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Universal integrals of motion and universal invariants of quantum systems

机译:运动的通用积分和量子系统的通用不变量

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Universal quantum integrals of motion are introduced, and their relation with the universal quantum invariants is established. The invariants concerned are certain combinations of the second- and higher-order moments (variances) of quantum-mechanical operators, which are preserved in time independently of the concrete form of the coefficients of the Schrodinger equation, provided the Hamiltonian is either a generic quadratic form of the coordinate and momenta operators, or a linear combination of generators of some finite-dimensional algebra (in particular, any semisimple Lie algebra). Using the phase space representation of quantum mechanics in terms of the Wigner function, the relations between the quantum invariants and the classical universal integral invariants by Poincare and Cartan are elucidated. Examples of the 'universal invariant solutions' of the Schrodinger equation, i.e. self-consistent eigenstates of the universal integrals of motion, are given. Applications to the physics of optical and particle beams are discussed. [References: 81]
机译:介绍了运动的通用量子积分,并建立了它们与通用量子不变量的关系。有关的不变量是量子力学算符的二阶和高阶矩(方差)的某些组合,只要哈密顿量是泛型二次方,这些时间就可以独立于薛定inger方程系数的具体形式而及时保留。坐标和矩运算符的形式,或某些有限维代数(特别是任何半简单李代数)的生成器的线性组合。使用基于维格纳函数的量子力学的相空间表示,阐明了庞加莱和卡丹的量子不变量与经典通用积分不变量之间的关系。给出了薛定inger方程的``通用不变解''的示例,即运动的通用积分的自洽本征态。讨论了光束和粒子束的物理应用。 [参考:81]

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