Ciencias,UNAM

BLOCH ELECTRON DYNAMICS

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dc.contributor.author FUJITA, S
dc.contributor.author GODOY, S
dc.contributor.author NGUYEN, D
dc.date.accessioned 2011-01-22T10:28:19Z
dc.date.available 2011-01-22T10:28:19Z
dc.date.issued 1995
dc.identifier.issn 0015-9018
dc.identifier.uri http://hdl.handle.net/11154/3024
dc.description.abstract New equations of motion for a Bloch electron [momentum p = hk, energy epsilon( m(j) d upsilon(j)\d(t) = -e(E + v x B)(j) are proposed, where v = partial derivative epsilon(n)(p)/partial derivative p is the velocity, and {m(j)} are the principal masses m(j)(-1) = partial derivative(epsilon,n)(2)/partial derivative p(j)(2) along the normal and the two principal axes of curvatures at each point of the constant-energy surface represented by epsilon = epsilon(n)(p). Their advantages over the prevalent equations of motion where the left-hand-side is replaced by hk(j) are demonstrated by examining de Haas-van Alphen oscillations arm orientation-dependent cyclotron resonance peaks. en_US
dc.language.iso en en_US
dc.title BLOCH ELECTRON DYNAMICS en_US
dc.type Article en_US
dc.identifier.idprometeo 3153
dc.source.novolpages 25(8):1209-1220
dc.subject.wos Physics, Multidisciplinary
dc.description.index WoS: SCI, SSCI o AHCI
dc.relation.journal Foundations of Physics

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