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Maps and inverse maps in open quantum dynamics

机译:开放量子动力学中的映射和逆映射

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Two kinds of maps that describe evolution of states of a subsystem coming from dynamics described by a unitary operator for a larger system, maps defined for fixed mean values and maps defined for fixed correlations, are found to be quite different for the same unitary dynamics in the same situation in the larger system. An affine form is used for both kinds of maps to find necessary and sufficient conditions for inverse maps. All the different maps with the same homogeneous part in their affine forms have inverses if and only if the homogeneous part does. Some of these maps are completely positive; others are not, but the homogeneous part is always completely positive. The conditions for an inverse are the same for maps that are not completely positive as for maps that are. For maps defined for fixed mean values, the homogeneous part depends only on the unitary operator for the dynamics of the larger system, not on any state or mean values or correlations. Necessary and sufficient conditions for an inverse are stated several different ways: in terms of the maps of matrices, basis matrices, density matrices, or mean values. The inverse maps are generally not tied to the dynamics the way the maps forward are. A trace-preserving completely positive map that is unital cannot have an inverse that is obtained from any dynamics described by any unitary operator for any states of a larger system.
机译:发现两种描述子系统状态演变的图谱是由一元算子描述的用于较大系统的动力学,对于固定均值定义的图谱和对于固定相关性定义的图谱对于相同的dynamic一阶动力学而言是完全不同的。在较大的系统中,情况相同。两种地图都使用仿射形式,以找到逆映射的必要条件和充分条件。当且仅当同质部分具有相似的仿射形式时,所有具有相同同质部分的不同图都具有逆。这些地图中有些是完全正面的。其他人则不是,但同质部分始终是完全积极的。逆的条件对于不完全为正的图与对于正的图相同。对于为固定平均值定义的映射,齐次部分仅取决于较大系统动力学的一元运算符,而不取决于任何状态或平均值或相关性。求逆的必要条件和充分条件用几种不同的方式表示:根据矩阵图,基本矩阵,密度矩阵或平均值。反向映射通常不像映射向前的方式那样依赖于动力学。单一单位的保持迹线的完全正图不能具有从较大单位的任何状态的任何统一运算符描述的任何动力学中获得的逆。

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