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Limborg, C. G.

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Last Name: Limborg

Full Name: Limborg, C. G.

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2 papers

title: Start-to-End Simulations for the LCLS X-Ray Free-Electron Laser

format: conference procceeding

conference: 25th International Free Electron Laser Conference

year: 2003

7 authors: Sven Reiche | C. Pellegrini | P. Emma | Nuhn, H. D. | Limborg, C. G. | Borland, M. | W. Fawley

abstract: The LCLS Free-Electron Lasers operates in the wavelength range of 1.5-15 Angstrom, using an electron beam with an energy between 4.5 and 14.5 GeV. The generation of the electron beam, the preservation of its brightness during acceleration and compression, and the amplififcation of the spontaneous radiation within the FEL can only be described by a consistent set of simulation codes. We preset the change in the FEL performance with respect to the LCLS design case, when various effects are included, altering the electron beam distribution and motion (e.g. wake fields, CSR, magnet misalignment or field errors of the undulator field). To distinguish the individual contribution of each effect, multiple start-end simulations are performed, including step by step additional effects and, thus, approaching a more and more realistic model of the LCLS FEL.

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title: Photoinjector design for the LCLS

format: conference procceeding

conference: 23rd International Free Electron Laser Conference

year: 2002

16 authors: Bolton, P. R. | Clendenin, J. E. | Dowell, D. H. | M. Ferrario | Fisher, A. S. | Gierman, S. M. | Kirby, R. E. | P. Krejcik | Limborg, C. G. | Mulhollan, G. A. | D. Nguyen | D. T. Palmer | J. B. Rosenzweig | Schmerge, J. F. | L. Serafini | X. J. Wang

abstract: The design of the Linac Coherent Light Source assumes that a low-emittance, 1 nC, 10 ps beam will be available for injection into the 15 GeV linac. The proposed RF photocathode injector that will meet this requirement is based on a 1.6-cell S-band RF gun equipped with an emittance-compensating solenoid. The booster accelerator with a gradient of 25 MV/m is positioned at the beam waist coinciding with the first emittance maximum, i.e., the "new working point." The UV pulses required for cathode excitation will be generated by tripling the output of a Ti:sapphire laser system. Details of the design and the supporting simulations are presented. (12 References).

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title:	Start-to-End Simulations for the LCLS X-Ray Free-Electron Laser
format:	conference procceeding
conference:	25th International Free Electron Laser Conference
year:	2003
7 authors:	Sven Reiche \| C. Pellegrini \| P. Emma \| Nuhn, H. D. \| Limborg, C. G. \| Borland, M. \| W. Fawley
abstract:	The LCLS Free-Electron Lasers operates in the wavelength range of 1.5-15 Angstrom, using an electron beam with an energy between 4.5 and 14.5 GeV. The generation of the electron beam, the preservation of its brightness during acceleration and compression, and the amplififcation of the spontaneous radiation within the FEL can only be described by a consistent set of simulation codes. We preset the change in the FEL performance with respect to the LCLS design case, when various effects are included, altering the electron beam distribution and motion (e.g. wake fields, CSR, magnet misalignment or field errors of the undulator field). To distinguish the individual contribution of each effect, multiple start-end simulations are performed, including step by step additional effects and, thus, approaching a more and more realistic model of the LCLS FEL.
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title:	Photoinjector design for the LCLS
format:	conference procceeding
conference:	23rd International Free Electron Laser Conference
year:	2002
16 authors:	Bolton, P. R. \| Clendenin, J. E. \| Dowell, D. H. \| M. Ferrario \| Fisher, A. S. \| Gierman, S. M. \| Kirby, R. E. \| P. Krejcik \| Limborg, C. G. \| Mulhollan, G. A. \| D. Nguyen \| D. T. Palmer \| J. B. Rosenzweig \| Schmerge, J. F. \| L. Serafini \| X. J. Wang
abstract:	The design of the Linac Coherent Light Source assumes that a low-emittance, 1 nC, 10 ps beam will be available for injection into the 15 GeV linac. The proposed RF photocathode injector that will meet this requirement is based on a 1.6-cell S-band RF gun equipped with an emittance-compensating solenoid. The booster accelerator with a gradient of 25 MV/m is positioned at the beam waist coinciding with the first emittance maximum, i.e., the "new working point." The UV pulses required for cathode excitation will be generated by tripling the output of a Ti:sapphire laser system. Details of the design and the supporting simulations are presented. (12 References).
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