Observation of the polarization electric field in the intense neutralized proton beam propagating undeflectedly across a magnetic field
Author(s) -
Takashi Ikehata,
K. Kamada,
Hiroshi Ishizuka,
T. Kawabe,
S. Miyoshi
Publication year - 1982
Publication title -
physical review. a, general physics
Language(s) - English
Resource type - Journals
ISSN - 0556-2791
DOI - 10.1103/physreva.25.3415
Subject(s) - physics , polarization (electrochemistry) , magnetic field , electric field , beam (structure) , atomic physics , proton , nuclear physics , optics , quantum mechanics , chemistry
A neutralized proton beam (averaged velocity v=3.6×108 cm/s, velocity spread v=0.9×108 cm/s, proton current density 18 A/cm2) is injected into a transverse magnetic field B(3 kG). It is found that the electric field which satisfies the condition E=vB value is formed in the beam and the beam propagates across the magnetic field by the polarization drift when the dielectric constant =1+(pici)2 of the beam is larger than 100-180. The lowest value of for the beam propagation given above is consistent with the theoretical prediction 43. © 1982 The American Physical Society
Accelerating Research
Robert Robinson Avenue,
Oxford Science Park, Oxford
OX4 4GP, United Kingdom
Address
John Eccles HouseRobert Robinson Avenue,
Oxford Science Park, Oxford
OX4 4GP, United Kingdom