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Two Colour and Two Photon Ionization Processes in Intense

EUV

and

Optical

Fields at F

LAS

H

John T. Costello

National Centre for Plasma Science & Technology (NCPST)/ School of Physical Sciences, Dublin City University www.physics.dcu.ie/~jtc

' F LAS H ' - Free Electron LAS er in H amburg

Ultrafast Imaging Workshop, Ischia May 3, 2009

Acknowledgements LIXAM (Orsay):

D. Cubaynes, M. Meyer

Universite Paris 06 (PMC):

R. Taieb, A. Maquet

DESY (Hamburg)

: A. Azima, S. D üsterer, P. Radcliffe, H. Redlin, W-B Li, J. Feldhaus

PTB (Berlin):

A. A. Sorokin, M. Richter

Moscow State University

: A. N. Grum-Grzhimailo, E. V. Gryzlova, S. I. Strakhova

Queen’s University Belfast:

Hugo van der Hart

Dublin City University:

J. Dardis, P. Hayden, P. Hough, T. Kelly, V. Richardson, E. T. Kennedy, J. T. Costello Thanks to AG Photon (R Treusch et al.) & AG Machine (M Yurkov et al.) Ultrafast Imaging Workshop, Ischia May 3, 2009

Collaboration - Origin

Collaboration grew out of EU RTD Project: HRPI-CT-1999-50009

Title: “X-Ray FEL Pump Probe Facility” Partners: Orsay, DCU, Lund, MBI, BESSY & DESY

Ultrafast Imaging Workshop, Ischia May 3, 2009

Outline of the Talk

FLASH (Brief) Overview

Atoms & Molecules in Intense EUV + NIR Fields

Coherent Photoionization Processes in Superposed Fields Optically probing fragments in EUV dissociated H 2

Two Photon Ionization in Intense EUV Fields

Next steps

Ultrafast Imaging Workshop, Ischia May 3, 2009

Part 1 - FLASH Overview

Ultrafast Imaging Workshop, Ischia May 3, 2009

FLASH Overview

RF-gun Diagnostics Accelerating Structures Laser 5 MeV Bunch Compressor 127 MeV Collimator Undulators Bunch Compressor 450 MeV 1000 MeV 300 m •

Energy range: ~ 0.3 – 1 GeV

~ 6.5 – 60 nm

Bypass FEL Diagnostics Ultrafast Imaging Workshop, Ischia May 3, 2009

FLASH: Key Performance Indicators Wavelength range (fundamental): water window

6 - 60 nm

FEL harmonics (@13.7 nm): 3 rd : 4.6 nm (270 eV) 5 rd : 2.7 nm (450 eV) Spectral width (FWHM): 0.5-1 % Pulse energy: up to 70 µJ (average), 170 µJ (peak) Pulse duration (FWHM): 10-50 fs Peak power (fundamental): Few GW Average power (fundamental): 0.1 W (up to 3000 pulses / sec) Photons per pulse: ~ 10 13

Ackermann et al., Nature Photonics

1

336 (2007)

O/P Profile and Spectral Distribution

FEL output builds up from spontaneous emission (photon noise) =>

SASE – ‘Self Amplified Spontaneous Emission’

Spectral Fluctuations Temporal Fluctuations Ultrafast Imaging Workshop, Ischia May 3, 2009

O/P Profile and Spectral Distribution

FEL output builds up from spontaneous emission (photon noise) =>

SASE – ‘Self Amplified Spontaneous Emission’

Raw EUV Spectrum Corrected EUV Spectrum Ultrafast Imaging Workshop, Ischia May 3, 2009

Part 2 - Experiments on dilute targets with FLASH

Motivations

1. ‘FLASH’ Characterisation 2. Demonstration Experiments 3. Future (Pathfinding)

Ultrafast Imaging Workshop, Ischia May 3, 2009

Atoms & Molecules in Intense EUV + Optical (800/400 nm) fields

1. Photoionization of rare gas atoms dressed by intense optical fields 2. Optical probing EUV dissociated H

2

Summary of AMOP@FLASH http://hasylab.desy.de/science/user_collaborations/amopflash Photoionization Experiments with the Ultrafast EUV Laser FLASH - Free Electron Laser in Hamburg J T Costello, J Phys Conf Ser

88

Art No 012057 (2007) C. Bostedt et al.,

Experiments at FLASH,

Nucl. Inst. Meth. in Res. A

601

108-122 (2009) Ultrafast Imaging Workshop, Ischia May 3, 2009

FLASH NIR/Vis and EUV Beam Layout

BL2 BL3 BL1 PG2 visible laser light

Ultrafast Imaging Workshop, Ischia May 3, 2009

Two colour ATI/ Laser Assisted PES

Superposition of visible and VUV pulses in a noble gas jet

Schins et al. PRL

73

, 2180 (1994)

