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THz-pump and X-ray-probe sources based on an electron linac

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dc.contributor.authorSetiniyaz, Sadiq-
dc.contributor.authorPark, Seong Hee-
dc.contributor.authorKim, Hyun Woo-
dc.contributor.authorVinokurov, Nikolay A.-
dc.contributor.authorJang, Kyu-Ha-
dc.contributor.authorLee, Kitae-
dc.contributor.authorBaek, In Hyung-
dc.contributor.authorJeong, Young Uk-
dc.date.accessioned2021-09-02T23:49:29Z-
dc.date.available2021-09-02T23:49:29Z-
dc.date.created2021-06-19-
dc.date.issued2017-11-
dc.identifier.issn0034-6748-
dc.identifier.urihttps://scholar.korea.ac.kr/handle/2021.sw.korea/81758-
dc.description.abstractWe describe a compact THz-pump and X-ray-probe beamline, based on an electron linac, for ultrafast time-resolved diffraction applications. Two high-energy electron (gamma > 50) bunches, 5 ns apart, impinge upon a single-foil or multifoil radiator and generate THz radiation and X-rays simultaneously. The THz pulse from the first bunch is synchronized to the X-ray beam of the second bunch by using an adjustable optical delay of a THz pulse. The peak power of THz radiation from the multifoil radiator is estimated to be 0.14 GW for a 200 pC well-optimized electron bunch. GEANT4 simulations show that a carbon foil with a thickness of 0.5-1.0 mm has the highest yield of 10-20 keV hard X-rays for a 25 MeV beam, which is approximately 10(3) photons/(keV pC-electrons) within a few degrees of the polar angle. A carbon multifoil radiator with 35 foils (25 mu m thick each) can generate close to 10(3) hard X-rays/(keV pC-electrons) within a 2 degrees acceptance angle. With 200 pC charge and a 100 Hz repetition rate, we can generate 10(7) X-rays per 1 keV energy bin per second or 10(5) X-rays per 1 keV energy bin per pulse. The longitudinal time profile of an X-ray pulse ranges from 400 to 600 fs depending on the acceptance angle. The broadening of the time duration of an X-ray pulse is observed owing to its diverging effect. A double-crystal monochromator will be used to select and transport the desired X-rays to the sample. The heating of the radiators by an electron beam is negligible because of the low beam current. Published by AIP Publishing.-
dc.languageEnglish-
dc.language.isoen-
dc.publisherAMER INST PHYSICS-
dc.subjectTRANSITION RADIATION-
dc.subjectCRYSTAL-
dc.subjectCOEFFICIENTS-
dc.subjectATTENUATION-
dc.subjectBEAMLINE-
dc.subjectDESIGN-
dc.titleTHz-pump and X-ray-probe sources based on an electron linac-
dc.typeArticle-
dc.contributor.affiliatedAuthorPark, Seong Hee-
dc.identifier.doi10.1063/1.5006550-
dc.identifier.scopusid2-s2.0-85034609540-
dc.identifier.wosid000416780600022-
dc.identifier.bibliographicCitationREVIEW OF SCIENTIFIC INSTRUMENTS, v.88, no.11-
dc.relation.isPartOfREVIEW OF SCIENTIFIC INSTRUMENTS-
dc.citation.titleREVIEW OF SCIENTIFIC INSTRUMENTS-
dc.citation.volume88-
dc.citation.number11-
dc.type.rimsART-
dc.type.docTypeArticle-
dc.description.journalClass1-
dc.description.journalRegisteredClassscie-
dc.description.journalRegisteredClassscopus-
dc.relation.journalResearchAreaInstruments & Instrumentation-
dc.relation.journalResearchAreaPhysics-
dc.relation.journalWebOfScienceCategoryInstruments & Instrumentation-
dc.relation.journalWebOfScienceCategoryPhysics, Applied-
dc.subject.keywordPlusTRANSITION RADIATION-
dc.subject.keywordPlusCRYSTAL-
dc.subject.keywordPlusCOEFFICIENTS-
dc.subject.keywordPlusATTENUATION-
dc.subject.keywordPlusBEAMLINE-
dc.subject.keywordPlusDESIGN-
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