Exawatt Center for Extreme Light Studies Project (XCELS)

Transcription

1 Exawatt Center for Extreme Light Studies Project (XCELS) A.G. Litvak, E.A. Khazanov, A.M. Sergeev Institute of Applied Physics of the Russian Academy of Sciences Nizhny Novgorod, Russia

2 XCELS- EXawatt Center for Extreme Light Studies is a new research infrastructure selected by the Russian government among 6 mega science projects to be constructed by XCELS is based on a new laser facility comprising of 12 amplification channels, each of them providing 400 J, 25 fs pulses, with the total pulse power of almost 200 PW. A new research institute will be built around this laser facility. 12 channels 15 PW each 400 J, 25 fs, 910 nm Quality: 3 divergence limits Phasing: T/10

3 Host Institute: IAP RAS IAP RAS began independent activities in April IAP RAS is one of the largest and most successful institutions of the Russian Academy of Sciences. Scientific studies are provided by about 1,200 employees, about 490 of whom are scientists, including 11 academicians and corresponding members of RAS, around 90 doctors and 200 candidates of science. About one third of the scientists are young people aging less than 35. Main directions of research: high power microwave electronics plasma physics and plasma technologies radiophysical methods of diagnostics and remote sensing wave processes in geophysics dynamics of nonlinear processes,laser physics and nonlinear optics (pioneering works in self-focusing, relativistic nonlinear optics, OPA, phase conjugation awarded by USSR State Prizes) Exawatt Center for Extreme Light Studies (XCELS)

4 PEARL First petawatt OPCPA laser in the world 3 cascades of parametric amplification in DKDP crystals (the final stage with aperture D = 10 cm) ensures total amplification gain 24 J/43 fs = 0/56 PW Focusable to W/cm 2

5 From PEARL to XCELS PEARL 0.5 PW Front-end for XCELS-Proto 2007 PEARL 10 5 PW Technological upgrade of PEARL 2013 XCELS - Proto 2 x 10 PW Scaling of PEARL to d30 cm DKDP 2016 XCELS 12 x 15 PW Final 2020

6 From PEARL to PEARL 10 PEARL PEARL 10 Growth rate Pulse duration 45 fs 25 fs 2 Pump laser 2ω 180 J 270 J 2 cascades (527 micron, 2 ns) Crystal size 10x10 cm x12.5 cm Efficiency (compressed) 15% 25% PW x 2 x 2 x 1.5 x 1.6 = 5 PW PEARL-10: Increasing OPCPA power of PEARL facility in 10 times

7 From PEARL to PEARL 10 4 cascades of parametric amplification in DKDP crystals (2 final stages with aperture D = 12.5 cm) to ensure total amplification gain Repetition rate to be increased from 1/30min to 1/(1-3)min

8 XCELS Main Technological Issues: Scaling of PEARL to 30 cm aperture DKDP crystal 2-3 kj Nd:glass pump lasers 12 separate amplifying chains with shared front-end Adaptive optics to provide beam quality and coherent combining First prototyping stage - XCELS-Proto - two channel laser facility to be built at IAP RAS

9 XCELS-Proto PEARL architecture FEMTA & UFL-2M architectures (Sarov)

10 Available Technologies Crystals 1-3 with mm size were grown by the high-rate growth technique for about 40 days. KDP crystal 4 with mm size was grown by a conventional technique for about a year.

11 Available Technologies "LUCH" facility with parametric amplifier FEMTA at VNIIEF (Sarov) and record characteristics of parametric amplification of femtosecond pulses

12 Available Technologies Schematic diagram of the compressor. Gratings G-2 and G-3 are composite here. For normal operation of the 15 PW compressor diffraction gratings of appropriate size (500 mm 800 mm) are required. For the radiation energy of a pulse arriving at the compressor of 500 J, the energy density in a 40 cm beam will be a little more than 0.4 J/cm2.

