Author: Frisch, J.C.
Paper Title Page
TUOANO03
Bunch Profile Measurement of the LCLS Electron Beam via Mid-IR Spectroscopy  
 
  • T.J. Maxwell, Y. Ding, A.S. Fisher, J.C. Frisch, H. Loos
    SLAC, Menlo Park, California, USA
  • C. Behrens
    DESY, Hamburg, Germany
 
  Funding: Work supported by US Department of Energy contract number DE-AC02-76SF00515.
For the generation of ultrashort x-ray FEL pulses, a similarly short, high-brightness electron beam is needed with compression tuned to the extent that a narrow energy spread can still be preserved. Further reduction of the nominal LCLS bunch length by lowering the bunch charge or employing an upstream, emittance-spoiling foil promises to reduce the pulse duration to the level of only a few femtoseconds, presenting a challenge to the temporal resolution of existing longitudinal diagnostics. In answer to this, we have recently commissioned a single-shot, middle-infrared spectrometer for the LCLS. Developed as a robust and cost-effective alternative to other femtosecond-scale beam diagnostics, coherent mid-IR beam radiation measurements and analysis are then employed to probe the LCLS beam just prior to the undulator. Results resolving beam structure to the few-fs level for 20 - 150 pC beams will be presented. Practical design challenges and diagnostic limitations will also be discussed.
 
slides icon Slides TUOANO03 [2.337 MB]  
 
TUOBNO04
Femtosecond Electron and X-ray Beam Temporal Diagnostics Using an X-band Transverse Deflector at LCLS  
 
  • Y. Ding, C. Behrens, J.C. Frisch, Z. Huang, P. Krejcik, H. Loos, T.J. Maxwell, J.W. Wang, M.-H. Wang, J.J. Welch
    SLAC, Menlo Park, California, USA
  • C. Behrens
    DESY, Hamburg, Germany
 
  X-ray free-electron lasers provide ultrashort x-ray pulses for multidisciplinary users. Temporal characterization of these ultrashort pulses with a femtosecond precision remains a challenging topic. At the Linac Coherent Light Source (LCLS), an X-band radio-frequency transverse deflector proposed in 2011 [*] has just been installed and commissioning of the RF system has started. By measuring the electron beam longitudinal phase space between lasing and non-lasing conditions, both the e-beam and x-ray temporal profiles can be reconstructed. We report the latest progress of the commissioning of the deflector and the measurements on the e-beam and x-ray pulse length with this deflector at LCLS. The resolution, stability and operational performance will also be discussed.
[*] Y. Ding et al., Phys. Rev. ST Accel. Beams 14, 120701 (2011)
 
slides icon Slides TUOBNO04 [4.086 MB]  
 
WEPSO27 Recent LCLS Performance From 250 to 500 eV 554
 
  • R.H. Iverson, J. Arthur, U. Bergmann, C. Bostedt, J.D. Bozek, A. Brachmann, W.S. Colocho, F.-J. Decker, Y. Ding, Y. Feng, J.C. Frisch, J.N. Galayda, T. Galetto, Z. Huang, E.M. Kraft, J. Krzywinski, J.C. Liu, H. Loos, X.S. Mao, S.P. Moeller, H.-D. Nuhn, A.A. Prinz, D.F. Ratner, T.O. Raubenheimer, S.H. Rokni, W.F. Schlotter, P.M. Schuh, T.J. Smith, M. Stanek, P. Stefan, M.K. Sullivan, J.L. Turner, J.J. Turner, J.J. Welch, J. Wu, F. Zhou
    SLAC, Menlo Park, California, USA
  • P. Emma
    LBNL, Berkeley, California, USA
  • R. Soufli
    LLNL, Livermore, California, USA
 
  Funding: Work supported by US Department of Energy contract DE-AC02-76SF00515 and BES.
The Linac Coherent Light Source is an X-ray free-electron laser at the SLAC National Accelerator Laboratory. It produces coherent soft and hard X-rays with peak brightness nearly ten orders of magnitude beyond conventional synchrotron sources and a range of pulse durations from 500 to <10 fs. The facility has been operating at X-ray energy from 500 to 10,000eV. Users have expressed great interest in doing experiments with X-Rays near the carbon absorption edge at 284eV. We describe the operation and performance of the LCLS in the newly established regime between 250 and 500eV.
[1] Emma, P. et al., “First lasing and operation of an ˚angstrom-wavelength free-electron laser,” Nature Pho-
ton. 4(9), 641–647 (2010).
 
 
WEPSO37 Femtosecond Fiber Timing Distribution System for the Linac Coherent Light Source 583
 
  • H. Li, P.H. Bucksbaum, J.C. Frisch, A.R. Fry, J. May, K. Muehlig, S.R. Smith
    SLAC, Menlo Park, California, USA
  • L. Chen, H.P.H. Cheng
    Idesta Quantum Electronics, New Jersey, USA
  • F.X. Kaertner
    CFEL, Hamburg, Germany
  • F.X. Kaertner
    MIT, Cambridge, Massachusetts, USA
  • A. Uttamadoss
    PU, Princeton, New Jersey, USA
 
  Funding: This work is supported by Department of Energy under STTR grant DE-C0004702.
We present the design and progress of a femtosecond fiber timing distribution system for the Linac Coherent Light Source (LCLS) at SLAC to enable the machine diagnostic at the 10 fs level. The LCLS at the SLAC is the world’s first hard x-ray free-electron laser (FEL) with unprecedented peak brightness and pulse duration. The time-resolved optical/x-ray pump-probe experiments on this facility open the era of exploring the ultrafast dynamics of atoms, molecules, proteins, and condensed matter. However, the temporal resolution of current experiments is limited by the time jitter between the optical and x-ray pulses. Recently, sub-25 fs rms jitter is achieved from an x-ray/optical cross-correlator at the LCLS, and external seeding is expected to reduce the intrinsic timing jitter, which would enable full synchronization of the optical and x-ray pulses with sub-10 fs precision. Of such a technique, synchronization between seed and pump lasers would be implemented. Preliminary test results of the major components for a 4 link system will be presented. Currently, the system is geared towards diagnostics to study the various sources of jitter at the LCLS.
*P. Emma et al.,Nat. Photonics 4,641-647(2010).
*J. Kim et al.,Opt. Lett,, 31,3659(2006).
*J. Kim et al.,Opt. Lett,, 32,1044(2007).
*J.Kim et al.,Nat. Photonics 2,733-736(2008).