AMO Early Science Capability AMO will be first

AMO Early Science Capability • AMO will be first experiment online @ LCLS • Planning for commissioning / first experiments in August 2009 • Adaptable to reality of source performance – i. e. planning for FEL and spontaneous source • Currently in final design phase (>50% of drawings complete) May 14, 2008 AMO Early Science Capability 1 John Bozek jdbozek@slac. stanford. edu

Scientific Goals of AMO Program Investigate multiphoton and high-field x-ray processes in atoms, molecules and clusters Multi-photon ionization/excitation in atoms/molecules/clusters Accessible intensity on verge of high-field regime Study time-resolved phenomena in atoms, molecules and clusters using ultrafast x-rays Inner-shell side band experiments Photoionization of aligned molecules Temporal evolution of state-prepared systems May 14, 2008 AMO Early Science Capability 2 John Bozek jdbozek@slac. stanford. edu

AMO studies fundamental interactions Through years of investigation, we have a pretty good idea what happens when we hit an atom with an x-ray? Consider Ne atoms and ~1 ke. V photons Photoabsorption Photoelectron Auger fluorescence May 14, 2008 AMO Early Science Capability 3 John Bozek jdbozek@slac. stanford. edu

AMO @ LCLS What happens when we illuminate atoms with high peak power of LCLS? ? ? Multiple ionization Multiphoton ionization Tunneling ionization Subsequent de-excitation dynamics May 14, 2008 AMO Early Science Capability 4 John Bozek jdbozek@slac. stanford. edu

AMO Instrumentation Pulse Picker Focusing optics High Field Physics Experiment Diagnostics Synchronized pulsed laser May 14, 2008 AMO Early Science Capability 5 John Bozek jdbozek@slac. stanford. edu

AMO Instrumentation - Schematic May 14, 2008 AMO Early Science Capability 6 John Bozek jdbozek@slac. stanford. edu

What’s there July 2009? Focusing Optics High Field Physics Chamber Pulsed gas jet Ion TOF (Wiley Mc. Laren type) Electron TOFs Diagnostics Effusive gas jet Magnetic bottle TOF Beam screens Synchronized Laser May 14, 2008 AMO Early Science Capability 7 John Bozek jdbozek@slac. stanford. edu

And what’s commissioned later ? Pulse picker (12/09) High Field Physics Chamber Velocity map imaging ion spectrometer (10/09) Momentum resolving ion spectrometer (reaction microscope/Col. TRIMS) (2/10) X-ray spectrometers (1/10) Diagnostics Pulse energy monitor (11/09) May 14, 2008 AMO Early Science Capability 8 John Bozek jdbozek@slac. stanford. edu

A little more detail – focusing optics Built by LBNL as a full assembly Focus in experimental chamber or diagnostics Focus beam to ~ 1 um diameter May 14, 2008 AMO Early Science Capability 9 John Bozek jdbozek@slac. stanford. edu

AMO Design – focusing optics Peak intensity depends on size of beam focus – accessible physics depends on intensity Focus W/cm 2 1 mm 7× 1012 100μm 7× 1014 LBNL mirror bender design 10 μm 7× 1016 1 μm 7× 1018 100 nm 7× 1020 May 14, 2008 AMO Early Science Capability 10 John Bozek jdbozek@slac. stanford. edu

Ne charge state vs Intensity Rohringer & Santra, PRA 76, 033416 (2007) May 14, 2008 AMO Early Science Capability 11 John Bozek jdbozek@slac. stanford. edu

Probable Ne Charge State with hv Rohringer & Santra, PRA 76, 033416 (2007) May 14, 2008 AMO Early Science Capability 12 John Bozek jdbozek@slac. stanford. edu

AMO Interaction region Five electron spectrometers & one ion spectrometer May 14, 2008 AMO Early Science Capability 13 John Bozek jdbozek@slac. stanford. edu

