m. hosaka a , m. katoh b , c. szwaj c , h. zen b m. adachi b , s. bielawski c , c. evain c

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M. Hosaka a , M. Katoh b , C. Szwaj c , H. Zen b M. Adachi b , S. Bielawski c , C. Evain c M. Le Parquier c , Y. Takashima a ,Y. Tanikawa b Y. Taira b , N. Yamamoto a a Synchrotron Radiation Research Center, Nagoya University (Japan) b UVSOR Facility, Institute for Molecular Sciences, Okazaki (Japan) c Lab PhLAM,Université de Lille (France) Intense coherent THz synchrotron radiation induced by a storage ring FEL seeded with a femtosecond laser

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M. Hosaka a , M. Katoh b , C. Szwaj c , H. Zen b M. Adachi b , S. Bielawski c , C. Evain c M. Le Parquier c , Y. Takashima a ,Y. Tanikawa b Y. Taira b , N. Yamamoto a a Synchrotron Radiation Research Center, Nagoya University (Japan) - PowerPoint PPT Presentation

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Page 1: M. Hosaka a , M. Katoh b , C. Szwaj c , H. Zen b M. Adachi b , S. Bielawski c , C. Evain c

M. Hosakaa, M. Katohb, C. Szwajc, H. ZenbM. Adachib, S. Bielawskic, C. Evainc

M. Le Parquierc, Y. Takashimaa ,Y. Tanikawab Y. Tairab, N. Yamamotoa

aSynchrotron Radiation Research Center, Nagoya University (Japan) bUVSOR Facility, Institute for Molecular Sciences, Okazaki (Japan)

cLab PhLAM,Université de Lille (France)*

Intense coherent THz synchrotron radiation

induced by a storage ring FEL seeded with a femtosecond laser

Page 2: M. Hosaka a , M. Katoh b , C. Szwaj c , H. Zen b M. Adachi b , S. Bielawski c , C. Evain c

ContentsLaser bunch slicing and coherent

synchrotron radiation (CSR) Example: UVSOR experiment:

Storage ring FELSeeded storage ring FEL experimentSummary

Page 3: M. Hosaka a , M. Katoh b , C. Szwaj c , H. Zen b M. Adachi b , S. Bielawski c , C. Evain c

Laser Bunch Slicing and Coherent Synchrotron Radiation

(CSR)

BESSY, ALS, UVSOR-II etc.

• Injection of short pulse high power laser (100 fsec, 10 GW).• FEL interaction between the laser and electron beam inside undulator.

Storage ring

Page 4: M. Hosaka a , M. Katoh b , C. Szwaj c , H. Zen b M. Adachi b , S. Bielawski c , C. Evain c

Laser Bunch Slicing and CSR (Cont.)

After bending magnet(s)

Projection to horizontal (temporal) axis

△ z=R56△ e/EPhase space

• Local energy modulation is created. • After bending magnet, it is converted to density modulation(time of flight dispersion).• CSR is generated due to the micro-structure.

Page 5: M. Hosaka a , M. Katoh b , C. Szwaj c , H. Zen b M. Adachi b , S. Bielawski c , C. Evain c

M. Shimada et al. JJAP 46 (2007) 7939

Power radiated by N electrons=N2 x Power radiated by 1 electronSpectrum ~ Fourier transform of (z)

Laser Bunch Slicing and CSR (Cont.)

Page 6: M. Hosaka a , M. Katoh b , C. Szwaj c , H. Zen b M. Adachi b , S. Bielawski c , C. Evain c

Narrow-band CSR (@UVSOR-II)

S. Bielawski et al. Nature Physics, 4, 390–393 (2008)

Page 7: M. Hosaka a , M. Katoh b , C. Szwaj c , H. Zen b M. Adachi b , S. Bielawski c , C. Evain c

Narrow-band Coherent Synchrotron Radiation

:Measured spectra

“Tunable” “Narrow Band” CSR”

Application of narrow band CSR: H. Zen et al. TUPA 14

Page 8: M. Hosaka a , M. Katoh b , C. Szwaj c , H. Zen b M. Adachi b , S. Bielawski c , C. Evain c

CSR using a storage ring FEL (an internal laser) instead of an external

short pulse laser. Why SR-FEL?

Electron bunch

Optical klystronLaser pulse

MirrorMirror

•Storage ring FEL repetition rate is ~ 10 MHz !•Ordinal CSR (or Bunch slice): repetition rate is limited by laser repetition ( ~ 1 kHz or less)•Using SR-FEL, CSR with much higher repetition rate is expected.

