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note
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We measure angular momentum in units of h, so components of S and J are dimensionless.
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note
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We focus on the fundamental case of a pair of atoms, but in principle the method may be generalized for systems consisting of more than two atoms.
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This classical property of coherent states is well known in the context of the quantized light field. See AHARONOV Y., FALKOFF D., LERNER E. and PENDLETON H., Ann. Phys. (N. Y.), 39 (1966) 498; MANN A., REVZEN M. and SCHLEICH W., Phys. Rev. A, 46 (1992) 5363. As was shown in [32], in general coherent states are the unique pure states which factorize upon splitting for any quantum system with semisimple-Lie-group symmetry.
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As was shown in [32], in general coherent states are the unique pure states which factorize upon splitting for any quantum system with semisimple-Lie-group symmetry
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This classical property of coherent states is well known in the context of the quantized light field. See AHARONOV Y., FALKOFF D., LERNER E. and PENDLETON H., Ann. Phys. (N. Y.), 39 (1966) 498; MANN A., REVZEN M. and SCHLEICH W., Phys. Rev. A, 46 (1992) 5363. As was shown in [32], in general coherent states are the unique pure states which factorize upon splitting for any quantum system with semisimple-Lie-group symmetry.
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