13 XCELS Layout

14 Focusing geometry for 12 XCELS beams Rule of thumb for coherent combining of several beams: To maximize the electric field at focusing point, radiation of several combining beams should reproduce configuration of phase conjugated dipole radiation field z x Minimum focusing volume

15 Belt and Double-Belt approximation of dipole wave Intensity, W/cm 2 1,5 1 0,5 0 Belt Number of beams 1,5 1 0,5 0 Dipole-wave (ideal) Double-Belt P total = 180 PW W/cm 2 single beam (f = 1) Number of beams W/cm 2 W/cm 2 Belt-6 Double-Belt-12

16 How many EW from 200 PW? Geometry Single beam (f=1.2) Belt-8 8 (f=1.2) Belt-3 3 (f=0.3) Double-Belt (f=0.96) Power per channel Intensity, W/cm 2 I/I(f=1.2) Equivalent power (f=1.2) P 0 =200 PW PW P 0 / EW P 0 / EW P 0 / EW Dipole-Wave EW P total = 200 PW

17 XCELS Exawatt-and-Beyond Program C3 = CPA + OPCPA + BRA No coherence combining required! Malkin, V. M. et al. Fast compression of laser beams to highly overcritical powers. Phys. Rev. Lett. 82, (1999) G.Mourou et al. Exawatt-Zettawatt Pulse Generation and Applications, Opt.Com. (2011) R. M. G. M. Trines et al. Simulations of efficient Raman amplification into the multipetawatt regime, Nat.Phys. 7, p.87 (2011) Exawatt Center for Extreme Light Studies (XCELS)

18 XCELS Program of Experimental Research 1. Creation of sources of ultrashort coherent and incoherent radiation with record high brightness in the X-ray and gamma ranges based on radiation of ultrarelativistic charged particles moving in ultraintense laser fields, use of these sources for diagnosing processes and structures with picometer spatial and subfemtosecond temporal resolution. 2. Development of multicascade compact laser electron accelerators with energies above 100 GeV, use of the laser-plasma acceleration principles for developing advanced accelerator complexes with particle energies of 1-10 TeV. 3. Elaboration of compact laser ion accelerators with energies of GeV and development of their applications in radiography and medicine. 4. Production and investigation of extreme states of matter arising under the action of ultrarelativistic laser fields; modeling of astrophysical and early cosmological phenomena in laboratory conditions. Exawatt Center for Extreme Light Studies (XCELS)

19 XCELS Program of Experimental Research 5. Creation of sources of electromagnetic waves of attosecond (10-18 s) and subattosecond duration based on the generation of high harmonics of laser radiation and supercontinuum in a hyperwide spectral range in the course of the nonlinear interaction of powerful femtosecond laser pulses with matter, development of methods for application of such sources in the fundamental metrology and diagnostics of fast processes in matter. 6. Creation of a source of electromagnetic radiation with peak power over 1 Exawatt (10 18 W) on the basis of the interaction of multipetawatt laser pulses with plasma in ultrarelativistic regime. 7. Study of the space-time structure of vacuum probed by radiation with intensity exceeding W/cm 2, investigation of the phenomena of quantum electrodynamics in the presence of ultraintense laser fields, including producing of matter and antimatter by means of radiation. 8. Research into a new field of science nuclear optics based on the use of secondary sources of gamma radiation for excitation and diagnostics of intranuclear processes. Exawatt Center for Extreme Light Studies (XCELS)

20 XCELS Program of Experimental Research Experiments in three dedicated ELI areas where high-field effects will be marginally observable at ELI-Beamlines, ELI-ALPS, and ELI-NP facilities New experimental areas that are opened up with XCELS power and intensity Developments to exawatt-and-beyond power and W/cm 2 - and- beyond intensity using XCELS radiation conversion at nonlinear coupling with matter and vacuum Exawatt Center for Extreme Light Studies (XCELS)

21 XCELS Program of Experimental Research New experimental areas that are opened up with XCELS power and intensity 1. Dominating radiative losses new γ-ray sources 2. Relativistic ions 3. Probing vacuum by light 4. Plasma with exotic parameters Exawatt Center for Extreme Light Studies (XCELS)

