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This is in contrast to putting together the operators U and V, as seen by the last relation in Eq. (2); we will shortly come back to this difference
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This is in contrast to putting together the operators U and V, as seen by the last relation in Eq. (2); we will shortly come back to this difference.
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15
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85037768130
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This example, for which we are grateful to H. Kastrup, provides a simplified version of what will be found for the phase space S by the systematic procedure employed in Sec. III [cf. Eqs. (10) and (7)]
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This example, for which we are grateful to H. Kastrup, provides a simplified version of what will be found for the phase space S by the systematic procedure employed in Sec. III [cf. Eqs. (10) and (7)].
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16
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85037758099
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We are grateful to D. Giulini for this remark
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We are grateful to D. Giulini for this remark.
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For further realizations we refer to Ref. 5 and to Sec. III B 5
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For further realizations we refer to Ref. 5 and to Sec. III B 5.
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27
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85037751664
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note
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min=θ=0 in our notation, i.e., for parameters where the identification with the group theoretical quantization breaks down) in the context of quantum optics, where the phase space S plays a major role (cf. Ref. 28, we are grateful to H. Kastrup for this remark).
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