2015
DOI: 10.1088/1674-1137/39/1/017006
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Beam breakup simulation study for a high energy ERL

Abstract: Sen-Lin( ) 2;1) LIU Ke-Xin( ) 2;2) CHEN Jia-Er( ) 1,2

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Cited by 2 publications
(2 citation statements)
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“…4. For the ERL-LS, the design value of the average electron beam current is a few 10 mA, which is limited in the threshold current due to beam breakup caused by higher order modes (HOM-BBU) [29][30][31][32][33]. In order to increase the threshold current, the ERL-booster energy is designed to a few 10 MeV, which is larger than the other ERL projects [13,14].…”
Section: A Beam Energy and Currentmentioning
confidence: 99%
“…4. For the ERL-LS, the design value of the average electron beam current is a few 10 mA, which is limited in the threshold current due to beam breakup caused by higher order modes (HOM-BBU) [29][30][31][32][33]. In order to increase the threshold current, the ERL-booster energy is designed to a few 10 MeV, which is larger than the other ERL projects [13,14].…”
Section: A Beam Energy and Currentmentioning
confidence: 99%
“…Higher-order modes (HOMs) will be excited when electron beam passes through the radio-frequency (rf) cavity, which is one of the main causes of emittance dilution [1] and beam current limit in a superconducting rf (SRF) cavity [2][3][4]. For TESLA cavity, two coaxial type couplers are therefore installed on both ends of the cavity with a specific orientation to extract HOMs and transfer the power to the load [5].…”
Section: Introductionmentioning
confidence: 99%