High Harmonic Analysis Using a COLTRIMS Technique

Slides:



Advertisements
Similar presentations
Collisions inside subfemtoseconds laser pulsesPrague, November 4, 2002 Collisions inside subfemtosecond laser pulses L. Kocbach 1, L.B. Madsen 2 and J.P.
Advertisements

Intense Field Femtosecond Laser Interactions AMP TalkJune 2004 Ultrafast Laser Interactions with atoms, molecules, and ions Jarlath McKenna Supervisor:
Sub femtosecond K-shell excitation using Carrier Envelop Phase Stabilized 2-Cycles IR (2.1  m) Radiation Source. Gilad Marcus The Department of Applied.
Generation of short pulses
2. High-order harmonic generation in gases Attosecond pulse generation 1. Introduction to nonlinear optics.
Research Opportunities in Radiation-Induced Chemical Dynamics Scientific Opportunities for Studying Laser Excited Dynamics at the LCLS: David Bartels Notre.
X-ray Free-Electron Lasers: Challenges for Theory, Cambridge, Massachusetts, USA, June 19, 2006 Infrared X-ray pump-probe spectroscopy Hans Ågren Department.
Laser-induced vibrational motion through impulsive ionization Grad students: Li Fang, Brad Moser Funding : NSF-AMO October 19, 2007 University of New Mexico.
Photoelectron Spectroscopy Lecture 7 – instrumental details –Photon sources –Experimental resolution and sensitivity –Electron kinetic energy and resolution.
TOF Mass Spectrometer &
1 Femtosecond Time and Angle-Resolved Photoelectron Spectroscopy of Aqueous Solutions Toshinori Suzuki Kyoto University photoelectron.
Discussion of measurement methods for femtosecond and attosecond pulses.
High Harmonic Generation in Gases Muhammed Sayrac Texas A&M University.
Fragmentation mechanisms for Methane induced by electron impact
CLEO2004 K. L. Ishikawa No. 0 Enhancement in photoemission from He + by simultaneous irradiation of laser and soft x-ray pulses Kenichi L. Ishikawa Department.
Alvaro Sanchez Gonzalez Prof. Jon Marangos Prof. Jim Clarke
A. Doyuran, L. DiMauro, W. Graves, R. Heese, E. D. Johnson, S. Krinsky, H. Loos, J.B. Murphy, G. Rakowsky, J. Rose, T. Shaftan, B. Sheehy, Y. Shen, J.
Christina Dimopoulou Max-Planck-Institut für Kernphysik, Heidelberg IPHE, Université de Lausanne, Exploring atomic fragmentation with COLTRIMS.
Interaction of laser pulses with atoms and molecules and spectroscopic applications.
Femtosecond Laser Spectroscopy of C 60 Nieuwegein, The Netherlands August 21, 2001 Eleanor Campbell, Göteborg University & Chalmers, Sweden R.D. Levine,
“Design Of The Ion Extraction System In A Reaction Microscope” Speaker: Marco Panniello Federico II University Federico II University Industrial Engineering.
-Plasma can be produced when a laser ionizes gas molecules in a medium -Normally, ordinary gases are transparent to electromagnetic radiation. Why then.
Attosecond Physics Dawn Fraser University of Ottawa, Dec 2005 Dawn Fraser University of Ottawa, Dec 2005 Ultrafast Physics at a new Frontier.
1 Pengqian Wang Department of Physics Western Illinois University March 4, 2013.
Wave packet dynamics in atoms and molecules Eva Heesel Corinne Glendinning Helen Fielding Department of Chemistry University College London UCL Progress.
Ultrafast Laser Interactions with Atoms, Ions and Molecules
Precision spectroscopy of HCI in a reaction microscope Max-Planck-Institut für Kernphysik, Heidelberg C. Dimopoulou HITRAP Meeting, May 2005, Munich.
Intramolecular Energy Redistribution in C 60 M. Boyle, Max Born Institute.
Rydberg Series of C 60 Osnabrück, Germany March 2002 Eleanor Campbell, Göteborg University & Chalmers, Sweden R.D. Levine, Fritz Haber Center, Hebrew University.
Attosecond Optical Science V R. The key idea; F=ma Classically an atom’s own electron, driven by a strong electric field can interact with its parent.
Ionization in atomic and solid state physics. Paul Corkum Joint Attosecond Science Lab University of Ottawa and National Research Council of Canada Tunneling.
Time-Resolved X-ray Absorption Spectroscopy of Warm Dense Matter J.W. Lee 1,2,6, L.J. Bae 1,2, K. Engelhorn 3, B. Barbel 3, P. Heimann 4, Y. Ping 5, A.
Time-Resolved Photoemission Spectroscopy
The Electromagnetic Spectrum High Harmonic Generation
Modeling Auger processes DUE to high Intensity, ultrafast x-ray pulses
High Harmonic Generation from overdense plasma
Dissociation of Molecular Ions Studied by
B. D. Bruner1, H. Soifer1, C. Vozzi2, M. Negro3, M. Devetta3, S
Experiments at LCLS wavelength: 0.62 nm (2 keV)
Introduction to Synchrotron Radiation
ISMS 2016 Urbana, IL Vura-Weis Group - UIUC
“Electron cooling device in the project NESR (FAIR)"
Muhammed Sayrac Phys-689 Modern Atomic Physics Spring-2016
sub-femtosecond correlated dynamics probed with antiprotons
Mass Spectroscopy. Mass Spectroscopy Mass Spectrometry Most useful tool for molecular structure determination if you can get it into gas phase Molecular.
1. Ionization of molecules - ( MO-ADK theory)
Fragmentation Dynamics of H2+ / D2+ Kansas State University
Wavelength-dependence of Momentum-Space Images
Extreme Ultraviolet Radiation Spectrometer Design and Optimization
Instrumental Chemistry
Diatomic molecules
Xiao Min Tong and Chii Dong Lin
Peking University: Jinqing Yu, Ronghao Hu, Haiyang Lu & Xueqing Yan
Photoelectron diffraction from small molecules:
from W. Demtröder “Molecular Physics”
Electron Transfer in cluster Anions:
2D Momentum Spectra of the ATI Electrons by 10 fs Laser Pulses
P. Ranitiovic, I. Litvinuyk, and C.L. Cocke
T. L. Guasco, B. M. Elliott, M. Z. Kamrath and M. A. Johnson
Diagnosis of a High Harmonic Beam Using
Watching the Time Evolution of Wave-Packets in Diatomic Molecules
I. Bocharova L. Cocke, I. Litvinyuk, A. Alnaser, C. Maharjan, D. Ray
Strong field atomic ionization
AMO Early Science Capability
Recent Physics and Future Developments
from W. Demtröder “Molecular Physics”
Scientific goals of the instrument Status before the CR
Pump and probe technique
Image-potential States in Carbon Nanotubes
Few-body quantum dynamics in strong fields:
Presentation transcript:

