49 research outputs found

    Perturbation of Continuous Frames on Quaternionic Hilbert Spaces

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    In this note, following the theory of discrete frame perturbations in a complex Hilbert space, we examine perturbation of rank nn continuous frame, rank nn continuous Bessel family and rank nn continuous Riesz family in a non-commutative setting, namely in a right quaternionic Hilbert space.Comment: 18 page

    Squeezed states in the quaternionic setting

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    Using a left multiplication defined on a right quaternionic Hilbert space, we shall demonstrate that pure squeezed states can be defined with all the desired properties on a right quaternionic Hilbert space. Further, we shall also demonstrate squeezed states can be defined on the same Hilbert space, but the noncommutativity of quaternions prevent us in getting the desired results. However, we will show that if once considers the quaternionic slice wise approach, then the desired properties can be obtained for quaternionic squeezed states.Comment: arXiv admin note: text overlap with arXiv:1704.0294

    On the dimensions of oscillator-like algebras induced by orthogonal polynomials: non-symmetric case

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    There is a generalized oscillator-like algebra associated with every class of orthogonal polynomials {Ξ¨n(x)}n=0∞\{\Psi_n(x)\}_{n=0}^{\infty}, on the real line, satisfying a four term non-symmetric recurrence relation xΞ¨n(x)=bnΞ¨n+1(x)+anΞ¨n(x)+bnβˆ’1Ξ¨nβˆ’1(x),Β Ξ¨0(x)=1,Β bβˆ’1=0x\Psi_n(x)=b_n\Psi_{n+1}(x)+a_n\Psi_n(x)+b_{n-1}\Psi_{n-1}(x),~\Psi_0(x)=1,~b_{-1}=0. This note presents necessary and sufficient conditions on ana_n and bnb_n for such algebras to be of finite dimension. As examples, we discuss the dimensions of oscillator-like algebras associated with Laguerre and Jacobi polynomials

    On the dimensions of the oscillator algebras induced by orthogonal polynomials

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    There is a generalized oscillator algebra associated with every class of orthogonal polynomials {Ξ¨n(x)}n=0∞\{\Psi_n(x)\}_{n=0}^{\infty}, on the real line, satisfying a three term recurrence relation xΞ¨n(x)=bnΞ¨n+1(x)+bnβˆ’1Ξ¨nβˆ’1(x),Ξ¨0(x)=1,bβˆ’1=0x\Psi_n(x)=b_n\Psi_{n+1}(x)+b_{n-1}\Psi_{n-1}(x), \Psi_0(x)=1, b_{-1}=0. This note presents necessary and safficient conditions on bnb_n for such algebras to be of finite dimension. As examples, we discuss the dimensions of oscillator algebras associated with Hermite, Legendre and Gegenbauer polynomials. In addition we shall also discuss the dimensions of some generalized deformed oscillator algebras. Some remarks on the dimensions of oscillator algebras associated with multi-boson systems are also presented.Comment: 16 pages, J. Math. Phys (2014

    Coherent state Quantization of quaternions

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    Parallel to the quantization of the complex plane, using the canonical coherent states of a right quaternionic Hilbert space, quaternion field of quaternionic quantum mechanics is quantized. Associated upper symbols, lower symbols and related quantities are analysed. Quaternionic version of the harmonic oscillator and Weyl-Heisenberg algebra are also obtained.Comment: 19 page

    Kato S-spectrum in the quaternionic setting

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    In a right quaternionic Hilbert space, for a bounded right linear operator, the Kato S-spectrum is introduced and studied to a certain extent. In particular, it is shown that the Kato S-spectrum is a non-empty compact subset of the S-spectrum and it contains the boundary of the S-spectrum. Using right-slice regular functions, local S-spectrum, at a point of a right quaternionic Hilbert space, and the local spectral subsets are introduced and studied. The S-surjectivity spectrum and its connections to the Kato S-spectrum, approximate S-point spectrum and local S-spectrum are investigated. The generalized Kato S-spectrum is introduced and it is shown that the generalized Kato S-spectrum is a compact subset of the S-spectrum.Comment: 30 page

    Coherent states with complex functions

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    The canonical coherent states are expressed as infinite series in powers of a complex number zz in their infinite series version. In this article we present classes of coherent states by replacing this complex number zz by other choices, namely, iterates of a complex function, higher functions and elementary functions. Further, we show that some of these classes do not furnish generalized oscillator algebras in the natural way. A reproducing kernel Hilbert space is discussed to each class of coherent states.Comment: 14 page

    Generalized 2D Laguerre polynomials and their quaternionic extensions

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    The analogous quaternionic polynomials of a class of bivariate orthogonal polynomials (arXiv: 1502.07256, 2014) introduced. The ladder operators for these quaternionic polynomials also studied. For the quaternionic case, the ladder operators are realized as differential operators in terms of the so-called Cullen derivatives. Some physically interesting summation and integral formulas are proved, and their physical relevance is also briefly discussed.Comment: 21 page

    Coherent states on quaternion Slices and a measurable field of Hilbert spaces

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    A set of reproducing kernel Hilbert spaces are obtained on Hilbert spaces over quaternion slices with the aid of coherent states. It is proved that the so obtained set forms a measurable field of Hilbert spaces and their direct integral appears again as a reproducing kernel Hilbert space for a bigger Hilbert space over the whole quaternions. Hilbert spaces over quaternion slices are identified as representation spaces for a set of irreducible unitary group representations and their direct integral is shown to be a reducible representation for the Hilbert space over the whole quaternion field.Comment: 19 page

    The Quaternionic Affine Group and Related Continuous Wavelet Transforms on Complex and Quaternionic Hilbert Spaces

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    By analogy with the real and complex affine groups, whose unitary irreducible representations are used to define the one and two-dimensional continuous wavelet transforms, we study here the quaternionic affine group and construct its unitary irreducible representations. These representations are constructed both on a complex and a quaternionic Hilbert space. As in the real and complex cases, the representations for the quaternionic group also turn out to be square-integrable. Using these representations we constrct quaternionic wavelets and continuous wavelet transforms on both the complex and quaternionic Hilbert spaces.Comment: 15 page
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