1 Efficient high order harmonic generation using quasi phase matching Sameh DABOUSSI Journées...

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1 Efficient high order harmonic generation using quasi phase matching Sameh DABOUSSI Journées scientifiques de L'EDOM 7 et 8 mars 2011

Transcript of 1 Efficient high order harmonic generation using quasi phase matching Sameh DABOUSSI Journées...

Page 1: 1 Efficient high order harmonic generation using quasi phase matching Sameh DABOUSSI Journées scientifiques de L'EDOM 7 et 8 mars 2011.

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Efficient high order harmonic generation using quasi phase matching 

Sameh DABOUSSI

Journées scientifiques de L'EDOM 7 et 8 mars 2011

Page 2: 1 Efficient high order harmonic generation using quasi phase matching Sameh DABOUSSI Journées scientifiques de L'EDOM 7 et 8 mars 2011.

2Presentation

Sameh DABOUSSI, PhD Student at :LPGP : Laboratoire de Physique des Gaz et des Plasmas : Gilles MAYNARD.ITFIP : Interaction et Transport de Faisceaux Intenses dans les Plasmas : Brigitte CROS.

I started my thesis in January 2010 !

Co-supervisors: Sophie KAZAMIAS and Brigitte CROS .

LASERIX : A facility of the University Paris Sud 11 attached to the research federation LUMAT (Lumière-Matière).Director : David ROS

Located In Bat P, ENSTA-Palaiseau.

Team Staff /Assistant professor : Sophie KAZAMIAS, Olivier GUILBAUD, Kevin CASSOU.Laser engineer : Moana PITTMAN.Electronics engineer : Olivier NEVEU.

Aim: Optimisation of a high order harmonic generation source using quasi-phase matching method.

Journées scientifiques de L'EDOM 7 et 8 mars 2011

Page 3: 1 Efficient high order harmonic generation using quasi phase matching Sameh DABOUSSI Journées scientifiques de L'EDOM 7 et 8 mars 2011.

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100 mJ – 40 fs – 10 Hz HHG : > 10 nm - 10 Hz

High repetition rate X-ray laser

CPA Ti:Sa

Laser System :

800nm 10Hz 3 J

HHG beam line HHG beam line

XUV laser Beam line

LASERIX, a Facility with a Large combination of XUV sources : LASERIX, a Facility with a Large combination of XUV sources :

Journées scientifiques de L'EDOM 7 et 8 mars 2011

Page 4: 1 Efficient high order harmonic generation using quasi phase matching Sameh DABOUSSI Journées scientifiques de L'EDOM 7 et 8 mars 2011.

4Gas cell orcapillary

Intense fs laser 1014 W/cm2LensIris

High-order harmonics

X-ray filter

Soft X-ray spectrometer

HHG beam line at LASERIX: HHG beam line at LASERIX:

Journées scientifiques de L'EDOM 7 et 8 mars 2011

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Microscopic effect : Three-step model of the intense laser pulse interaction with atoms

1- Strong electric field distorts Coulomb potential of atom.

2- Acceleration of free electron by the electric field : gained kinetic energy.

3- Recombination : high energy photon emission.

Principle of High-Order Harmonic Generation Principle of High-Order Harmonic Generation

2. Acceleration

3. Recombination

Laser field

Atomicpotential

1. Tunnelingelectron

Photon XUV

qEXUV= Ip + Ec

Journées scientifiques de L'EDOM 7 et 8 mars 2011

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Phase matching : Constructive addition of X-ray fieldsPhase matching : Constructive addition of X-ray fields

ktlcoh

)(

Laser fieldXUV emission

atmos

qq eE

Conversion efficiency: ~ 10-6 Science 280, 1412 (1998)

Destructive interference : lmed is an even multiple of lcoh

Constructive interference:

lmed is an odd multiple of lcoh

kkq Laserkq

0

Propagation in gaz medium

Journées scientifiques de L'EDOM 7 et 8 mars 2011

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Conversion efficiency >10-6

Science 302, 95 (2003)- Suppress the emissions from the out-of-phase range.- The HHG can add constructively and their amplitude increase

Quasi Phase Matching HHG from Gas mediumQuasi Phase Matching HHG from Gas medium

No absorption limitsHigh ionisation

Higher HHG orders

Journées scientifiques de L'EDOM 7 et 8 mars 2011

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Methods to achieve Quasi Phase MatchingMethods to achieve Quasi Phase Matching

-QPM via Pressure modulations.

-QPM via intensity modulations:

Method 1:Modulation of the inner diameter of the capillary

Method 2:Fundamental and higher order mode beating in a gas filled capillary tube (Adopted method) !

Expected Results :Conversion efficiency >10-6

Brightness ~1021 photons s-1mm-2mrad-2.

M.Zepf PRL 99, 143901 (2007)

150 μm

Journées scientifiques de L'EDOM 7 et 8 mars 2011

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9Harmonic order (q)

Experimental conditions :

Gaz cell : 8mmGaz : Néon E = 20 mJP= 20 mbar gaz cellλlaser= 800 nmPulse duration = 40 fs1 m foc length

High-Order Harmonic in gas cell at LASERIXHigh-Order Harmonic in gas cell at LASERIX

HHG characteristics :

•Harmonic order : 31 – 47•Wavelength : 17-27 nm•Energy per harmonic order : 10nJ•Pulse duration : 10fs

Journées scientifiques de L'EDOM 7 et 8 mars 2011

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Conclusions :

- The new high harmonic line is implemented at LASERIX-I performed numerical simulations using a 1D code of harmonic generation in a cell : Controversy about the new method of high harmonic generation called “XPA” (X-ray parametric amplification)

S. Kazamias, S. Daboussi, O. Guilbaud, K. Cassou, C. Montet, O. Neveu, D. Ros, B. Cros and G. Maynard, Nature Physics 6, 926 (2010).

Prospects :

- Optimisation of a high-order harmonic source in order to achieve a high energy, reliable and efficient HHG source.

- Generation of high order harmonic in Argon and Neon in Capillary tubes with QPM : experiments at LASERIX and comparison to simulation results (LPGP code).

Journées scientifiques de L'EDOM 7 et 8 mars 2011

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Thanks for attention

[email protected]://laserix.u-psud.fr

Journées scientifiques de L'EDOM 7 et 8 mars 2011