High Harmonic Analysis Using a COLTRIMS Technique Ben Gramkow November 2, 2005

Pump-Probe Experiment Outline COLTRIMS High Harmonics Pump-Probe Experiment

Pump-Probe Experiment Outline COLTRIMS High Harmonics Pump-Probe Experiment

Magnetic Collection Field Target Jets Vacuum System COLTRIMS COLd Target Recoil-Ion Momentum Spectroscopy Spectrometer Detectors Magnetic Collection Field Target Jets Vacuum System

COLTRIMS Spectrometer & Detectors Point out spectrometer and detectors. Reaction products are directed toward detectors by spectrometer

Magnetic Collection Field Target Jets Vacuum System COLTRIMS COLd Target Recoil-Ion Momentum Spectroscopy Spectrometer Detectors Magnetic Collection Field Target Jets Vacuum System

COLTRIMS Spectrometer E-field

Magnetic Collection Field Target Jets Vacuum System COLTRIMS COLd Target Recoil-Ion Momentum Spectroscopy Spectrometer Detectors Magnetic Collection Field Target Jets Vacuum System

COLTRIMS Detectors

Magnetic Collection Field Target Jets Vacuum System COLTRIMS COLd Target Recoil-Ion Momentum Spectroscopy Spectrometer Detectors Magnetic Collection Field Target Jets Vacuum System

COLTRIMS Magnetic Collection Field

Magnetic Collection Field Target Jets Vacuum System COLTRIMS COLd Target Recoil-Ion Momentum Spectroscopy Spectrometer Detectors Magnetic Collection Field Target Jets Vacuum System

