1996
DOI: 10.1103/physrevb.54.5334
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Magnetic-electric two-dimensional Euclidean group

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Cited by 5 publications
(3 citation statements)
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“…The dual problem corresponds to a simultaneous reverse in the directions of B and E. We notice that the commutators in the second line of Eq. (8) are part of the Lie algebra of the EM-Galilean two dimensional group [24,25]. This group is obtained when the usual rotation and boost operators of the planar-Galilean group are replaced by their electric-magnetic generalization in which the operators are enlarged by the effect of a gauge transformation.…”
Section: Electric Evolution and Magnetic Translationsmentioning
confidence: 99%
“…The dual problem corresponds to a simultaneous reverse in the directions of B and E. We notice that the commutators in the second line of Eq. (8) are part of the Lie algebra of the EM-Galilean two dimensional group [24,25]. This group is obtained when the usual rotation and boost operators of the planar-Galilean group are replaced by their electric-magnetic generalization in which the operators are enlarged by the effect of a gauge transformation.…”
Section: Electric Evolution and Magnetic Translationsmentioning
confidence: 99%
“…The commutators in the second line of Eq. ( 6) are part of the more general Lie algebra of the magnetic-electric Euclidean two dimensional group [8]. Schrödinger's equation and the symmetry operators are expressed in terms of covariant derivatives π µ and O µ , respectively.…”
mentioning
confidence: 99%
“…Hence, the meaning of ( 9) is that the ratio of the Stark ladder spacing (bE) to the Brillouin zone for the quasienergy (2πv d /b) is given by the rational number φ = p/q. We henceforth consider that the three conditions ( 7), (8), and (9) hold simultaneously. In this case the three EMB operators: the electric evolution T 0 ≡ T 0 (τ 0 ) and the magnetic translations T L ≡ T L (qb), and T T ≡ T T (b) form a set of mutually commuting symmetry operators.…”
mentioning
confidence: 99%