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書目名稱Group Theoretical Methods in Physics影響因子(影響力)




書目名稱Group Theoretical Methods in Physics影響因子(影響力)學(xué)科排名




書目名稱Group Theoretical Methods in Physics網(wǎng)絡(luò)公開度




書目名稱Group Theoretical Methods in Physics網(wǎng)絡(luò)公開度學(xué)科排名




書目名稱Group Theoretical Methods in Physics被引頻次




書目名稱Group Theoretical Methods in Physics被引頻次學(xué)科排名




書目名稱Group Theoretical Methods in Physics年度引用




書目名稱Group Theoretical Methods in Physics年度引用學(xué)科排名




書目名稱Group Theoretical Methods in Physics讀者反饋




書目名稱Group Theoretical Methods in Physics讀者反饋學(xué)科排名

北京人起源

Chang Samuel Hsu,Paul R. Robinsonvery useful information on the admissible equations of motion and on the group theoretical concept of an elementary particle (which is defined as an irreducible quantum-mechanical system obeying such an equation). Here we consider the case where an external (classical) e.m. field is present. In this

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impaction

constitutional

Wave equations for extended hadrons,tural group of the bundle is taken to be the (4+1) de Sitter group acting as a group of motion in a locally defined space of constant curvature [the fiber] possessing a radius of curvature of the order of one Fermi. A gauge theory of strong interaction is formulated in terms of the geometry in such

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Covariance principle and covariance group in presence of external E.M. Fields,very useful information on the admissible equations of motion and on the group theoretical concept of an elementary particle (which is defined as an irreducible quantum-mechanical system obeying such an equation). Here we consider the case where an external (classical) e.m. field is present. In this

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Evocative

,Construction explicite de l’indice de Maslov. Applications,e..Les propriétés cohomologiques de cet indice permettent de rendre transitive la . ; on construit ainsi un espace de Hilbert où agissent naturellement le groupe de Heisenberg-Weyl (.) et le groupe métaplectique (.)..Dans le cas d‘un oscillateur harmonique, l‘espace ainsi construit co?ncide avec l‘e

訓(xùn)誡

車床

Quarks and the Poincare group SU(6) x SU(3) as a classification group for baryons,