COLTRIMS Target Jet

Magnetic Collection Field Target Jets Vacuum System COLTRIMS COLd Target Recoil-Ion Momentum Spectroscopy Spectrometer Detectors Magnetic Collection Field Target Jets Vacuum System

COLTRIMS Vacuum System

COLTRIMS Vacuum System 0.44 torr 1.2x10-5 torr 2.7x10-8 torr

Pump-Probe Experiment Outline COLTRIMS High Harmonics Pump-Probe Experiment

High Harmonic Generation Three Step HHG Model Ionization Free Electron Motion Recombination High Harmonic Analysis Divergence Harmonic Content Flux

High Harmonic Generation Three Step HHG Model Ionization Free Electron Motion Recombination High Harmonic Analysis Divergence Harmonic Content Flux

High Harmonic Generation Ionization < 1014 W/cm2 1014 - 1015 W/cm2 > 1015 W/cm2 Multi-photon Processes (ATI) Tunneling Ionization Over the Barrier Ionization

High Harmonic Generation Three Step HHG Model Ionization Free Electron Motion Recombination High Harmonic Analysis Divergence Harmonic Content Flux

High Harmonic Generation Free Electron Motion

High Harmonic Generation Three Step HHG Model Ionization Free Electron Motion Recombination High Harmonic Analysis Divergence Harmonic Content Flux

High Harmonic Generation Recombination Two photons per optical cycle Doubled frequency separation

High Harmonic Generation Three Step HHG Model Ionization Free Electron Motion Recombination High Harmonic Analysis Divergence Harmonic Content Flux

High Harmonic Analysis Divergence

High Harmonic Analysis Divergence

High Harmonic Analysis Divergence

High Harmonic Generation Three Step HHG Model Ionization Free Electron Motion Recombination High Harmonic Analysis Divergence Harmonic Content Flux

High Harmonic Analysis Harmonic Content Energy [eV]

High Harmonic Analysis Time of Flight Spectra Electrons Recoil Ions Time of Flight [ns] Time of Flight [ns]

High Harmonic Analysis Wiggle Spectrum radius [mm/2] Time of Flight [ns] Time of Flight [ns]

High Harmonic Analysis Momentum Spectra Pz vs. Px [a.u.] Pz vs. Py [a.u.]

High Harmonic Analysis Photoelectron Energy Spectrum 23rd 25th 21st 19th Energy [eV]

High Harmonic Generation Three Step HHG Model Ionization Free Electron Motion Recombination High Harmonic Analysis Divergence Harmonic Content Flux

High Harmonic Analysis Flux Two orders of magnitude low We have not sought to maximize it.

Pump-Probe Experiment Outline COLTRIMS High Harmonics Pump-Probe Experiment

Pump-Probe Experiment Laser pump, x-ray probe Well-defined probe energy Valence Electrons Inner-Shell Electrons

Pump-Probe Experiment

Pump-Probe Experiment

Closing Remarks Our high harmonics can be examined with COLTRIMS. Our laser pulse duration and intensity lets follow the dynamics of the lightest molecules.

Equations and Parameters

Free Electron Motion Ekin, max = 3.17 Up

Harmonic Sources

Photoelectron Energy Spectrum Energy [eV]

Photoelectron Energy Spectrum Harmonic Order 11th 13th 15th 17th 19th 21st 23rd 25th Ehn [eV] 17.05 20.15 23.25 26.35 29.45 32.55 36.65 39.75 Ehn - Ip [eV] 1.35 4.45 7.55 10.65 13.75 16.85 19.95 23.05 p [a.u.] 0.31 0.57 0.74 0.88 1.01 1.11 1.21 1.3

Photoelectron Energy Spectrum 23rd 25th 21st 19th 11th 13th 15th 17th 19th 21st 23rd 25th Ehn [eV] 17.05 20.15 23.25 26.35 29.45 32.55 36.65 39.75 Ehn - Ip [eV] 1.35 4.45 7.55 10.65 13.75 16.85 19.95 23.05 p [a.u.] 0.31 0.57 0.74 0.88 1.01 1.11 1.21 1.3

Equations and Parameters