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DC Field | Value | Language |
---|---|---|
dc.contributor.author | S. Sukara | en_US |
dc.contributor.author | H. Ohgaki | en_US |
dc.contributor.author | S. Rimjaem | en_US |
dc.date.accessioned | 2022-10-16T07:29:29Z | - |
dc.date.available | 2022-10-16T07:29:29Z | - |
dc.date.issued | 2021-01-28 | en_US |
dc.identifier.issn | 17426596 | en_US |
dc.identifier.issn | 17426588 | en_US |
dc.identifier.other | 2-s2.0-85100781198 | en_US |
dc.identifier.other | 10.1088/1742-6596/1719/1/012003 | en_US |
dc.identifier.uri | https://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=85100781198&origin=inward | en_US |
dc.identifier.uri | http://cmuir.cmu.ac.th/jspui/handle/6653943832/77377 | - |
dc.description.abstract | At the PBP-CMU Electron Linac Laboratory, the existing linear accelerator system is under developing to produce electron beams with suitable properties for generation of oscillator mid-infrared free-electron laser (MIR-FEL) and super-radiant terahertz (THz) undulator radiation. This work focuses on the simulation of the oscillator MIR-FEL with expected electron beam energy of 20 - 25 MeV to evaluate the required electron beam parameters. To achieve FEL saturation, the single-pass FEL simulation using the code GENESIS 1.3 was performed to estimate the laser wavelength, FEL gain and electron macro-pulse duration. In the simulation, electron beams with energy spread of 0, 0.5 and 1.0 %, and the electron peak current of 25 and 50 A were considered. As a result, the electron beam with energy of 20 - 25 MeV can produce the FEL wavelengths of 13.5 - 21.2 µm using a 1.6-m undulator with maximum undulator parameter of 1.07. The largest FEL gain is 216% when using electron beam energy and peak current of 20 ± 0% MeV and 50 A, which requires the electron macro-pulse duration of 1.6 µs to saturate FEL. Due to the possible macro-pulse duration at our facility of 6 µs, the operation of electron beam with energy spread of 0.5% and peak current of higher than 25 A is required to saturate FEL. Results from this single-pass simulation can be used as a based information for further practical consideration with multi-pass simulation. | en_US |
dc.subject | Physics and Astronomy | en_US |
dc.title | Investigation of electron energy spread effects on the intracavity MIR-FEL power at the PBP-CMU electron linac laboratory | en_US |
dc.type | Conference Proceeding | en_US |
article.title.sourcetitle | Journal of Physics: Conference Series | en_US |
article.volume | 1719 | en_US |
article.stream.affiliations | Kyoto University | en_US |
article.stream.affiliations | Chiang Mai University | en_US |
article.stream.affiliations | Science | en_US |
Appears in Collections: | CMUL: Journal Articles |
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