Mitsuru Uesaka- Laser plasma cathode by 12 TW, 50 fs laser and its application to radiation chemistry

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  • 8/3/2019 Mitsuru Uesaka- Laser plasma cathode by 12 TW, 50 fs laser and its application to radiation chemistry

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    Laser plasma cathode by 12 TW, 50 fs laser

    and its application to radiation chemistry

    Mitsuru Uesaka

    Nuclear Engineering Research Laboratory ,

    University of Tokyo

    June 26, 2004

    International Symposium on

    Ultrafast Accelerators for Pulse Radiolysis

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    Two New Accelerator Rooms

    Compact Medical Linac/Laser Plasma Beam Source

    Linac Building(1st Floor)

    Fusion Blanket Building(1st Floor)

    Compact Medical Linac

    Laser Plasma Beam Source

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    12TW 50fs Laser Plasma Beam Source

    Amplifier 2

    Amplifier 1

    Clean Room

    Regenerative amplifier

    Pre-amplifier

    YAG lasers

    Laser system

    Compressor chamberExperimental area

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    0.0 25.0 50.0 100.075.0

    [mm]

    0.0

    50.0

    100.0

    150.0

    200.0

    250.0

    300.0

    350.0

    90

    180

    270

    Energetic electronsup to ~40MeV

    Spotsize D~8.1mm (FWHM)

    Typical Image of Electron Beam Generation(Experimental Results: Signals on I.P.)

    (180mm from gasjet)He 2.8x1019cm-3, Laser ~4.8TW

    Experimental Set-up

    Reference:T.Hosokai,et al.,Phys Rev.E 67,036407 (2003)

    0 20 40 60Electron Energy [MeV]

    PIC simulation

    1 0-2

    10-3

    10-4

    10-5

    Ele

    ctr

    on

    Dis

    trib

    ut

    ion

    [ar

    b.u

    n]

    Electro

    nSignal[arb.un]

    e-spectrum

    a b c

    Laserpulse

    -1~1ns (Main Pulse)b: 1ns~3ns c: 2ns~5ns

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    Pump-and-probe Experiment Using Plasma Cathode at University of Tokyo

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    Pump and probe Experiment Using Plasma Cathode at University of Tokyo

    Fs laser

    Probe laser

    50fs(FWHM)

    Pump EB

    40fs(FWHM)

    Supersonic

    He gas jet

    Sample

    Photo-detectors

    for measuring

    light absorption

    Fig. Schematic diagram of pump-probe

    experiment using plasma cathode

    Dominant factors for time resolution

    EB for pump : 40fs(FWH Laser for probe : 50fs(FWH

    Timing jitter : ~0fs

    Desynchronization in sample : ~1ps/mm

    Current problems to be solved Electron beam

    - Energy spread : 100%

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    Big Advantage of Laser Plasma Accelerator

    for Pump-and-probe analysis

    Synchronization is perfectly passive without any electronics.

    12TW Laser

    Beam Splitter Optical Delay

    Laser Plasma Cathode

    Laser(50fs)

    Electron Bunch(40fs)

    No timing jitter and drift between laser and secondary beam.Femtosecond time-resolved analysis is surely available

    after the bean quality and stability are upgraded.

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    Summary of Synchronization

    1. Laser vs Accelerator Synchronization System via Electronics

    Picoseconds time-resolution

    2. Laser Seeded Staged Accelerator

    Femtoseconds time-resolution

    Available for multibunches

    3. Laser Plasma Accelerator

    Beam Splitter enables even Attoseconds time-resolution

    After Stable and reliable beam generation and diagnosis

    are established

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    Tens Femtosecond or Quasi Monochromatic Electron Single Bunch

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    Tens Femtosecond or Quasi-Monochromatic Electron Single Bunch

    by Laser Plasma Cathode (RAL, LBNL, LOA, AIST, U.Tokyo at AAC2004)

    100

    101

    102

    103

    104

    600 700 800 900 1000 1100 1200 1300

    Intens

    ity

    (arb.unit)

    Wavelength (nm)

    1st-Stokes

    Laser Wavelength

    Tens femtoseconds

    Quasi-

    monochromatic

    U.Tokyo(cal)

    AIST(exp)

    AAC 2004 Experimental Results Laser-Plasma Accelerator WG

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    AAC 2004 Experimental Results Laser Plasma Accelerator WG

    2

    MeV

    Self-

    trapped

    1x101

    8 cm-3

    2TW0.8

    mkm

    SM-

    LWF

    A

    KERI

    Glass

    capillary

    100 MeV

    Self-

    trapped

    6x1016 cm-3

    30TW1.06 mkm

    LWFA

    Osaka

    University

    2 TW

    beam for

    LIPA

    injector

    Ponderom

    otive

    channel

    Integrated

    over 90

    shots

    spectrum

    Channel

    40 MeV20 MeV38 MeV40 MeV7 1 MeV

    2 pC

    78 2

    MeV

    20 pC

    86 2 -150

    MeV

    300 pC

    >17015

    MeV, 500

    pC,

    Energy

    Gain

    Self-

    trapped

    Optical

    Injectionioniz.

    12 MeV

    external

    Self-

    trapped

    Self-

    trapped

    Self-

    trapped

    Self-

    trapped

    Self-trappedInjector

    type

    1.4x1020

    cm-31x1019 cm-3

    1x1016 cm-3

    1.8x1019

    cm-3.1.5x1020

    cm-32x1019 cm-

    3

    2x1019 cm-3

    6x1018 cm-3Plasm.

    Density

    20TW0.8

    mkm2.x10

    19

    W/cm2W0

    =5 mkm,,

    23fs

    10TW1.06

    mkm3x10

    18

    W/cm2W0

    =12 mkm,

    500s

    1TW10.3+

    10.6.mk

    6TW0.8 mkm

    1x1019

    W/cm2W0

    =6

    mkm,50fs

    2TW 0.8mkm

    5x1018

    W/cm2W0

    =5

    mkm,50fs

    16TW0.8

    mkm ,1x1

    018

    W/cm2W0

    =25

    mkm,40fs

    8TW0.8

    mkm,1x10

    19

    W/cm2W0

    =7 mkm,

    55fs

    30TW0.8 mkm,

    3x1018

    W/cm2,

    W0=18

    mkm, 30fs

    Laserparrs

    SM-

    LWFA

    SM-

    LWFA

    PBWASM-

    LWFA

    SM-

    LWFA

    SM-

    LWFA

    SM-

    LWFA

    SM(for-

    ced)LWFA

    Scheme

    JAERINRLNeptune,

    UCLA

    University

    of Tokio

    AISTRAL-

    alphaX

    LBNLLOA