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| 001 | 576801 | ||
| 005 | 20230227212421.0 | ||
| 037 | _ | _ | |a PUBDB-2023-00913 |
| 041 | _ | _ | |a English |
| 100 | 1 | _ | |0 P:(DE-H253)PIP1023917 |a Georgiev, Georgi |b 0 |
| 111 | 2 | _ | |a 40th International Free Electron Laser Conference |c Trieste |d 2022-08-22 - 2022-08-26 |g FEL2022 |w Italy |
| 245 | _ | _ | |a Simulations of Seeding Options for THz FEL at PITZ |
| 260 | _ | _ | |c 2022 |
| 336 | 7 | _ | |0 33 |2 EndNote |a Conference Paper |
| 336 | 7 | _ | |2 DataCite |a Other |
| 336 | 7 | _ | |2 BibTeX |a INPROCEEDINGS |
| 336 | 7 | _ | |2 DRIVER |a conferenceObject |
| 336 | 7 | _ | |2 ORCID |a LECTURE_SPEECH |
| 336 | 7 | _ | |0 PUB:(DE-HGF)6 |2 PUB:(DE-HGF) |a Conference Presentation |b conf |m conf |s 1677489821_25804 |
| 500 | _ | _ | |a Approved by PITZ CB JACoW Proceedings |
| 520 | _ | _ | |a A THz FEL is under commissioning at PITZ as a proof-of-principle experiment for a high power and high repetitionrate THz source and as an option for THz-driven experi-ments at the European XFEL. Some of these experimentsrequire excellent coherence and CEP stable THz pulses. InSASE regime, the coherent properties of the FEL radiationare limited. A seeding scheme can be used instead of SASEto improve the coherent properties and shot-to-shot stability.Several options for seeding are considered in simulation forthe THz FEL at PITZ: external laser pulse, pre-bunched elec-tron beam, energy modulated electron beam and additionalshort spike on top of a smooth beam profile. The improve-ments over SASE in energy, spectral and temporal stabilityof the THz pulse are presented. |
| 536 | _ | _ | |0 G:(DE-HGF)POF4-621 |a 621 - Accelerator Research and Development (POF4-621) |c POF4-621 |f POF IV |x 0 |
| 693 | _ | _ | |0 EXP:(DE-H253)PITZ-20150101 |5 EXP:(DE-H253)PITZ-20150101 |e Photo Injector Test Facility |x 0 |
| 700 | 1 | _ | |0 P:(DE-H253)PIP1019294 |a Boonpornprasert, Prach |b 1 |
| 700 | 1 | _ | |0 P:(DE-H253)PIP1004128 |a Krasilnikov, Mikhail |b 2 |
| 700 | 1 | _ | |0 P:(DE-H253)PIP1081485 |a Li, Xiangkun |b 3 |
| 700 | 1 | _ | |0 P:(DE-H253)PIP1032393 |a Hillert, Wolfgang |b 4 |
| 787 | 0 | _ | |0 PUBDB-2022-04414 |a Georgiev, Georgi et.al. |d 2022 |i IsMemberOf |t Simulations of Seeding Options for THz FEL at PITZ |
| 909 | C | O | |o oai:bib-pubdb1.desy.de:576801 |p VDB |
| 910 | 1 | _ | |0 I:(DE-588b)2008985-5 |6 P:(DE-H253)PIP1023917 |a Deutsches Elektronen-Synchrotron |b 0 |k DESY |
| 910 | 1 | _ | |0 I:(DE-HGF)0 |6 P:(DE-H253)PIP1023917 |a External Institute |b 0 |k Extern |
| 910 | 1 | _ | |0 I:(DE-588b)2008985-5 |6 P:(DE-H253)PIP1019294 |a Deutsches Elektronen-Synchrotron |b 1 |k DESY |
| 910 | 1 | _ | |0 I:(DE-588b)2008985-5 |6 P:(DE-H253)PIP1004128 |a Deutsches Elektronen-Synchrotron |b 2 |k DESY |
| 910 | 1 | _ | |0 I:(DE-588b)2008985-5 |6 P:(DE-H253)PIP1081485 |a Deutsches Elektronen-Synchrotron |b 3 |k DESY |
| 910 | 1 | _ | |0 I:(DE-H253)_CFEL-20120731 |6 P:(DE-H253)PIP1032393 |a Centre for Free-Electron Laser Science |b 4 |k CFEL |
| 910 | 1 | _ | |0 I:(DE-HGF)0 |6 P:(DE-H253)PIP1032393 |a External Institute |b 4 |k Extern |
| 913 | 1 | _ | |0 G:(DE-HGF)POF4-621 |1 G:(DE-HGF)POF4-620 |2 G:(DE-HGF)POF4-600 |3 G:(DE-HGF)POF4 |4 G:(DE-HGF)POF |a DE-HGF |b Forschungsbereich Materie |l Materie und Technologie |v Accelerator Research and Development |x 0 |
| 914 | 1 | _ | |y 2022 |
| 920 | 1 | _ | |0 I:(DE-H253)Z_PITZ-20210408 |k Z_PITZ |l Technologie |x 0 |
| 980 | _ | _ | |a conf |
| 980 | _ | _ | |a VDB |
| 980 | _ | _ | |a I:(DE-H253)Z_PITZ-20210408 |
| 980 | _ | _ | |a UNRESTRICTED |
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