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Expected properties of the radiation from VUV-FEL at DESY: femtosecond mode of operation
For the next three years the nominal "long pulse" (200 fs) mode of FEL operation at VUV-FEL, based on a linearized bunch compression, is not available due to the lack of a key element - a 3rd harmonic RF cavity. Essentially nonlinear compression leads naturally to a formation of a short hi...
Autores principales: | , , |
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Lenguaje: | eng |
Publicado: |
2004
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Acceso en línea: | http://cds.cern.ch/record/798233 |
_version_ | 1780904700798828544 |
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author | Saldin, E L Schneidmiller, E A Yurkov, M V |
author_facet | Saldin, E L Schneidmiller, E A Yurkov, M V |
author_sort | Saldin, E L |
collection | CERN |
description | For the next three years the nominal "long pulse" (200 fs) mode of FEL operation at VUV-FEL, based on a linearized bunch compression, is not available due to the lack of a key element - a 3rd harmonic RF cavity. Essentially nonlinear compression leads naturally to a formation of a short high-current leading peak (spike) in the density distribution that produces FEL radiation. Such a mode of operation was successfully tested at VUV-FEL, Phase I. In this paper we present optimized parameters of the beam formation system that allow us to get a current spike which is bright enough to get SASE saturation for the VUV-FEL, Phase 2 at shortest design wavelength down to 6 nm. The main feature of the considered mode of operation is the production of short (15-50 fs FWHM) radiation pulses with GW-level peak power that are attractive for many users. Main parameters of the SASE FEL radiation (temporal and spectral characteristics, intensity distributions, etc.) are presented, too. |
id | cern-798233 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2004 |
record_format | invenio |
spelling | cern-7982332019-09-30T06:29:59Zhttp://cds.cern.ch/record/798233engSaldin, E LSchneidmiller, E AYurkov, M VExpected properties of the radiation from VUV-FEL at DESY: femtosecond mode of operationAccelerators and Storage RingsFor the next three years the nominal "long pulse" (200 fs) mode of FEL operation at VUV-FEL, based on a linearized bunch compression, is not available due to the lack of a key element - a 3rd harmonic RF cavity. Essentially nonlinear compression leads naturally to a formation of a short high-current leading peak (spike) in the density distribution that produces FEL radiation. Such a mode of operation was successfully tested at VUV-FEL, Phase I. In this paper we present optimized parameters of the beam formation system that allow us to get a current spike which is bright enough to get SASE saturation for the VUV-FEL, Phase 2 at shortest design wavelength down to 6 nm. The main feature of the considered mode of operation is the production of short (15-50 fs FWHM) radiation pulses with GW-level peak power that are attractive for many users. Main parameters of the SASE FEL radiation (temporal and spectral characteristics, intensity distributions, etc.) are presented, too.DESY-TESLA-FEL-2004-06oai:cds.cern.ch:7982332004 |
spellingShingle | Accelerators and Storage Rings Saldin, E L Schneidmiller, E A Yurkov, M V Expected properties of the radiation from VUV-FEL at DESY: femtosecond mode of operation |
title | Expected properties of the radiation from VUV-FEL at DESY: femtosecond mode of operation |
title_full | Expected properties of the radiation from VUV-FEL at DESY: femtosecond mode of operation |
title_fullStr | Expected properties of the radiation from VUV-FEL at DESY: femtosecond mode of operation |
title_full_unstemmed | Expected properties of the radiation from VUV-FEL at DESY: femtosecond mode of operation |
title_short | Expected properties of the radiation from VUV-FEL at DESY: femtosecond mode of operation |
title_sort | expected properties of the radiation from vuv-fel at desy: femtosecond mode of operation |
topic | Accelerators and Storage Rings |
url | http://cds.cern.ch/record/798233 |
work_keys_str_mv | AT saldinel expectedpropertiesoftheradiationfromvuvfelatdesyfemtosecondmodeofoperation AT schneidmillerea expectedpropertiesoftheradiationfromvuvfelatdesyfemtosecondmodeofoperation AT yurkovmv expectedpropertiesoftheradiationfromvuvfelatdesyfemtosecondmodeofoperation |