22 XCELS Program of Experimental Research At W/cm 2 radiative losses over the field cycle become comparable with energy acquired by electron from the laser field Ultrarelativistic electrons are just convertors of energy from visible to gamma range and plasma becomes a strongly absorptive medium This fact evokes some skepticism regarding usage of very high fields for regular electron acceleration On the other hand, it opens up opportunities to create a variety of new gamma sources with unique parameters

23 Electron Trapping and Directed Gamma Rays Excitation at Converging Dipole Wave Laser Focusing To maximize the electric field at focus, radiation of several combining beams should reproduce configuration of phase conjugated dipole radiation field 12 beams 200 PW total > W/cm 2 Electron density versus time and radius at 30 fs dipole wave laser pulse focusing with peak total power of 200 PW A.V.Bashinov et al. Quantum Electronics 43(4),291 (2013), A.Gonoskov et al. arxiv: v1 [plasm-ph] Hard photon emission distribution as a function of angle and energy (radial coordinate, log scale)

24 Generation of Giant Attosecond Pulses at Laser Interaction with Solid Density Target Overcritical plasma surface Incident pulse, W/cm 23 W/cm 2 2 Oscillating Mirror Model (OMM) S.V. Bulanov et al., Phys. Plasm (1994) S.R. Lichters et al., Phys. Plasm (1996) S. Gordienko et al, PRL (2004) T. Baeva et al., PRE (2006) D. an der Brugge at al, Phys. Plasm (2010) Re-emitted pulse Relativistic Electronic Spring (RES) Model A.Gonoskov et al, PRE (2011)

25 Stages: Effect of Relativistic Electronic Spring 1) pushing of electrons and the formation of a thin current layernanoplasmonic structure, which results in energy transfer from the laser field to the plasma fields and particles; 2) backward motion of the electrons towards the incident wave with conversion of energy accumulated in the plasma and laser field energy into the kinetic energy of an ultrarelativistic electron bunch; 3) radiation of the attosecond pulse by an electron bunch due to conversion of the kinetic energy and laser field energy to the XUV and X- ray range. Y X Z v plasma csin electrons ions

26 Pair Production from Vacuum For 200 PW and W/cm 2 at the groove target 0.5 mm wide we have W/cm 2 in the volume V~10nm 3 Number of pairs N~10 9 Cascades are strongly suppressed due to the superluminal motion of the focal area W/cm 2 10 nm v f = c/sinθ

27 Laser Intensity vs. Years XCELS I Z E S T ELI- DC

28 XCELS Program of Experimental Research Vacuum breakdown Laser facilities probing vacuum XCELS gamma ray sources radiative losses relativistic ions EM cascades XCELS ELI I-III relativistic electrons ionization

29 Collaboration of Russian Research Centers Institute of Applied Physics RAS (IAP RAS) Institute on Laser and Information Technologies RAS (ILIT RAS), Russian Research Center (RRC) "Kurchatov Institute", Joint Institute for Nuclear Research (JINR), P.N.Lebedev Physics Institute RAS (LPI RAS), General Physics Institute RAS (GPI RAS), Budker Institute of Nuclear Physics (BINP), Joint Institute for High Temperatures RAS (JIHT RAS), Institute of Laser Physics of the Siberian Branch of RAS (ILP SB RAS), Russian Federal Nuclear Center (RFNC-VNIIEF), Moscow State University (MSU), National Research Nuclear University MEPhI (MEPhI), University of Nizhny Novgorod (UNN), and others Exawatt Center for Extreme Light Studies (XCELS)

30 International Collaboration The main contribution of foreign partners is supposed in the form of high-tech research equipment for the laser complex and research laboratories, totaling about 15% of the Project cost. Interest from: The Ministry of Education and Science of France The Commissariat of Atomic Energy of France The Nuclear Energy Agency of Japan, High Energy Accelerator Research Organization KEK (Japan), Los Alamos National Laboratory (USA), Fermi National Accelerator Laboratory (USA), Rutherford Appleton Laboratory (UK), The John Adams Institute for Accelerator Science (UK), Center for Antiproton and Ion Research FAIR (Germany), National Research Institute of Canada XCELS and ELI Joint Venture? Exawatt Center for Extreme Light Studies (XCELS)