Autonomous beam buncher for ECM applications

Vomvoridis, JL; Frantzeskakis, DJ; Hizanidis, K

dc.contributor.author	Vomvoridis, JL	en
dc.contributor.author	Frantzeskakis, DJ	en
dc.contributor.author	Hizanidis, K	en
dc.date.accessioned	2014-03-01T02:48:07Z
dc.date.available	2014-03-01T02:48:07Z
dc.date.issued	1992	en
dc.identifier.issn	0277786X	en
dc.identifier.uri	https://dspace.lib.ntua.gr/xmlui/handle/123456789/33539
dc.relation.uri	http://www.scopus.com/inward/record.url?eid=2-s2.0-0027000249&partnerID=40&md5=ce3ebeecbba7858d2fd032ae90ffa8ce	en
dc.subject.other	Cyclotron resonance	en
dc.subject.other	Cyclotrons	en
dc.subject.other	Guided electromagnetic wave propagation	en
dc.subject.other	Magnetostatics	en
dc.subject.other	Autonomous beach bunchers	en
dc.subject.other	Axial velocity electron beams	en
dc.subject.other	Beam bunching	en
dc.subject.other	Electron beams	en
dc.title	Autonomous beam buncher for ECM applications	en
heal.type	conferenceItem	en
heal.publicationDate	1992	en
heal.abstract	The authors investigate the potential of an axial velocity electron beam to generate slow waves and to become azimuthally bunched. The electron beam is considered to be initially unmodulated, monoenergetic, with no initial transverse velocity of each constituent electron, infinitesimally thin and at low current. The electrons are acted upon by a guided mode, under conditions of cyclotron resonance. The nonlinear dynamics of the electron beam is described by means of the equations of motion, which have been found to be integrable since they exhibit two integrals of motion. The first invariant gives the conditions for the beam voltage to decrease below its initial value.	en
heal.publisher	Publ by Society of Photo-Optical Instrumentation Engineers, Bellingham, WA, United States	en
heal.journalName	Proceedings of SPIE - The International Society for Optical Engineering	en
dc.identifier.volume	1929	en
dc.identifier.spage	270	en
dc.identifier.epage	271	en