TY - GEN
T1 - Experimental study on low-velocity-spread axis-encircling electron beam
AU - Jeon, S. G.
AU - Baik, C. W.
AU - Kim, D. H.
AU - Jia, B.
AU - Park, G. S.
AU - Sato, N.
AU - Yokoo, K.
N1 - Publisher Copyright:
© 2003 IEEE.
PY - 2003
Y1 - 2003
N2 - In the theory proposed recently,1 ,2) the effect of small orbit gyration of electron beam before the magnetic cusp was investigated analyhcally and numerically. The small orbit gyration comes from the crossing of the electron beam and the magnetic flux line and it affects all characteristics of the electron beam such as the velocity ratio, the Lannor r d u s , the guiding center r d u s and the velocity spread. The physical model used in the analysis is shown in Fig. 1. In the drift region defined as [z1+z2] in Fig. 1, the electron beam is assumed to be in a small orbit gyro-motion that is caused by the crossing of the electron beam and the magnetic flux line in the diode region. The diode region is defined as the extent from the cathode to z, in Fig.1. Here, as shown in Fig.1, an ideal magnetic cusp is used for analyhcal calculation The radial position of the electron at the position of the mayetic cusp is given as Eq. (1).
AB - In the theory proposed recently,1 ,2) the effect of small orbit gyration of electron beam before the magnetic cusp was investigated analyhcally and numerically. The small orbit gyration comes from the crossing of the electron beam and the magnetic flux line and it affects all characteristics of the electron beam such as the velocity ratio, the Lannor r d u s , the guiding center r d u s and the velocity spread. The physical model used in the analysis is shown in Fig. 1. In the drift region defined as [z1+z2] in Fig. 1, the electron beam is assumed to be in a small orbit gyro-motion that is caused by the crossing of the electron beam and the magnetic flux line in the diode region. The diode region is defined as the extent from the cathode to z, in Fig.1. Here, as shown in Fig.1, an ideal magnetic cusp is used for analyhcal calculation The radial position of the electron at the position of the mayetic cusp is given as Eq. (1).
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U2 - 10.1109/IVEC.2003.1286323
DO - 10.1109/IVEC.2003.1286323
M3 - Conference contribution
AN - SCOPUS:79960605073
T3 - 4th IEEE International Vacuum Electronics Conference, IVEC 2003 - Proceedings
SP - 292
EP - 293
BT - 4th IEEE International Vacuum Electronics Conference, IVEC 2003 - Proceedings
PB - Institute of Electrical and Electronics Engineers Inc.
T2 - 4th IEEE International Vacuum Electronics Conference, IVEC 2003
Y2 - 28 May 2003 through 30 May 2003
ER -