A 2-4 nm Linac Coherent Light Source (LCLS) using the SLAC linac
We describe the use of the SLAC linac to drive a unique, powerful, short wavelength Linac Coherent Light Source (LCLS). Operating as an FEL, lasing would be achieved in a single pass of a high peak current electron beam through a long undulator by self-amplified spontaneous emission. The main compon...
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Published in: | Proceedings of International Conference on Particle Accelerators pp. 1445 - 1447 vol.2 |
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Main Authors: | , , , , , , , , , , , , , , , , , , , |
Format: | Conference Proceeding |
Language: | English |
Published: |
IEEE
1993
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Subjects: | |
Online Access: | Get full text |
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Summary: | We describe the use of the SLAC linac to drive a unique, powerful, short wavelength Linac Coherent Light Source (LCLS). Operating as an FEL, lasing would be achieved in a single pass of a high peak current electron beam through a long undulator by self-amplified spontaneous emission. The main components are a high-brightness rf photocathode electron gun; pulse compressors; about 1/5 of the SLAC linac; and a long undulator with a FODO quadrupole focusing system. Using electrons below 8 GeV, the system would operate at wavelengths down to about 3 nm, producing /spl ges/10 GW of peak power in sub-ps pulses. At a 120 Hz rate the average power is /spl ap/1 W.< > |
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ISBN: | 9780780312036 0780312031 |
DOI: | 10.1109/PAC.1993.308574 |