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sl(2)-modules by sl(2)-coherent states

机译:sl(2)-由sl(2)相干态构成的模块

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Irreducible sp(4)-module with highest weight, labeled by the azimuthal and magnetic quantum numbers l and m, is split into the direct sums of the irreducible su(2)- and su(1,1)-submodules in four different ways: finite integer unitary irreducible subspaces corresponding to the orbital angular momentum algebra su(2), infinite positive discrete series of su(1,1) with an arbitrary half-integer Bargmann index, and the positive and negative discrete series of su(1,1) with both the Bargmann indices 1/4 and 3/4. Even and odd coherent states for the positive su(1,1)-submodules with the Bargmann indices 1/4 and 3/4 are constructed and it is shown that they enjoy the property of completeness by two appropriate positive definite measures. We show that the even and odd coherent states themselves form the positive discrete series of su(1,1) with the Bargmann indices 1/4 and 3/4, respectively. For these even and odd coherent states, we consider the uncertainty relations for the x- and y-components of the angular momentum as well as the generators of the negative discrete series of su(1,1) with the Bargmann indices 1/4 and 3/4. Published by AIP Publishing.
机译:具有最大权重的不可约sp(4)-模块,由方位角和磁量子数l和m标记,以四种不同方式分为不可约su(2)-和su(1,1)-子模块的直接和:有限整数unit不可约子空间,它对应于轨道角动量代数su(2),具有任意半整数Bargmann指数的su(1,1)的无限正离散序列,以及su(1,的正负离散序列), 1)的巴格曼指数均为1/4和3/4。构造具有Bargmann指数1/4和3/4的正su(1,1)-子模的偶数和奇数相干态,并通过两个适当的正定度量显示它们具有完备性。我们表明,偶数和奇数相干态本身形成su(1,1)的正离散序列,其Bargmann指数分别为1/4和3/4。对于这些偶数和奇数相干态,我们考虑了角动量的x和y分量的不确定性关系以及su(1,1)的负离散序列su(1,1)的Bargmann指数为1/4和3/4。由AIP Publishing发布。

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