Electron Spectrometer VUV Visible fs laser pulse

Sideband intensity very Sensitive to overlap

Ar(IP)

gas jet

E.S. Toma et al. PRA

62

061801 (2000)

h

w

ir =1.55eV

15.76 eV

Two colour ATI/ Laser Assisted PES

Experimental Layout at FLASH - (EU-RTD)

P. Radcliffe, et al., Nucl. Instr. and Meth. A

83

, 516-525 (2007)

Two colour ATI/ Laser Assisted PES

Sideband number/intensity depend strongly on EUV/NIR overlap  by comparison with theory

we are able to determine relative time delay to better than 100 fs

550 fs

1. New ultrafast EUV-modulated optical-reflectivity methods

C. Gahl et al., Nature Photonics

2

165-169 (2008) T. Maltezopoulos et al., New J Phys

10

Art. No. 033026 (2008)

2. ‘TEO’

A. Azima et al., APL.

(In Press 2009) P. Radcliffe, et al., Nucl. Instr. and Meth. A

83

, 516-525 (2007) P Radcliffe, et al., APL

90

131108 (2007)



Two colour ATI ‘Soft Photon’

‘n’ photon ATI cross-section 

d

d

  

k k

0

J n

2   

d

d

  

E k

One photon cross-section  

F

w

L

- Classical excursion vector of an electron in a laser field of amplitude

F K

    - Momentum transfer  After a little work………….sideband strength is given by an expression like……  

S

 0 

Sin

  1  

P

2 

Cos

  

J

2

n

  0

k n Cos

 

d

 J n Bessel function (first kind order ‘n’) k n - Shifted wavenumber of the ejected electron =  - Usual asymmetry parameter 2  w

IP

 w

FEL

n

w

L

  A Maquet and R Taieb, J. Mod. Opt.

54

1847 (2007)

Two colour ATI - Z Scaling

800 nm Ti-Sa 1.55 eV/ 120 fs FLASH h  ~ 93 eV 20  J/pulse

Two colour ATI - Z Scaling

Intesnity ratio of n= 1:2 sidebands - Model vs Experiment Experiment ‘Soft Photon’ Fitted 800 nm intensity ~ 5 x 10 11 W.cm

-2 Ultrafast Imaging Workshop, Ischia May 3, 2009

2 colour ATI - FEL Wavelength Scaling

 FEL + 800 nm . SB Ratio - Comparison of SPA with Experiment Ultrafast Imaging Workshop, Ischia May 3, 2009

2 colour ATI - Optical Intensity Scaling

Ne: Asymmetry in sideband distribution

S

  

Sin

  1  

P

2 

Cos

  

J n

2   0

k n Cos

 

d

 0  Ultrafast Imaging Workshop, Ischia May 3, 2009

2 colour ATI - Optical Intensity Scaling

Ne: ‘Toy’ SFA Code / Asymmetry in sideband distribution

S

  

Sin

  1  

P

2 

Cos

  

J n

2   0

k n Cos

 

d

 0 Ne: Simulation h  FEL = 46 eV 

Atomic Dichroism in Two colour ATI

Strong Polarisation Dependence of Sidebands (Low Field) FLASH: 13.7 nm, 10 20 fs, 20µJ OL: 800nm, 4ps, 400µJ, 6 x 10 11 W/cm 2

He 1s 2 He 1s 2 + h  XUV + h  XUV ----> He + + h  OL 1s + ---> He +  p 1s +  s,  d  Meyer et al., PRL

101

Art. no. 193002 (2008)

Atomic Dichroism in Two colour ATI - He Low Optical Laser Field High Optical Laser Field

 (  ) = 3S d S s /S d + (5S s =1.25 ± 0.3

+ S d ) cos 2 

P. Theory:

A Grum-Grzhimailo et al.

Meyer et al., PRL

101



S He



d

d

   

J n

2   

d

d

  

E k

0  

Sin

 

Cos

2  

J n

2   0

k n Cos

 

d

SPA:

A Maquet/ R Taieb

Atomic Dichroism in Two colour ATI - Kr

AD in TC-ATI: Ne, Kr, Xe: work in progress

FLASH: 13.7 nm, 10 20 fs, 20µJ OL: 800nm, 4ps, 6 x 10 11 W/cm 2

Ultrafast Imaging Workshop, Ischia May 3, 2009

Atomic Dichroism in 2 colour ATI - Ne +

Sequential Ionization

‘Work in progress’ - but we can begin to think about studying isonuclear trends…….

