50 Years of the Laser in the City of Light

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    50 Years of the Laser in the City of LightWednesday, June 23, 2010

    Ecole Pol techni ue

    Palaiseau

    Hi h Fi l i n

    A Second Wave of LaserToshiki Tajima

    Blaise Pascal Chair,

    . ourou,

    Institut de Lumire Extrme

    andLMU,MPQ, Garching

    Acknowledgments for collaboration and advice: G. Mourou, F. Krausz, D. Habs. K. Homma, M.

    Kando, A. Suzuki, F. Takasaki, M. Teshima, W. Leemans, E. Esarey, S. Karsch, F. Gruener, W.

    1

    an ner, . euer, . a we , . oses, . s r epov, . u anov, . a aune, . ross, .

    Urakawa, H. Gies, T. Heinzl, R. Schuetzhold, G. Dunne, K. Kondo, S. Iso, X. Yan, R. Assmann, C.Barty, M. Nozaki, A. Chao, W. Chou, N. Naumova, J. Chambaret, C. Keitel, P. Chomaz, D.

    Normand P. Martin P. Chen M Downer A. Caldwell

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    Laser probing nonlinearities in matter

    vs

    m

    eEx

    2

    x

    ~

    Rutherfords (accelerator) approach vs Laser approach

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    E =m c2

    NL Optics

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    Chirped Pulse Amplification did it!

    100fs100fs

    D. Strickland and G. Mourou 1985

    4

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    Nonlinearities in atom, plasma, and vacuum

    AtomicPlasma electronnonlinear Vacuum nonlinearity

    vs.

    Keldysh field forlaseratomic

    Schwinger field forvacuum breakdown

    Laserwakefield

    ionization

    Compact high energy colliders

    Compact accelerator applications

    Nonlinear QED fields

    General relativistic effects

    e acce era on or quan um grav y acuum pro e s.a. ar energy

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    Relativistic nonlinearity under intense laser

    Plasma free of binding potential , but its electron responses:

    a)a) ClassicalClassical optics :optics : v

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    WakefieldNonlinearity-driven, CollectiveCollective phenomenon = all particles in medium participate

    Kelvin wake

    Wave breaks at vcNo wave breaks and wake peaks at vcNonlinearities of plasma and water waves

    (Wave-head hardto overtake trough. density cusp singularity)

    (Wave-head overtakes trough)

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    Thousand-fold Compactification

    Laser Wakefield Acceleration (LWFA): 103-4 fold gradient

    --

    -

    -

    ---------

    --- --------

    ---

    plasma

    ~ . mm

    -

    -- -

    --

    --

    ----

    -

    -- -

    -----

    ---

    -

    -

    --

    -

    -

    -----

    ---

    - -

    --

    --

    --

    - ++

    +

    ++

    + +++

    ++

    +

    +

    ++

    ++

    + ++--

    -

    - ---

    --

    --

    -

    - - --

    (gas tube)

    upercon uc ng nacr - u e

    Fermilab

    ~40cm

    Emax

    ~32MV/mEmax~100,000MV/m

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    GeV electrons from a centimeter LWFAa slide iven to me b S. Karsch

    310-m-diameterchannel ca illar

    P= 40 TW

    ensity 4.310 cm .

    Leemans et al., Nature Physics, september 2006 laser intensity 1018 W/cm2

    (emphasis by S. Karsch)

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    Table-top Brilliant Undulator X-ray Radiationfrom LWFA

    ( F. Gruener, S. Karsch, et al., Nature Phys., 2009)

    Observed undulatorradiation spectrum

    LWFA

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    Livingston Chart and Recent Saturation

    (Suzuki,

    20

    09)

    (http://tesla.desy.de/~rasmus/media/Accelerator%20physics/slides/Livingston%20Plot%202.html)

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    World Labgoal =

    Put SLACon a football field,

    Laser acceleration = no material breakdown ( 3/4 orders

    hi her radient however:

    (50GeV)

