Beam emittance measurement for the PLS-II linac
© 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 imp...
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th-cmuir.6653943832-562992018-09-05T03:13:31Z Beam emittance measurement for the PLS-II linac Byung Joon Lee Ilmoon Hwang Chong do Park Changbum Kim Som Jai Chunjarean Physics and Astronomy © 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. 2018-09-05T03:13:31Z 2018-09-05T03:13:31Z 2016-09-01 Journal 19768524 03744884 2-s2.0-84989338724 10.3938/jkps.69.989 https://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=84989338724&origin=inward http://cmuir.cmu.ac.th/jspui/handle/6653943832/56299 |
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Physics and Astronomy Byung Joon Lee Ilmoon Hwang Chong do Park Changbum Kim Som Jai Chunjarean Beam emittance measurement for the PLS-II linac |
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© 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. |
format |
Journal |
author |
Byung Joon Lee Ilmoon Hwang Chong do Park Changbum Kim Som Jai Chunjarean |
author_facet |
Byung Joon Lee Ilmoon Hwang Chong do Park Changbum Kim Som Jai Chunjarean |
author_sort |
Byung Joon Lee |
title |
Beam emittance measurement for the PLS-II linac |
title_short |
Beam emittance measurement for the PLS-II linac |
title_full |
Beam emittance measurement for the PLS-II linac |
title_fullStr |
Beam emittance measurement for the PLS-II linac |
title_full_unstemmed |
Beam emittance measurement for the PLS-II linac |
title_sort |
beam emittance measurement for the pls-ii linac |
publishDate |
2018 |
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https://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=84989338724&origin=inward http://cmuir.cmu.ac.th/jspui/handle/6653943832/56299 |
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