Optical Parametrical Chirped Pulse Amplification

Transcription

1 Optical Parametrical Chirped Pulse Amplification for Petawatt Lasers Efim Khazanov Institute of Applied Physics of Russian Academy of Science Introduction Physics of OPCPA Compact 0.56 PW laser system - PEARL Scalability to multi-petawatt power Conclusion 1

2 Introduction. CPA invention D. Strickland and G. Mourou, "Compression of Amplified Chirped Optical Pulses," Opt. Commun. 56, 219 (1985). CPA 2

3 Introduction. OPCPA invention A. Piskarskas, A. Stabinis, and A. Yankauskas, "Phase effects in optical parametric amplifiers and oscillators of ultrashort optical pulses," Sov. Phys. Ups, 29, 969 (1986). A.Dubietis, G.Jonusauskas, A.Piskarskas, Powerful femtosecond pulse generation by chirped and stretched pulse parametric amplification in BBO crystal Opt. Commun. 88, 437 (1992) A.Piskarskas Vilnius University OPCPA 3

4 Optical Parametrical Chirped Pulse Amplification for Petawatt Lasers Introduction Physics of OPCPA Compact 0.56 PW laser system - PEARL Scalability to multi-petawatt power Conclusion 4

5 Physics of OPCPA. Wideband phase-matching ω ω + ω = ω = ω1 ω2 = ω Ω Ω () t () t k 10 v v 1 ϕ 12 2 Z k Δk 2x ( ω 2 ) = k 3x ( Ω ) = Δk( Ω ) z 0 k ϕ 12 2 ( ) Ω k 20 ϕ 13 k 3 Δk ( Ω) Δk(0) 0= phase-matching k 3 = k 0) + k 1 ( 2 (0) 2 Рис 1 2 dk1 dk 1 2z d k1 d k2z 2 + Ω 0( Ω dω dω Ω dω dω V 1g =0 wideband phase-matching = V 2g cos ϕ 12 =0 super-wideband phase-matching 3 ) 5

6 Physics of OPCPA. KD*P vs KDP. superbroadband 1800 phasematching FWHM of gain spectra, cm -1 (lines) generated phase matching λ signal =2λ pump =1053nm KD*P bandwidth KD P bandwidth KD*P absorption KDP absorption signal wavelength, nm KD*P DKDP V.V.Lozhkarev, G.I.Freidman, V.N.Ginzburg, E.A.Khazanov, О.V.Palashov, A.M.Sergeev, I.V.Yakovlev. Laser Physics, 15, 1319 (2005). 0,35 0,3 0, ,2 = + 527nm 911nm 1250nm 0,15 0,1 0,05 0 ordinary wave absorbtion, cm -1 (dots) 6

7 Physics of OPCPA. Monochromatic case. Pump beam aberration are transferred to new wave pump beam (with aberration) amplified beam (no aberration!) new injected beam no aberration beam (with aberration) OPCPA pump beam (with aberration) OPCPA injected beam no aberration new beam (with aberration) amplified beam (no aberration!) Injected beam keeps its (plane) wavefront at any pump wavefront 7

8 Physics of OPCPA. Defenition of signal and idler waves. Wide-band case. Signal beam is injected Idler beam is injected OPCPA pump beam (monochromatic) amplified beam wide-band! no angular chirp! injected beam no angular chirp new beam with angular chirp! narrow-band! injected beam no angular chirp new beam with angular chirp! wide-band! pump beam (monochromatic) OPCPA amplified beam narrow-band! Signal beam must be injected. Not idler. Idler may be injected with angular chirp. 8

9 Physics of OPCPA. Wideband phase-matching ω ω + ω = ω = ω1 ω2 = ω Ω Ω () t () t k 10 v v 1 ϕ 12 2 Z k Δk 2x ( ω 2 ) = k 3x ( Ω ) = Δk( Ω ) z 0 k ϕ 12 2 ( ) Ω k 20 ϕ 13 k 3 Δk ( Ω) Δk(0) 0= phase-matching k 3 = k 0) + k 1 ( 2 (0) 2 Рис 1 2 dk1 dk 1 2z d k1 d k2z 2 + Ω 0( Ω dω dω Ω dω dω V 1g =0 wideband phase-matching = V 2g cos ϕ 12 =0 super-wideband phase-matching 3 ) 9

