Linac Coherent Light Source (LCLS) at 2--4 nm using the SLAC linac
Abstract
The authors describe the possible use of the SLAC linac to drive a unique, powerful, short wavelength Linac Coherent Light Source (LCLS). Using the FEL principle, lasing is achieved in a single pass of a high peak current electron beam through a long undulator by self-amplified-spontaneous-emission (SASE). The main components are a high-brightness electron RF gun with a photocathode, two electron bunch length compressors, the existing SLAC linac, beam diagnostics, and a long undulator combined with a FODO quadrupole focusing system. The RF gun, to be installed about 1 km from the end of the SLAC linac, would produce a single bunch of 6 x 10{sup 9} electrons with an invariant emittance of about 3 mm-mrad and a bunch length of about 500 {mu}m. That bunch is then accelerated to 100 MeV and compressed to a length of about 200 {mu}m. The main SLAC linac accelerates the bunch to 2 GeV were a second bunch compressor reduces the length to 30--40 {mu}m and produces a peak current of 2--3 kA. The bunch is then accelerated to 7--8 GeV and transported to a 50--70 m long undulator. Using electrons below 8 GeV, the undulator could operate at wavelengths down to 2more »
- Authors:
-
- Stanford Linear Accelerator Center, Menlo Park, CA (United States)
- Univ. of California, Los Angeles, CA (United States). Dept. of Physics
- Lawrence Livermore National Lab., CA (United States)
- Lawrence Berkeley Lab., CA (United States)
- Publication Date:
- Research Org.:
- Stanford Linear Accelerator Center, Menlo Park, CA (United States)
- Sponsoring Org.:
- USDOE, Washington, DC (United States)
- OSTI Identifier:
- 10114933
- Report Number(s):
- SLAC-PUB-6312; LBL-33456; CONF-930722-56
ON: DE94005235; TRN: AHC29402%%80
- DOE Contract Number:
- AC03-76SF00515
- Resource Type:
- Conference
- Resource Relation:
- Conference: Annual meeting of the Society of Photo-Optical Instrumentation Engineers (SPIE),San Diego, CA (United States),11-16 Jul 1993; Other Information: PBD: Aug 1993
- Country of Publication:
- United States
- Language:
- English
- Subject:
- 43 PARTICLE ACCELERATORS; 42 ENGINEERING; LINEAR ACCELERATORS; X-RAY LASERS; DESIGN; LIGHT SOURCES; FREE ELECTRON LASERS; ACCELERATOR FACILITIES; PERMANENT MAGNETS; BEAM DYNAMICS; 430100; 426002; DESIGN, DEVELOPMENT, AND OPERATION; LASERS AND MASERS
Citation Formats
Seeman, J T, Bane, K, Boyce, R, Loew, G, Morton, P, Nuhn, H D, Paterson, J, Pianetta, P, Raubenheimer, T, Tatchyn, R, Vylet, V, Winick, H, Pellegrini, C, Rosenzweig, J, Travish, G, Prosnitz, D, Scharlemann, E T, Halbach, K, Kim, K J, and Xie, M. Linac Coherent Light Source (LCLS) at 2--4 nm using the SLAC linac. United States: N. p., 1993.
Web.
Seeman, J T, Bane, K, Boyce, R, Loew, G, Morton, P, Nuhn, H D, Paterson, J, Pianetta, P, Raubenheimer, T, Tatchyn, R, Vylet, V, Winick, H, Pellegrini, C, Rosenzweig, J, Travish, G, Prosnitz, D, Scharlemann, E T, Halbach, K, Kim, K J, & Xie, M. Linac Coherent Light Source (LCLS) at 2--4 nm using the SLAC linac. United States.
Seeman, J T, Bane, K, Boyce, R, Loew, G, Morton, P, Nuhn, H D, Paterson, J, Pianetta, P, Raubenheimer, T, Tatchyn, R, Vylet, V, Winick, H, Pellegrini, C, Rosenzweig, J, Travish, G, Prosnitz, D, Scharlemann, E T, Halbach, K, Kim, K J, and Xie, M. Sun .
"Linac Coherent Light Source (LCLS) at 2--4 nm using the SLAC linac". United States. https://www.osti.gov/servlets/purl/10114933.
@article{osti_10114933,
title = {Linac Coherent Light Source (LCLS) at 2--4 nm using the SLAC linac},
author = {Seeman, J T and Bane, K and Boyce, R and Loew, G and Morton, P and Nuhn, H D and Paterson, J and Pianetta, P and Raubenheimer, T and Tatchyn, R and Vylet, V and Winick, H and Pellegrini, C and Rosenzweig, J and Travish, G and Prosnitz, D and Scharlemann, E T and Halbach, K and Kim, K J and Xie, M},
abstractNote = {The authors describe the possible use of the SLAC linac to drive a unique, powerful, short wavelength Linac Coherent Light Source (LCLS). Using the FEL principle, lasing is achieved in a single pass of a high peak current electron beam through a long undulator by self-amplified-spontaneous-emission (SASE). The main components are a high-brightness electron RF gun with a photocathode, two electron bunch length compressors, the existing SLAC linac, beam diagnostics, and a long undulator combined with a FODO quadrupole focusing system. The RF gun, to be installed about 1 km from the end of the SLAC linac, would produce a single bunch of 6 x 10{sup 9} electrons with an invariant emittance of about 3 mm-mrad and a bunch length of about 500 {mu}m. That bunch is then accelerated to 100 MeV and compressed to a length of about 200 {mu}m. The main SLAC linac accelerates the bunch to 2 GeV were a second bunch compressor reduces the length to 30--40 {mu}m and produces a peak current of 2--3 kA. The bunch is then accelerated to 7--8 GeV and transported to a 50--70 m long undulator. Using electrons below 8 GeV, the undulator could operate at wavelengths down to 2 nm, producing about 10 GW peak power in sub-ps light pulses. At a linac repetition rate of 120 Hz, the average power is about 1 W. Linac operation at lower beam energies provides longer wavelength radiation. After the undulator, the beam is deposited in a dump. The LCLS light pulses are then distributed to multiple user stations using grazing incident mirrors. Length compression, emittance control, phase stability, FEL design criteria, and parameter tolerances are discussed. A demonstration experiment is also described which uses the SLAC linac and (possibly) the PALADIN undulator to study SASE to power saturation at wavelengths of 40--360 nm.},
doi = {},
url = {https://www.osti.gov/biblio/10114933},
journal = {},
number = ,
volume = ,
place = {United States},
year = {1993},
month = {8}
}