Ultrafast Imaging Workshop, Ischia May 3, 2009

Summary - Two Colour ATI

1. Demonstrated interference free SBs to high order, polarisation control, laser and FEL parameter dependencies & SBs in atomic and ionic targets 2. At low optical intensities 2nd OPT & SPA agree 3. Beyond He we really need to measure angular distributions to try to unravel the ‘l’ channels… 4. SPA works well at high intensities but the number of open high angular momentum channels is a challenge for other approaches such as R-Matrix Floquet (HvdH) 5. Is there really value in going beyond SPA here ? Does the residual ion core atomic structure really matter….?

Ultrafast Imaging Workshop, Ischia May 3, 2009

Optical Probing of H

2

Dissociation Demonstration Experiment

Ultrafast Imaging Workshop, Ischia May 3, 2009

Optical Probing of H

2 < 100 fs

Dissociation

1) H 2 + h  (FEL) --> H + H*

FEL : 13.7 nm, 90.5 eV h

VUV

2) H* + h  (las) --> H + + e -

Opt.Las. : 400 nm, 3.1 eV H + + H + H + + H(nl) H + + H(1s) H(1s) + H(1s)

Ultrafast Imaging Workshop, Ischia May 3, 2009

Optical Probing of H

2

Dissociation

13.7 nm (pump) + 400 nm (probe) High Intensity (1.5 mJ/120 fs) Low Intensity (0.5 mJ/120 fs) Ultrafast Imaging Workshop, Ischia May 3, 2009

Optical Probing of H

2

Dissociation

Dynamics - more to do - jitter limited.

expt.

fit

risetime = 500 fs

Ultrafast Imaging Workshop, Ischia May 3, 2009

Xe ionization in intense EUV fields

Ultrafast Imaging Workshop, Ischia May 3, 2009

4d two photon direct ionization

FEL only. h

~ 93 eV Xe + 2h

 

Xe + + e Replace PIS by MBES - First evidence of inner-shell TPI

Ultrafast Imaging Workshop, Ischia May 3, 2009

Part 3. Current and Future Interests

Two Colour

Resonant

Photoionization Processes 1. To date we have looked only at one and two colour

non-resonant

processes 2. Next phase - FEL tunable and so we can explore

resonant two colour

processes where inner shell electrons dominate Ultrafast Imaging Workshop, Ischia May 3, 2009

Kr (3d 9 4d) 2 Photon Resonance Auger

Kr + 3d 9 2 D 5/2

4d

92.0eV

Auger

Kr + 4p 4 4d, 5d ?

Expt. June 2009 (Hopefully) MLM - 3 degree incidence VUV 46.1 eV

Kr 3d 10 4s 2 4p 6 Ultrafast Imaging Workshop, Ischia May 3, 2009

Kr (3d 9 4d) DOR-Auger First Effort: Resonant Auger Spectrum

Kr + 3d 9 2 D 5/2

4d

5p 92.0eV

Auger

1.55 eV Kr + 4p 4 4d, 5d ?

XUV 13.9 nm FEL+las FEL 4s 4p SB

Kr 3d 10 4s 2 4p 6 TOF (ns)

Next Expt: eV) h

FEL (89 eV) + h

OL (3.1

Ultrafast Imaging Workshop, Ischia May 3, 2009

Experiments post-upgrade

Upgrade -

Optical Parametric Amplifier

- (fs OPA)

Laser coupling/spectroscopy of autoionization states 'Autler-Townes' meets ‘Codling-Madden’

Ultrafast Imaging Workshop, Ischia May 3, 2009

Tunable Optical Laser - Laser Coupling of autoionization states - 'Autler Townes' Autoionizing Resonances - He

Bachau & Lambropoulos, PRA (1986) Themelis, Lambropoulos, Meyer, JPB (2005) ‘New Knobs’ 1.

2.

Laser Frequency Laser Intensity Laser Coupled Autoionising State Dynamics Ultrafast Imaging Workshop, Ischia May 3, 2009

FLASH - Technical Developments OPA Upgrade Synchronisation Seeding with HHs -

0.01 - 1 mJ/ 0.1 - 20 ps New FIR Undulator (THz) Full coherence Stabilisation Synchroniosation Ultrafast Imaging Workshop, Ischia May 3, 2009

In Conclusion

1. To date we have looked only at one and two colour

non resonant

photoionization processes 2. Now -

FEL easily tunable

- we can explore

resonant two colour

processes where inner shell electrons dominate

3. Study fragmentation and ionization from vibrationally excited/selected wavepackets in simple molecules

4.

Beyond 2009: Seeding, fs jitter, angle resolved PES,…

5.

LCLS/XFEL/SPRING 8/NLS………..

Ultrafast Imaging Workshop, Ischia May 3, 2009