10 Non-degenerated broadband phase-matching in KD*P. Experiments with injection of idler angular-chirped wave. Injected (idler) divergence 4mrad 4mrad Output (signal) divergence 10 mrad 10 mrad 100nm Injected (idler) wavelength Output (signal) wavelength 10

11 OPCPA vs CPA Advantages of OPCPA: + broad gain bandwidth + high aperture + considerable decrease in thermal loading + significantly lower level of ASE + very high gain + no self-lasing + no backscattering from a target Disadvantages of OPCPA: high precision synchronization high quality of a pump beam short (1ns) pump pulse duration 11

12 Optical Parametrical Chirped Pulse Amplification for Petawatt Lasers Introduction Physics of OPCPA Compact 0.56 PW laser system - PEARL Scalability to multi-petawatt power Conclusion 12

13 PEtawatt parametric Architecture Laser (PEARL). Synchronization system Nd:YLF Q-switch laser λ=1053nm 10mJ 12nc Pulse shaper Cr:Forsterite fs-laser λ=1250nm 2nJ 40 fs 1nJ 0.5 ns Stretcher 40 fs 0.5 ns 1mJ 1.5ns 1 J 1.5ns Two-stage Nd:YLF amplifier 2J 1.5 ns OPA I KD*P CW Yb:fiber pump 10W λ= nm 2ω λ=911nm 0.8mJ 0.5ns OPA II KD*P λ=1250nm First λ=911 nm 50 mj 0.5 ns phase (TW Compressor 0.5 ns 50 fs level) 50 mj 50 fs 2 Hz Nd:glass amplifier 300J 1ns 2ω 170J 1ns OPA III KD*P 10cm dia 38J 0.5ns Compressor 0.5ns 50fs 24J 43fs Second phase (PW level) Freidman G., Andreev N., Ginzburg V., Katin E., Khazanov E., Lozhkarev V., Palashov Sergeev Institute A., Yakovlev of Applied I. Proc. Physics, SPIE, Russia v.4630, p , khazanov@appl.sci-nnov.ru O., 13

14 PEtawatt parametric Laser (PEARL). Nd:glass laser output beam 300J, 1ns λ/D=21μrad 50 μrad мм 14

15 PEtawatt parametric 110mm clear aperture ОPA Laser (PEARL). OPA 120 mm clear aperture SHG From front-end system (911nm) 300 J 1054 nm pump pulse OPA 3 38J to compressor (911nm) To diagnostic 300 J 1054 nm 180 J 527 nm SHG 910 nm Institute of Applied Physics, To compressor Russia From OPA 2 khazanov@appl.sci-nnov.ru 15

16 PEtawatt parametric Laser (PEARL). Energy characteristics of final OPCPA Efficiency, % Efficiency, % Pulse energy. J 38 J Output pulse energy, J 2.44λ/D=21μrad 25μrad Pump pulse energy, J

17 PEtawatt parametric Laser (PEARL). Compressed 0.56 PW pulse ACF experiment ACF of 33fs FTL pulse ACF, a.u time, fs 24 J/43fs=0.56PW Contrast: 10 8 (0.5ns window) 10 4 (1ps window) Lozhkarev V.V., Freidman G.I., Ginzburg V.N., Katin E.V., Khazanov E.A., Kirsanov A.V., Luchinin G.A., Mal'shakov A.N., Martyanov M.A., Palashov O.V., Poteomkin A.K., Sergeev A.M., Shaykin A.A., Yakovlev I.V. Laser Physics Letters, 4, (2007). 17

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19 Optical Parametrical Chirped Pulse Amplification for Petawatt Lasers Introduction Physics of OPCPA Compact 0.56 PW laser system - PEARL Scalability to multi-petawatt power Conclusion 19

