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dc.contributor.authorByung Joon Leeen_US
dc.contributor.authorIlmoon Hwangen_US
dc.contributor.authorChong do Parken_US
dc.contributor.authorChangbum Kimen_US
dc.contributor.authorSom Jai Chunjareanen_US
dc.date.accessioned2018-09-05T03:13:31Z-
dc.date.available2018-09-05T03:13:31Z-
dc.date.issued2016-09-01en_US
dc.identifier.issn19768524en_US
dc.identifier.issn03744884en_US
dc.identifier.other2-s2.0-84989338724en_US
dc.identifier.other10.3938/jkps.69.989en_US
dc.identifier.urihttps://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=84989338724&origin=inwarden_US
dc.identifier.urihttp://cmuir.cmu.ac.th/jspui/handle/6653943832/56299-
dc.description.abstract© 2016, The Korean Physical Society. The second-generation Pohang Light Source (PLS-II) has a 100-MeV pre-injector for the 3-GeV linac. A thermionic gun produces an electron charge of 200 pC with a bunch duration of 500 ps by using a 250-ps triggering pulser. At the pre-injector, one of the most important beam parameters for identifying the beam quality is the transverse emittance of electron bunches. Therefore, we measure the beam emittance and the Twiss functions at 100 MeV in order to match the beam optics to the beam transport line and go through it to the storage ring. To measure the transverse emittance, we used a well-known technique, the quadrupole scan, at the pre-injector. The emittances were 0.591 mm-mrad in the horizontal direction and 0.774 mm-mrad in the vertical direction.en_US
dc.subjectPhysics and Astronomyen_US
dc.titleBeam emittance measurement for the PLS-II linacen_US
dc.typeJournalen_US
article.title.sourcetitleJournal of the Korean Physical Societyen_US
article.volume69en_US
article.stream.affiliationsPohang University of Science and Technologyen_US
article.stream.affiliationsChiang Mai Universityen_US
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