    3 orders finer accuracy, and2 orders more efficient laserneeded

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    Laser driven collider concept

    a TeV collider

    Leemans and Esarey (Phys. Today, 09)ICFA-ICUIL Joint Task Force on LaserAcceleration(Darmstadt,10)

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    15A. Suzuki (KEK)

    h igher energy

    h igher energy

    Le to enesisLe to enesis

    PeV Accelerator SUSY breakingSUSY breakingLaser

    Technology

    Dark matterDark matter

    SupersymmetrySupersymmetry

    1 TeV=101 TeV=101212 eVeV

    Standard model

    14

    HiggsHiggs

    QuarksQuarks

    Le tonsLe tons

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    Theory of wakefield toward extreme energy

    2 2 2 2 22 2 crn

    E m c a m c a

    (when 1D theory applies)en

    106

    107

    ) 1 TeV ,

    a0

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    -ray signal from primordial GRB

    (Abdo,

    Energy-dependent

    photon speed ?

    etal,

    20

    Gamma Ray Bursts (GRB)limit is ushed u

    )

    lo

    close to Planck mass)erenerg

    Lab PeV (from e-)

    y

    can explore thiswith control

    higher

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    Feel vacuum texture: PeV energy

    Laseracceleration controlled laboratory test to see quantum gravity texture

    on hoton ro a ation S ecial Theor of Relativit : c

    Coarser,ower energy

    texture

    Finer,

    hi her ener

    c < c0

    texture

    PeV (converted from e- )(1PeV : fs behind)

    . e

    1km

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    What is vacuum?

    crystal

    An observer (bug) in crystal

    looks at vacuum Phonon : excitation ofvacuum

    rong e rea s vacuum

    acuum roduces e+e- air vacuum

    =()=()(true)(nothing)

    Photon : distortion ofvacuum

    Strong laserfieldCompton lengthQED vacuum breakdown

    Laserwavelength(Naumova

    Mourou)

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    Intense laser probes matter /vacuum nonlinearity

    Crystal nonlinearity second harmonic generation (Franken et al)

    QED nonlinearityacuum non near y y g - mass

    field (dark energy, axion,..) second harmonic

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    QED vacuum probe by intense laser

    Heisenberg-Euler Langrangian: tiny nonlinearity, never observed

    intense laserneeded; sensitive probe, avoid blinding laser

    Phase contrast imaging(refractive index diffraction, noise reduction)

    with Homma Habs

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    Learning from laser parametric scattering:low ener meV - neV fields vacua

    Proposed scheme of co-parallel(with Homma, Habs)

    Many orders of magnitude gain

    sensitivity over long interaction:

    Nonlinearity ofvacuum

    cf. Brillouin forward scattering beat / opticalparametric excitation = phonon mediating

    (Nambu-Goldston boson)

    Mass of light fields(dark energy fields, axion-like fields) resonateswith specific crossing angle of co-propagating lasers

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    Scope ofScope of High Field ScienceHigh Field Science

    telescope

    llider

    co

    (with Homma, Habs)

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    Conclusions

    Laser: intensity sees no plateau/ceiling since 1990

    on near es o ma er y aser: non near op cs a om c or so

    nonlinearity) : Rutherford method vs Lasermethod

    Nonlinearity of relativistic plasma laserwakefield

    Laser wakefield acceleration: experimentally well established; unique

    properties getting known/applications spawn out

    e e ec rons; e soon; e wor a sugges e ;

    TeV lasercollider contemplated; PeV frontier (primordial GRBs in the lab)

    Vacuum nonlinearities: Heisenber ED vacuum robed b intense laserb

    phase contrast imaging

    Vacuum nonlinearities with weakly coupling light energy fields (meV- neV):

    - - ,

    dark energy fields

    High Fields Science: emerging, carves out new frontier, horizon yet to be

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    seen --------a second wave oflaserrevolution------------

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    Centaurus A:

    cosmic

    wakefield

    linac?

    Merci Beaucoup!