Abstract
An asymmetric nature of the boson `destruction' operator and its `creation' partner is made apparent by applying them to a quantum state different from the Fock state . We show that it is possible to {\em increase} (by many times or by any quantity) the mean number of quanta in the new `photon-subtracted' state . Moreover, for certain `hyper-Poissonian' states the mean number of quanta in the (normalized) state can be much greater than in the `photon-added' state . The explanation of this `paradox' is given and some examples elucidating the meaning of Mandel's -parameter and the exponential phase operators are considered.
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