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Entanglement of Grassmannian Coherent States

G. Najarbashi, Yusef Maleki

Published Aug 28, 2010• 0 citations
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Para-Grassmannian Coherent and Squeezed States for Pseudo-Hermitian q-Oscillator and their Entanglement

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In this paper, q-deformed oscillator for pseudo-Hermitian systems is investigated and pseudo-Hermitian appropriate coherent and squeezed states are studied.Also, some basic properties of these states is surveyed.The over-completeness property of the para-Grassmannian pseudo-Hermitian coherent states (PGPHCSs) examined, and also the stability of coherent and squeezed states discussed.The pseudo-Hermitian supercoherent states as the product of a pseudo-Hermitian bosonic coherent state and a para-Grassmannian pseudo-Hermitian coherent state introduced, and the method also developed to define pseudo-Hermitian supersqueezed states.It is also argued that, for q-oscillator algebra of k + 1 degree of nilpotency based on the changed ladder operators, defined in here, we can obtain deformed SU q 2 (2) and SU q 2k (2) and also SU q 2k (1, 1).Moreover, the entanglement of multilevel para-Grassmannian pseudo-Hermitian coherent state will be considered.This is done by choosing an appropriate weight function, and integrating over tensor product of PGPHCSs.

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Grassmann coherent states for spin systems

Pablo G. O. Anicich, Horacio Grinberg

Journal of Molecular Structure THEOCHEM•Jan 30, 2003•4 citations
In this paper, q-deformed oscillator for pseudo-Hermitian systems is investigated and pseudo-Hermitian appropriate coherent and squeezed states are studied.Also, some basic properties of these states is surveyed.The over-completeness property of the para-Grassmannian pseudo-Hermitian coherent states (PGPHCSs) examined, and also the stability of coherent and squeezed states discussed.The pseudo-Hermitian supercoherent states as the product of a pseudo-Hermitian bosonic coherent state and a para-Grassmannian pseudo-Hermitian coherent state introduced, and the method also developed to define pseudo-Hermitian supersqueezed states.It is also argued that, for q-oscillator algebra of k + 1 degree of nilpotency based on the changed ladder operators, defined in here, we can obtain deformed SU q 2 (2) and SU q 2k (2) and also SU q 2k (1, 1).Moreover, the entanglement of multilevel para-Grassmannian pseudo-Hermitian coherent state will be considered.This is done by choosing an appropriate weight function, and integrating over tensor product of PGPHCSs.
In this paper, we investigate the entanglement of multi-partite Grassmannian coherent states (GCSs) described by Grassmann numbers for n > 2 degree of nilpotency.Choosing an appropriate weight function, we show that it is possible to construct some wellknown entangled pure states, consisting of GHZ, W, Bell, cluster type and bi-separable states, which are obtained by integrating over tensor product of GCSs.It is shown that for three level systems, the Grassmann creation and annihilation operators b and b † together with b z form a closed deformed algebra, i.e., SU q (2) with q = e 2πi 3 , which is useful to construct entangled qutrit-states.The same argument holds for three level squeezed states.Moreover combining the Grassmann and bosonic coherent states we construct maximal entangled super coherent states.
Some properties of Grassmannian U(4)/U(2)2U(4)/U{(2)}^{2}U(4)/U(2)2 coherent states and an entropic conjecture
We analyze mathematical and physical properties of a previously introduced (Calixto and Pérez-Romero 2014 J. Phys. A: Math. Theor. 47 023027 ) family of U (4) coherent states (CS). They constitute a matrix version of standard spin U (2) CS when we add an extra (pseudospin) dichotomous degree of freedom: layer, sublattice, two-well, nucleon, etc. Applications to bilayer quantum Hall systems at fractions of filling factor are discussed, where Haldane’s sphere picture is generalized to a Grassmannian picture. We also extend Wehrl’s definition of entropy from Glauber to Grassmannian CS and state a conjecture on the entropy lower bound.