Storage ring FEL

Page 9: M. Hosaka a , M. Katoh b , C. Szwaj c , H. Zen b M. Adachi b , S. Bielawski c , C. Evain c

Why Q-switch SR-FEL ?

0 ms 1 ms

0 ns

2 ns0 ns

2 ns

CW operation

Q-switch

• In stable CW lasing, the laser pulse width is determined by an equilibrium condition.

Short pulse lasing is difficult

• In storage ring, there are two types of lasing, CW lasing and repetitive Q-switch lasing .• In Q-switch mode, rf modulation technique is used and a higher peak power is available.

Streak camera image of temporal structure of FELSlow timeFa

st ti

me

Page 10: M. Hosaka a , M. Katoh b , C. Szwaj c , H. Zen b M. Adachi b , S. Bielawski c , C. Evain c

Why Q-switch SR-FEL ?• In Q-switch lasing, the lasing starts from noise.• If short pulse laser is injected to Q-switch FEL as seed, short pulse lasing is expected.• Long sustain high repetition rate CSR (or bunch slice) is expected.

Injection short pulse laser

Short pulse FEL lasing

Page 11: M. Hosaka a , M. Katoh b , C. Szwaj c , H. Zen b M. Adachi b , S. Bielawski c , C. Evain c

Experimental setup

Laser : Second harmonics of Ti:Sa laser : Pulse width: 300 fsec –FWHM or ~ 100 psec-FWHM Undulator: Helical optical klystron 400 nm

Ti: Sa m

ode lock laser:800 nm

2mJ

SHG = 400 nm

Infra-red Beamline

InSb:Bolometer

Helical optical klystron

UVSOR-II storage ring

C. Szwaj TUPB05H. Zen WEPA17

Page 12: M. Hosaka a , M. Katoh b , C. Szwaj c , H. Zen b M. Adachi b , S. Bielawski c , C. Evain c

Experimental result (streak camera)

FEL intensity

Streak Camera Image

700

psec

5 msec

100

psec

NO injection

700

psec

5 msec

Femto-sec injection

• Short pulse lasing(Shorter than s.c. resolution) • Faster rise time• Intensity is not so changed.

Page 13: M. Hosaka a , M. Katoh b , C. Szwaj c , H. Zen b M. Adachi b , S. Bielawski c , C. Evain c

Experimental result (CSR)

CSR intensity increases 50 times (as compared the case no injection)

Page 14: M. Hosaka a , M. Katoh b , C. Szwaj c , H. Zen b M. Adachi b , S. Bielawski c , C. Evain c

Experimental result ( FEL& CSR )

Simultaneous measurement of CSR and FEL

• CSR is produced in early stage of the lasing

Page 15: M. Hosaka a , M. Katoh b , C. Szwaj c , H. Zen b M. Adachi b , S. Bielawski c , C. Evain c

Simple phase space simulation(1)

Phase

Ene

rgy

0.7 times of Synchrotron oscillation: Laser field is weak.

Projection

Fresh Electron

Page 16: M. Hosaka a , M. Katoh b , C. Szwaj c , H. Zen b M. Adachi b , S. Bielawski c , C. Evain c

Simple phase space simulation (2)

1.5 times of Synchrotron oscillation :Laser field is strong

Phase

Ene

rgy

Fresh Electron

Page 17: M. Hosaka a , M. Katoh b , C. Szwaj c , H. Zen b M. Adachi b , S. Bielawski c , C. Evain c

Simple phase space simulation (3)

3.5 times of Synchrotron oscillationLaser field is strong

Ene

rgy

Phase

No Fresh Electron

Page 18: M. Hosaka a , M. Katoh b , C. Szwaj c , H. Zen b M. Adachi b , S. Bielawski c , C. Evain c

Simple phase space simulation (4)

Simulation almost reproduces the experimental result.Detailed calculation is in progress.

Page 19: M. Hosaka a , M. Katoh b , C. Szwaj c , H. Zen b M. Adachi b , S. Bielawski c , C. Evain c

SummarySucceeded in Q-switch FEL lasing seeded by femto-sec laserIntense CSR production is observedSimple simulation is made, detailed simulation is in progress.

Future Applications:Bunch slice to produce short pulse SRInjection of the amplitude modulated laser to produce narrow band CSR