Author: Wu, J.
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]  
 
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]  
 
TUPD07 Generation of Longitudinally Coherent Ultra High Power X-Ray FEL Pulses by Phase and Amplitude Mixing 237
 
  • J. Wu, C. Pellegrini
    SLAC, Menlo Park, California, USA
  • A. Marinelli
    UCLA, Los Angeles, California, USA
 
  Funding: Work supported by U.S. Department of Energy, Office of Basic Energy Sciences, under Contract DE-AC02-76SF00515.
We study an improved-SASE (iSASE) scheme to generate narrow bandwidth Free Electron Laser (FEL) by introducing phase shifter between the undulator segments to speed up the slippage. Due to the shift of the FEL pulse with respect to the electron bunch, spikes with phase relation develop; therefore the coherent length increases faster. Furthermore, due to the similarity of these spikes in the temporal domain with respect to the spikes generated in the previous sections, the spectrum of such an FEL containing a regular temporal spike train is intrinsically narrower than that of a conventional SASE FEL. Here, we report study results for a soft x-ray FEL at 6 nm and a hard x-ray at 0.15 nm. With a narrower bandwidth, the FEL responds to a tapered undulator more efficiently than a conventional SASE FEL does. This then make it possible to reach high power. Analysis is carried out with GENESIS numerical simulation as well as 1-D analytical calculation.
 
 
TUPD08 Tolerances for a Seeded Free Electron Laser 241
 
  • J. Wu, T.O. Raubenheimer
    SLAC, Menlo Park, California, USA
 
  Funding: Work supported by U.S. Department of Energy, Office of Basic Energy Sciences, under Contract DE-AC02-76SF00515.
Tolerance and stability are important issues for designing and operating accelerator and FEL. Jitter can come from various sources. We identify and study well known sources as well as some particular ones, important for a seeded tapered high power FEL. Seed laser phase error, electron bunch current profile, self-seeding residual density bunching and energy modulation after the chicane, undulator wakefield, and phase errors in the undulator breaks are just a few important examples. Schemes to improve the stability of a seeded FEL are also discussed.
 
 
WEPD51 The parameter study of terahertz Free-Electron Laser Oscillator based on Electrostatic Accelerator 488
 
  • A.L. Wu, Q.K. Jia
    USTC/NSRL, Hefei, Anhui, People's Republic of China
  • F.W. Wang, J. Wu
    SLAC, Menlo Park, California, USA
 
  Free-Electron Laser Oscillator based on Electrostatic Accelerator (EA-FELO) is one of the best methods to realize the powerful terahertz source, which can not only produce high power, but also obtain coherent and tunable wavelength. In this paper, we investigate the effects of the main parameters in this scheme, including the initial electron-beam energy spread, emittance and beam current. Besides, the influence of the radius of the mirrors and the position of the undulator on FEL performance is also studied. The numerical results from 1D FEL Oscillator simulation code FELO are presented, and show that this compact device could achieve the terahertz light with the peak output power is about 5.3kW.  
 
THOC04
Femtosecond X-ray Pulse Duration and Separation Measurement using a Cross-Correlation Technique  
 
  • Y.T. Ding, F.-J. Decker, Z. Huang, H. Loos, J.J. Welch, J. Wu, F. Zhou
    SLAC, Menlo Park, California, USA
  • P. Emma
    LBNL, Berkeley, California, USA
  • C. Feng
    SINAP, Shanghai, People's Republic of China
 
  At the Linac Coherent Light Source (LCLS), the emittance-spoiling foil is a very simple and effective method to control the output x-ray pulse duration [*]. In addition, double slotted foil can be used to generate two femotsecond x-ray pulses with variable time delays. In this paper, we report the first measurement of x-ray pulse duration and double x-ray pulse separation by using a cross-correlation technique between x-rays and electrons [**]. The measured pulse separation can be used to calibrate the foil setup, and pulse duration of less than 3 fs rms has been achieved. This technique can be used to provide critical temporal diagnostics for x-ray experiments that employ the emittance-spoiling foil.
[*] P. Emma et al., PRL 92, 074801 (2004).
[**] G. Geloni et al., DESY 10-008.
 
slides icon Slides THOC04 [0.684 MB]