chapter 7 -experimental methods of time-resolved ......chapter 7 -experimental methods of...
TRANSCRIPT
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Chapter7- ExperimentalMethodsofTime-ResolvedSpectroscopy
1. Generationoffemtosecondpulses2. Femtosecondpump-probeexperiments3. Generationofattosecond pulses4. Attosecond time-resolvedexperiments
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The hierarchy of time scales
1 millisec.10-3 s
1 microsec.10-6 s
1 nanosec.10-9 s
1 picosec.10-12 s
1 femtosec.10-15 s
1 attosec.10-18 s
vibrationsrotations electronmotionprotontransferproteinmotions
DE=1eV:T=h/DE=4.12fs
spontaneousIRemission
Fastestenzyme-catalyzedreactions
lifetimeofelectronically-excitedstates
FastestIVRHigh-frequency
vibrations
Fastestchemicalprocesses (e.g.e-transfer)
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A.H.Zewail,J.Phys.Chem.A,104,5660(2000)
A.H.Zewail,NobelLecture,1999
A.H.Zewail,NobelLecture,1999
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Generationofshortlaserpulses
Chirped-pulseamplificationKerr-lensmodelocking
2.7 fsl =800nm
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Q-switching:accesstonanoseconds
Q-switch
gain
med
ium
1) highlosses,lowQ-factor,nolasing2) Q-factorsuddenlyincreasedà powerbuildup3) powerreachessaturationà outputpowerdecays
www.rp-photonics.com
F. J. McClung and R. W. Hellwarth, Giant optical pulsations from ruby,Journal of Applied Physics 33, 1962, 828–829.
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Mode-locking:accesstofemtoseconds
L Trt
mod
ulator
gain
med
ium
Manysynchronizedmodesmakeupashortpulse.
SuperpositionofNmodes:www.rp-photonics.com
Themodulatorintroduceslosstocw (narrow-band)operationandfavorsmode-lockedoperation.
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Importanceofthespectralphase
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Experimentalrealizationofmode-locking
e.g.Kerr-lensmode-locking:
• Kerreffect:n=n0+n2I• Shortpulseà highintensityà self-focusing• Anapertureinthecavityfavorsmode-locked
operationovercontinuous-waveoperation:
Pulseduration~10fs,Fourierlimit8fs
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Chirped-pulseamplification
http://en.wikipedia.org
FromnJtomJpulsesandbeyond...
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ELI
©Johan Jarnestad/The Royal Swedish Academy of Sciences
Focu
sed
inte
nsity
(W/c
m2)
CPA
Towards ever higher intensities
Several methods were developed for emitting extremely powerful short laser pulses, but then development stopped – it was not possible to amplify the light pulses further without damaging the amplifying material.
The world’s first functioning laser was built by the American physicist Theodore Maiman.
Extreme Light Infrastructure (ELI) is a European project with three sites that will be completed in a few years.
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Pump-probe:averyoldideaAugustToepler (1836-1912):Schlierenphotographie 1864
1.lightflashgeneratessoundwave2.lightflashrecordsimage
explosion of 10 mg AgNO3,
3cm above ground
© H. Kleine
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TheopticaldelaylineAbrahamandLemoine 1899:
Dt
2 Dz = c Dt
object
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High-speedphotography
inventor: Harold Edgerton (1903-1990)
Time resolution = duration of light flash > 1 µs
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Femtosecondpump-probeexperimentsThefastestdetectorshavesub-nanosecondresponsetimeà fastereventscannotbemeasuredelectronically.
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Time-resolvedlaser-inducedfluorescence
lpump =310nmlprobe=580-620nm
Dtoven
NaI beamvacuumchamber
Measuresthelaser-inducedfluorescencesignal asafunctionofthepump-probedelay
lprobe =589nm
lprobe =612nmNa
(...)3s
(...)3p
589nm
Na-I
620nmLIF
M.Rosker,T.RoseandA.Zewail,Chem.Phys.Lett.146,175(1988)
LIF
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Time-resolvedlaser-inducedfluorescence
A.H.Zewail,J.Phys.Chem.A,104,5660(2000)
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Time-resolvedtransientabsorption
www.stfc.ac.uk
D.Polli etal.,Nature 467,440(2010)
Measurestheabsorptionspectrumoftheexcitedmolecules asafunctionofthepump-probedelay
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Time-resolvedphotoelectronspectroscopyMeasuresthekinetic-energydistributionofphotoelectronsasafunctionofthepump-probedelay
Lochbrunner etal.,J.Chem.Phys.114,2519(2001)
protontransfer
internalconversion
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Time-resolvedstrong-fieldionization
TSO =h/DESO :42.7fs (Ne+),23.2fs (Ar+)
Firstpulse:800nm,8fs,5x1014 W/cm2 ionizesNeà Ne+Secondpulse:800nm,8fs,5x1014 W/cm2 ionizesNe+à Ne2+
H.J.Wörner andP.B.Corkum,J.Phys.B44,041001(2011)A.Fleischeretal.,Phys.Rev.Lett.107,093004(2011)
Measuresthestrong-fieldionizationyield asafunctionofthepump-probedelay