Author: Hastings, J.B.
Paper Title Page
TUOAI02
Hard X-ray Self-Seeding at the LCLS  
 
  • R.R. Lindberg, W. Berg, D. Shu, Yu. Shvyd'ko, S. Stoupin, E. Trakhtenberg, A. Zholents
    ANL, Argonne, USA
  • J.W. Amann, F.-J. Decker, Y.T. Ding, Y. Feng, J.C. Frisch, D. Fritz, J.B. Hastings, Z. Huang, J. Krzywinski, H. Loos, A.A. Lutman, H.-D. Nuhn, D.F. Ratner, J.A. Rzepiela, D.R. Walz, J.J. Welch, J. Wu, D. Zhu
    SLAC, Menlo Park, California, USA
  • V.D. Blank, S. Terentiev
    TISNCM, Troitsk, Russia
  • P. Emma
    LBNL, Berkeley, California, USA
  • S. Spampinati
    Elettra-Sincrotrone Trieste S.C.p.A., Basovizza, Italy
 
  Funding: U.S. Dept. of Energy Office of Sciences under Contract No. DE-AC02-06CH11357
The Linac Coherent Light Source (LCLS) has produced extremely bright hard x-ray pulses using self-amplified spontaneous emission (SASE) since 2009. In SASE, the electron beam shot noise initiates the FEL gain, resulting in output radiation characterized by poor temporal coherence and a fluctuating spectrum whose normalized width is given by the FEL bandwidth. Recently, colleagues at DESY suggested a self-seeding scheme for the LCLS to reduce the bandwidth*. Here, the SASE produced in the first half of the undulator line is put through a simple diamond-based monochromator; the resulting monochromatic light trailing the main SASE pulse is used to seed the FEL interaction in the downstream undulators. We report on the experimental results implementing such a scheme at the LCLS, in which we have measured a reduction in bandwidth by a factor of 40-50 from that of SASE at 8-9 keV. The self-seeded FEL operates close to saturation, with the maximum output energy approximately equal to that with no seeding for low charge. The observed level of power fluctuations in the seeded output is presently rather large, and future plans focus on discovering their origins and reducing their magnitude.
* Geloni, V. Kocharyan ,and E.L. Saldin, DESY 10-133, arXiv:1008.3036 (2010)
 
slides icon Slides TUOAI02 [22.104 MB]  
 
TUOB03
Complete Ultrafast X-ray Pulse Characterization at FELs  
 
  • A.L. Cavalieri, H. Bromberger, I. Grguras, S. Huber
    CFEL, Hamburg, Germany
  • C. Behrens, S. Düsterer, H. Schlarb
    DESY, Hamburg, Germany
  • C. Bostedt, J.D. Bozek, R.N. Coffee, Y.T. Ding, J.B. Hastings, M.C. Hoffmann, S. Schorb
    SLAC, Menlo Park, California, USA
  • J.T. Costello
    DCU, Dublin, Republic of Ireland
  • L.F. DiMauro
    Ohio State University, USA
  • G. Doumy
    ANL, Argonne, USA
  • W. Helml, R. Kienberger, A.R. Maier, W. Schweinberger
    MPQ, Garching, Munich, Germany
  • N.M. Kabachnik, T. Mazza, M. Meyer, T. Tschentscher
    XFEL. EU, Hamburg, Germany
  • A.K. Kazansky
    UPV-EHU, Leioa, Spain
 
  The ability to fully characterize X-ray pulses from free electron-lasers will underpin their exploitation in experiments ranging from single-molecule imaging to extreme timescale X-ray science. This issue is especially acute when confronted with the characteristics of current generation FELs operating on the principle of SASE, as most parameters fluctuate strongly from pulse to pulse. Here, we have extended the techniques of attosecond metrology with the use of single-cycle terahertz (THz) pulses, allowing for simultaneous, in-line, single-shot measurement of both the arrival time and temporal profile of FEL pulses on an absolute scale. The technique is non-invasive and could be incorporated in pump-probe experiments, eventually leading to characterization before and after interaction with most sample environments. Optical-laser-driven THz streaking measurements, revealing X-ray pulse structure shorter than 50 fs FWHM in the soft X-ray regime at FLASH and in the ~ keV range at LCLS will be discussed. With clear potential for improvement in resolution to the sub-10 fs regime, this method will ultimately allow for characterization of the shortest predicted few-femtosecond FEL pulses.  
slides icon Slides TUOB03 [15.857 MB]  
 
TUOB04 Comparison of Hard X-Ray Self-seeding with SASE after a Monochromator at LCLS 217
 
  • J.J. Welch, F.-J. Decker, J.B. Hastings, Z. Huang, A.A. Lutman, M. Messerschmidt, J.L. Turner
    SLAC, Menlo Park, California, USA
 
  Funding: ** Work supported in part by the DOE Contract DE-AC02-76SF00515.
Self-seeding of a hard x-ray FEL was demonstrated at LCLS in January 2012 and produced a factor of 40-50 bandwidth reduction using a electron bunch charge of 20-40 pC*. For many hard x-ray users, the photon intensity after a monochromator is an important performance parameter. In this paper, we report results from a subsequent study of self-seeding performance using the Si (111) K-monochromator with a full bandwidth of 1.2 eV at 8.2 keV. These include a direct comparison of the average intensity of the monochromatized seeded beam with that of a monochromatized fully tuned-up SASE beam, in both cases using 150 pC bunch charge. The intensity distribution, fluctuations, and spatial profiles of the monochromatized radiation are studied and compared.
* J. Amann, et. al, Nature Photonics, to be published
 
slides icon Slides TUOB04 [1.417 MB]  
 
TUOBI01 System Design for Self-Seeding the LCLS at Soft X-ray Energies 205
 
  • Y. Feng, J.W. Amann, D. Cocco, R.C. Field, J.B. Hastings, P.A. Heimann, Z. Huang, H. Loos, J.J. Welch, J. Wu
    SLAC, Menlo Park, California, USA
  • K. Chow, P. Emma, L. Rodes, R.W. Schoenlein
    LBNL, Berkeley, California, USA
 
  Funding: Portions of this research were carried out at the LCLS at the SLAC. LCLS is an Office of Science User Facility operated for the U.S. DOE Office of Science by Stanford University
The complete design for self-seeding the LCLS at soft X-ray energies from 400 to 1000 eV based on a grating monochromator is described. The X-ray optics system consists of a toroidal variable-line-space (VLS) grating with a resolving power greater than 5000 for creating a nearly transform-limited seed pulse from the upstream SASE undulator for pulse durations of the order of 25 fs, and focusing mirrors for imaging the seed pulse onto the downstream seeding undulator. Diagnostics for ensuring overlap with the reentrant electron beam are included in the design. The optical system is sufficiently compact to fit within a single 3.4 m LCLS undulator segment. The electron chicane system which serves to delay the electron beam to match the less than 1 ps delay from the optical system is similar to the chicane used in the hard X-ray self-seeding at LCLS. The seeded FEL pulse is expected to be nearly transform-limited with a bandwidth in the 10-4 range, potentially increasing the low-charge FEL X-ray peak brightness by 1-2 orders of magnitude.
 
slides icon Slides TUOBI01 [6.749 MB]