10-13
10-12
10-11
10-10
Inte
nsity
(J/
pul
se/1
%B
.W.)
Wavenumber (cm-1)
BC offBC on
1 10 100
10-13
10-12
10-11
10-10
Inte
nsity
(J/
pul
se/1
%B
.W.)
Wavenumber (cm-1)
BC offBC on
0 5 10 15 20 25
10-7
10-6
10-5
10-4
Lon
gitu
din
al F
orm
Fac
tor
Wavenumber (cm-1)
Coherent radiationTriangular bunch (29ps)
0 5 10 15 20 25
10-7
10-6
10-5
10-4
Lon
gitu
din
al F
orm
Fac
tor
Wavenumber (cm-1)
0 5 10 15 20 25
10-7
10-6
10-5
10-4
Lon
gitu
din
al F
orm
Fac
tor
Wavenumber (cm-1)
Coherent radiationTriangular bunch (29ps)Coherent radiationTriangular bunch (29ps)
Spectra of CR
Bunch form factors
B.C. on
Radiation loss of the single-bunch beam energy
in the bunch compressor
Coherent synchrotron radiation light source
CSR power1 J/%B.W. at 1 mm0.3 mJ at 0.7-1.4 mm (>30 MW peak power)
Beam conditions Energy: 27 MeV Electron charge: 30 nC/bunch Bunch length: 5-10 ps
Submillimeter to millimeter wave
light sources
Peak power (at =1 mm) Averaged power
1 Coherent radiation (100 Hz) 1
10-5 Terahertz radiation source 10-1
(10 MHz)
10-12 Incoherent SR source 10-4 (10 MHz)
10-20 Blackbody source (DC) 10-5
Experimental setup for absorption spectroscopy using CTR
Detector
Detector
Monochromator
Splitter
Shielding wall
Sample
Plane mirror
L-band linac
Transition radiation
Al plate
Quadrupole magnets
Electron beam
Window Concave mirror
Detector
Detector
Monochromator
Splitter
Shielding wall
Sample
Plane mirror
L-band linac
Transition radiation
Al plate
Quadrupole magnets
Electron beam
Window Concave mirror
Absorption spectroscopy for water
Incident LightQuartz
Water
Incident LightQuartz
Water
Temperature: 22 ℃Thickness of the sample: 186 m
(a)
(b)
1.5
2
2.5
3
9 10 11 12 13 14 15
0
50
100
150
200
9 10 11 12 13 14 15
Wavenumber (cm -¹)
Ab
sorp
tion
Co
effi
cie
nt
Re
fra
ctiv
e In
de
x(
Np
cm
-1)
Wavenumber (cm -¹)
(a)
(b)
1.5
2
2.5
3
9 10 11 12 13 14 15
0
50
100
150
200
9 10 11 12 13 14 15
Wavenumber (cm -¹)
Ab
sorp
tion
Co
effi
cie
nt
Re
fra
ctiv
e In
de
x(
Np
cm
-1)
Wavenumber (cm -¹)
Resolution: 1%
Setup for imaging
X-Y Stage
Collimator
Sample
Sample
Collimator (Al plate)
CTR
CTR
X-Y Stage
Collimator
Sample
X-Y Stage
Collimator
Sample
Sample
Collimator (Al plate)
CTR
CTR
MonochromatorDetector
Detector
SampleBeam Splitter
X-Y Stage
Collimator
Oscilloscope X-Y Stage Controller
CTR
MonochromatorDetector
Detector
SampleBeam Splitter
X-Y Stage
Collimator
Oscilloscope X-Y Stage Controller
CTR
Dried
1 cm 1 cm
Dried
1 cm 1 cm
Imaging with CTR
PrintPeak wavenumber : 11.1 cm-1
Wavenumber width: 0.2 cm-
1
Resolution: 0.8 mm
8 mm8 mm
Transmission (%) 0 25 50 75 100
Transmission (%) 0 25 50 75 100
LeafPeak wavenumber : 10.7 cm-1
Wavenumber width: 3.5 cm-
1
Resolution: 0.8 mm
Other application
Summary
High-current electron linac
91 nC/bunch (kA peak current)
Coherent radiation from electron beams
FELs
Coherent radiation
Applications of the coherent radiation
Electron bunch shape monitor
Absorption spectroscopy
Other applications
Research Center for Radiation and RadioisotopesRIAST, Osaka Prefecture Univ. Electron accelerators 18 MeV Linac 600 keV Cockcroft-Walton accelerator Ion accelerators 3 MeV Tandem accelerator Cobalt-60 gamma ray sources 4 x 1015 Bq (105 Ci ) 4 irradiation rooms and a water pool facility Radioisotope facilities
Water pool for 60Co -ray sources
Cherenkov radiation from 60Co -ray sources installed
in a water pool