20 Scalability to multi-petawatt power. Sarov N.Novgorod. Synchronization system Nd:YLF Q-switch laser λ=1053nm 10mJ 12nc Pulse shaper Cr:Forsterite fs-laser λ=1250nm 2nJ 40 fs 1nJ 0.5 ns Stretcher 40 fs 0.5 ns 1mJ 1.5ns 1 J 1.5ns Two-stage Nd:YLF amplifier 2J 1.5 ns OPA I KD*P CW Yb:fiber pump 10W λ= nm 2ω λ=911nm 0.8mJ 0.5ns OPA II KD*P λ=1250nm First phase ( λ=911 nm 70 mj 0.5 ns Compressor 0.5 ns 70 fs TW level) 32 mj 70 fs 2 Hz Nd:YLF Q-switch laser λ=1053nm 10mJ 12nc Pulse shaper Nd:YLF amplifier Nd:glass amplifier Nd:glass amplifier 300J 1ns 2kJ 1.5ns 2ω 2ω 180J 1ns 1kJ 1.5ns OPA III KD*P 10cm dia OPA IV KD*P 20cm dia 38J 0.5ns 150J 0.5ns Second phase (PW Compressor 0.5ns 50fs Third Compressor 0.5ns 50fs level) 24J 43fs phase ( 2 PW) 100J 50fs 20

21 Scalability to multi-petawatt Projects overview fs 1PW December, 2008 power λ/d = 12.2 μrad chirped pulse energy, J fs 600TW October, Pump energy, J I.A. Belov, O.A. et al. Petawatt laser system of the "Luch" facility International Institute Conference of Applied X Physics, Khariton's Russia Scientific Reading. p.145 khazanov@appl.sci-nnov.ru (2008). 21

22 Scalability to multi-petawatt State of the art. power. laser power, TW CPA 0.56 PW 1 PW year Vilnius U., Lithuania Rutherford Lab, UK SIOM, China Rochester, USA LLNL, USA IAP, Russia LLNL, USA Rutherford Lab, UK ILE, Japan JAEA, Japan SIOM, China Texas U., USA Sarov 22

23 Scalability to multi-petawatt Projects overview. power. PEARL-10, IAP, Russia, , 10PW Rutherford Lab, UK, , 10PW ELI, pan-european, PW (may be CPA or OPCPA) International Center for Extreme Light Study, Russia, , 200PW (under consideration in the Russian Government) 23

24 Scalability to multi-petawatt power. Rutherford Lab, UK, , 10PW Seed laser 300nmbandwidth High rep rate mj Pump 10PW Project Schematic Two Phases Phase I Joule level Hz repetition rate Phase II >300J; <30fs 1 shot every hour LBO Seed λ=900нм Phase I Stand alone ~3ns shaped pulse Few Hz rate Long stretch ~3 ns LBO LBO Diagnostic compressor Expanded Target Area East Interaction Chamber 300 J, 30 fs 10 PW, Wcm -2 KD*P DKDP KD*P DKDP >500 J Compress SHG Additional Vulcan 2 x 1.2 kj 3 ns 208 beamlines SHG 600 J 527 nm 600 J 527 nm Phase II 2 24

25 OPCPA scalability to multi-petawatt power. Estimation for laboratory scale option + Pulse duration: x2.5 (18fs instead of 45fs) + OPCPA efficiency: x2 (40% instead of 20%) + Pump power x3.3: (600J instead of 180J) + Compressor efficiency x1.2 (76% instead of 66%) TOTAL: x20 ( 10PW instead of 0.56PW ) 25

