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

19
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

Upload: grant-perry

Post on 19-Jan-2016

216 views

Category:

Documents


0 download

TRANSCRIPT

Page 1: 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

M. Hosakaa, M. Katohb, C. Szwajc, H. Zenb

M. 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 M. Le Parquier c, Y. Takashima a,Y. Tanikawa b Y. Taira b, N. Yamamoto

Contents

Laser bunch slicing and coherent

synchrotron radiation (CSR)

Example: UVSOR experiment:

Storage ring FEL

Seeded storage ring FEL experiment

Summary

Page 3: 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

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 M. Le Parquier c, Y. Takashima a,Y. Tanikawa b Y. Taira b, N. Yamamoto

Laser Bunch Slicing and CSR (Cont.)

After bending magnet(s)

Projection to horizontal (temporal) axis

△ z=R56△ e/E

Phase 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. Le Parquier c, Y. Takashima a,Y. Tanikawa b Y. Taira b, N. Yamamoto

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

Power radiated by N electrons

=N2 x Power radiated by 1 electron

Spectrum ~ 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 M. Le Parquier c, Y. Takashima a,Y. Tanikawa b Y. Taira b, N. Yamamoto

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 M. Le Parquier c, Y. Takashima a,Y. Tanikawa b Y. Taira b, N. Yamamoto

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 M. Le Parquier c, Y. Takashima a,Y. Tanikawa b Y. Taira b, N. Yamamoto

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

short pulse laser. Why SR-FEL?

Electron bunch

Optical klystron

Laser 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 M. Le Parquier c, Y. Takashima a,Y. Tanikawa b Y. Taira b, N. Yamamoto

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 timeF

ast

time

Page 10: 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

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 M. Le Parquier c, Y. Takashima a,Y. Tanikawa b Y. Taira b, N. Yamamoto

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: S

a mode lock laser:

800 nm 2m

JSHG = 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 M. Le Parquier c, Y. Takashima a,Y. Tanikawa b Y. Taira b, N. Yamamoto

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 M. Le Parquier c, Y. Takashima a,Y. Tanikawa b Y. Taira b, N. Yamamoto

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 M. Le Parquier c, Y. Takashima a,Y. Tanikawa b Y. Taira b, N. Yamamoto

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 M. Le Parquier c, Y. Takashima a,Y. Tanikawa b Y. Taira b, N. Yamamoto

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 M. Le Parquier c, Y. Takashima a,Y. Tanikawa b Y. Taira b, N. Yamamoto

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 M. Le Parquier c, Y. Takashima a,Y. Tanikawa b Y. Taira b, N. Yamamoto

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 M. Le Parquier c, Y. Takashima a,Y. Tanikawa b Y. Taira b, N. Yamamoto

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 M. Le Parquier c, Y. Takashima a,Y. Tanikawa b Y. Taira b, N. Yamamoto

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