Xe ions as function of irradiance • Focused 93 e. V photons to 2. 6 um into ambient Xe • Collected ion signal by ion TOF A. A. Sorokin et al. , PRL 99, 213002 (2007) May 14, 2008 AMO Early Science Capability 14 John Bozek jdbozek@slac. stanford. edu

Multiphoton Photoelectron Spectroscopy Recent measurements of electrons from Ar clusters at FLASH show that direct multistep ionization of cluster creates higher charge states with short l radiation (38. 5 e. V) C. Bostedt, et al. , PRL 100, 133401 (2008). May 14, 2008 AMO Early Science Capability 15 John Bozek jdbozek@slac. stanford. edu

Diagnostics - Magnetic Bottle being designed (and possibly built) by Ohio State University under contract with Louis Di. Mauro Very high electron collection efficiency (~2 p) Useful as a measure of LCLS spectrum by converting hn to electron KE Also unique experimental capability May 14, 2008 AMO Early Science Capability 16 John Bozek jdbozek@slac. stanford. edu

5 W Nd: YVO 4 NEH Laser Pulse Stretcher 30 fs Mode Locked Ti: sapp @ 800 nm 30 fs Bandwidth 30 W Nd: YLF Pump Laser @ 527 nm 1. 2 k. Hz Regenerative Amplifier 1 k. Hz, <5 m. J Pulse Cleaner Laser Hall Optical Transport Hutch 2 Optical Transport Pulse Compressor (Single Grating) May 14, 2008 AMO Early Science Capability 17 Harmonics Optical Transport Experiment Chambers John Bozek jdbozek@slac. stanford. edu

Diagnostic - Temporal Resolution Two photons of different energy in interaction region at same time can result in multiphoton ionization (i. e. FLASH FEL & laser) Phenomenon provides a means to measure temporal overlap of two pulses – i. e. providing measure of temporal overlap between LCLS & laser Measured relative jitter between two beams of 250 fs using Xe 5 p photoionization P. Radcliffe et al, APL, 90, 131108, 2007. May 14, 2008 AMO Early Science Capability 18 John Bozek jdbozek@slac. stanford. edu

ISMS for the AMO Instrument Define scope of work Using LCLS design review process - documentation and reviews Analyze hazards Working with SLAC safety experts Prepared Preliminary Hazards Assessment Document (PHAD) for AMO instrument Develop and implement hazard controls With advice and review by SLAC safety committees Build the instrumentation Re-analyze hazards May 14, 2008 AMO Early Science Capability 19 John Bozek jdbozek@slac. stanford. edu

Unique Hazards Identified for AMO High pressure gas bottles (samples) connected to vacuum chamber Health hazard gases will be used in some experiments High power laser system with multiple wavelengths High magnetic field in magnetic bottle spectrometer Numerous high voltage supplies May 14, 2008 AMO Early Science Capability 20 John Bozek jdbozek@slac. stanford. edu

The Path Forward Preliminary Design Review Completed Finish detailing high field physics chamber, diagnostics Finalize Design & Review – June 08 Procurement phase – Jul-Dec 08 Assembly & Testing – Jan-Jun 09 Readiness review – July 09 Ready for first light – July 09 Thanks - lots of help from engineering, controls, etc. May 14, 2008 AMO Early Science Capability 21 John Bozek jdbozek@slac. stanford. edu

Commissioning vs First Experiments First experiments need only some of the instrumentation’s capability i. e. with focusing optics, gas jet & ion spectrometer could do multiphoton ionization expt. OR with magnetic bottle & laser could study temporal overlap with LCLS – (may even be possible without lasing) Managing commissioning vs experiment – pressure for both !! May 14, 2008 AMO Early Science Capability 22 John Bozek jdbozek@slac. stanford. edu

The End AMO Proposal Study Workshop – June 2 -3, 2008 @ SLAC http: //www-conf. slac. stanford. edu/amo/2008 May 14, 2008 AMO Early Science Capability 23 John Bozek jdbozek@slac. stanford. edu