26 OPCPA scalability to multi-petawatt power. PEARL-10, IAP, Russia, , 10PW Synchronization system Nd:YLF Q-switch laser λ=1053nm 10mJ 12nc Pulse shaper Cr:Forsterite fs-laser λ=1250nm 2nJ 40 fs 1nJ 0.5 ns Stretcher 40 fs 0.5 ns 1mJ 1.5ns 1 J 1.5ns Two-stage Nd:YLF amplifier 2J 1.5 ns OPA I KD*P CW Yb:fiber pump 10W λ= nm 2ω λ=911nm 0.8mJ 0.5ns OPA II KD*P λ=1250nm First phase ( λ=911 nm 70 mj 0.5 ns Compressor 0.5 ns 70 fs TW level) 32 mj 70 fs 2 Hz Nd:glass amplifier 300J 2ns 2ω Nd:glass amplifier 200J 2ns 300J 2ns OPA III KD*P 10cm dia 2ω 80J 2ns 200J 2ns Nd:glass amplifier OPA IV KD*P 15cm dia 2ω 300J 2ns OPA V KD*P 20cm dia Second Compressor 2ns 15fs phase (10 PW 160J 2ns 200J 2ns 240J 2ns 180J 18fs 10PW level) 26

27 OPCPA scalability to multi-petawatt power. PEARL-10, IAP, Russia, , 10PW

28 OPCPA scalability to multi-petawatt power. PEARL-10, IAP, Russia, , 10PW

29 OPCPA scalability to multi-petawatt power. PEARL-10, IAP, Russia, , 10PW

30 OPCPA scalability to multi-petawatt power. PEARL-10, IAP, Russia, , 10PW

31 OPCPA scalability to multi-petawatt power. PEARL-10, IAP, Russia, , 10PW

32 Before conclusion. Another mission of OPCPA The CPA technique compresses 5ns, 20kJ into a ~20ps pulse. This pulse is used after frequency doubling, to pump an OPCPA. A strong idler wave is produced at 1250nm. The latter seeds, the plasma compression cell where by interfering with the 20ps pump pulse at 1050nm converts and transfers the pump into the seed pulse at 1250 nm. To preserve the pulse shortness, a prism in the OPCPA is used to produce the necessary angular chirp. G. A. Mourou, N. J. Fisch, V.M.Malkin, Z.Toroker, E.A.Khazanov, A.M.Sergeev, T.Tajima Exawatt-Zettawatt Pulse Generation and Applications submitted Institute of to Applied Optics Communications Physics, Russia khazanov@appl.sci-nnov.ru 32

33 Before conclusion. Another mission of OPCPA Diagram displaying the concept of Multiple-Beam-Pumping showing that the energy from several beams can be transferred to one signal seed pulse. 33

34 Before conclusion. Another mission of OPCPA Chirped Pulse Amplification + Optical Parametric Chirped Pulse Amplification + Plasma Compression by Raman Amplification = Cascaded Conversion Compression = C 3 34

35 Conclusion OPCPA will keep a major role on the route(s) to 10+ PW laser. Let s keep going. 35

36 V. Ginzburg E. Katin E. Khazanov A. Kirsanov V. Lozhkarev G. Luchinin S. Mironov M. Martyanov O. Palashov A. Poteomkin A. Sergeev A.Shaykin A. Soloviev M. Starodubtsev I. Yakovlev V. Zelenogorsky 36

37 Instead of Conclusion #1. OPCPA at 910 nm in DKDP is the best. No question. #2. There is only one question. Q.: The best or one of the best? A1: See message #1. 25μrad A2: Will live and see. 37

38 Physics of OPCPA. Wavefront distortions. Pump beam aberration transfers to new wave Pump beam deviation transfers to new wave pump (with aberration) Injected beam (no aberration!) OPCPA Injected beam New beam (with aberration) Injected beam keeps its wavefront at any pump wavefront 38

39 Introduction. Petawatt laser systems type I type II type III Gain medium Nd:glass Ti:sapphire KD*P Energy source Nd:glass Nd:glass Nd:glass Pump no 2ω Nd 2ω Nd Pump duration, ns no <30 1 Amplifier aperture, cm 40х х40 Minimum duration, fs Efficiency (1ω Nd фс), % Number of PWs from 1 kj 1ω Nd 4(3) 8 ( 5 ) 4 First PW-level power 1.3 PW LLNL, PW JAEA PW IAP 2006 Diffraction grating damage threshold Ti:sapphire damage threshold 39