50 Years of the Laser in the City of Light
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Transcript of 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.
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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
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plasma
~ . mm
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(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
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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
23
seen --------a second wave oflaserrevolution------------
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Centaurus A:
cosmic
wakefield
linac?
Merci Beaucoup!