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Communications in Theoretical Physics

Quantum Statistical Properties of κ-Quantum Nonlinear Coherent States

Ji‐Suo Wang, Tang-Kun Liu, Feng Jian, Jinzuo Sun

Published Sep 15, 2004• 1 citation
Publisher

Abstract

In our preceding work, a class of k-quantum nonlinear coherent states, i.e., the k eigenstates of the powers (B) over cap (k) (k greater than or equal to 3) of the annihilation operator (B) over cap = (a) over cap1/f((N) over cap) of f-oscillators, are introduced. In this paper, we introduce a new kind of higher-order squeezing and an antibunching effect. The quantum statistical properties of the k states are studied. The result shows that the M-th order [M = (n + 1/2)k; n = 0, 1,...] squeezing effects exist in all of the k states when k is even. There is the antibunching effect in all of the k states.

DOI
10.1088/0253-6102/42/3/419

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The completeness of the k orthonormalized eigenstates of the operator ((a) over capf((n) over cap))(k) (k greater than or equal to 3) is investigated. We introduce a new kind of higher-order squeezing and an antibunching. The properties of the Mth-order squeezing and the antibunching effect of the k states are studied. The result shows that these states may form a complete Hilbert space, and the Mth-order (M = (n + 1/2)k; n = 0, 1,...) squeezing effects exist in all of the k states when k is even. There is an antibunching effect in all of the states. An alternative method for constructing the k states is proposed, and the result shows that all of them can be generated by linear superposition of the time-dependent nonlinear coherent states at different instants.
Quantum statistical properties of orthonormalized eigenstates of the operator (â f (n^\hat nn^))k
The completeness of the k orthonormalized eigenstates of the operator (â f ( )) k ( k ⩾3) is investigated. We introduce a new kind of higher-order squeezing and an antibunching. The properties of the M th-order squeezing and the antibunching effect of the k states are studied. The result shows that these states may form a complete Hilbert space, and the M th-order ( M = ( n + 1/2) k ; n = 0,1,...) squeezing effects exist in all of the k states when k is even. There is an antibunching effect in all of the states. An alternative method for constructing the k states is proposed, and the result shows that all of them can be generated by linear superposition of the time-dependent nonlinear coherent states at different instants.
A new kind of even and odd nonlinear coherent states are defined. Using the numerical method, we have studied quantum statistical properties of the new even and odd nonlinear coherent states. It is shown that quantum statistical properties of the new even and odd nonlinear coherent states are very different from those of the usual even and odd coherent states. It is found that, in some ranges of 1beta1, the squeezing only exists in the new even nonlinear coherent state, and the amplitude-squared squeezing and antibunching effect appear for both new even and odd nonlinear coherent states.
The completeness of the k orthonormalized eigenstates of the operator ((a) over capf((n) over cap))(k)(k greater than or equal to 3) is investigated. We introduce an antibunching and a new kind of higher-order squeezing. The properties of the antibunching effect and M-th-order squeezing of the k states are studied. The result shows that these states may form a complete Hilbert space. There is antibunching effect in all of the states, and the M-th [M = ( n + 1/2) k; n = 0, 1 2, ...] squeezing effects exist in all of the k states when k is even.