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Related papers: SU(N) Coherent States and Irreducible Schwinger Bo…

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We generalize Schwinger boson representation of SU(2) algebra to SU(N) and define coherent states of SU(N) using $2(2^{N-1}-1)$ bosonic harmonic oscillator creation and annihilation operators. We give an explicit construction of all (N-1)…

Quantum Physics · Physics 2015-06-26 Manu Mathur , H. S. Mani

We define coherent states carrying SU(N) charges by exploiting generalized Schwinger boson representation of SU(N) Lie algebra. These coherent states are defined on $2 (2^{N - 1} - 1)$ complex planes. They satisfy continuity property and…

Quantum Physics · Physics 2015-06-26 Manu Mathur , Samir K. Paul

We construct SU(N) irreducible Schwinger bosons satisfying certain U(N-1) constraints which implement the symmetries of SU(N) Young tableaues. As a result all SU(N) irreducible representations are simple monomials of $(N-1)$ types of SU(N)…

Mathematical Physics · Physics 2015-03-13 Manu Mathur , Indrakshi Raychowdhury , Ramesh Anishetty

We define coherent states carrying SU(2) charges by exploiting Schwinger boson representation of SU(2) Lie algebra. These coherent states satisfy continuity property and provide resolution of identity on $S^{3}$. We further generalize these…

Quantum Physics · Physics 2009-11-11 Manu Mathur , Samir K. Paul

The idea of construction of the nonlinear coherent states based on the hypergeometric- type operators associated to the Weyl-Heisenberg group [J:P hys:A 45(2012) 095304], are generalized to the similar states for the arbitrary Lie group…

Mathematical Physics · Physics 2025-04-01 B. Mojaveri , A. Dehghani

The Schwinger oscillator operator representation of SU(3), studied in a previous paper from the representation theory point of view, is analysed to discuss the intimate relationships between standard oscillator coherent state systems and…

Quantum Physics · Physics 2009-11-07 S. Chaturvedi , N. Mukunda

We exploit SU(N) Schwinger bosons to construct and analyze the coupled irreducible representations of $SU(N) \times SU(N)$ in terms of the invariant group. The corresponding projection operators are constructed in terms of the invariant…

Mathematical Physics · Physics 2012-01-16 Manu Mathur , Indrakshi Raychowdhury , T P Sreeraj

We present a detailed derivation of the semiclassical propagator in the SU(n) coherent state representation. In order to provide support for immediate physical applications, we restrict this work to the fully symmetric irreducible…

Mathematical Physics · Physics 2011-05-09 Thiago F. Viscondi , Marcus A. M. de Aguiar

Generalized coherent states are developed for SU(n) systems for arbitrary $n$. This is done by first iteratively determining explicit representations for the SU(n) coherent states, and then determining parametric representations useful for…

Quantum Physics · Physics 2009-11-06 Kae Nemoto

We develop simple computational techniques for constructing all possible SU(3) representations in terms of irreducible SU(3) Schwinger bosons. We show that these irreducible Schwinger oscillators make SU(3) representation theory as simple…

Mathematical Physics · Physics 2009-06-12 Ramesh Anishetty , Manu Mathur , Indrakshi Raychowdhury

We define coherent states for SU(3) using six bosonic creation and annihilation operators. These coherent states are explicitly characterized by six complex numbers with constraints. For the completely symmetric representations (n,0) and…

Quantum Physics · Physics 2009-11-06 Manu Mathur , Diptiman Sen

Coherent states $(CS)$ of the $SU(N)$ groups are constructed explicitly and their properties are investigated. They represent a nontrivial generalization of the spining $CS$ of the $SU(2)$ group. The $CS$ are parametrized by the points of…

High Energy Physics - Theory · Physics 2009-10-22 D. M. Gitman , A. L. Shelepin

A SU(2) intertwiner with N legs can be interpreted as the quantum state of a convex polyhedron with N faces (when working in 3d). We show that the intertwiner Hilbert space carries a representation of the non-compact group SO*(2N). This…

Mathematical Physics · Physics 2017-09-13 Florian Girelli , Giuseppe Sellaroli

Schr\" odinger-Robertson uncertainty relation is minimized for the quadrature components of Weyl generators of the algebra $su(N)$. This is done by determining explicit Fock-Bargamann representation of the $su(N)$ coherent states and the…

Mathematical Physics · Physics 2009-11-10 M. Daoud

We study Bohr-Sommerfeld states in the context of the irreducible representations of SU(2). These states offer a precise bridge between the classical and quantum descriptions of angular momentum. We show that they recover the usual basis of…

Mathematical Physics · Physics 2023-07-03 Bruce Bartlett , Nzaganya Nzaganya

We study some properties of the $SU(1,1)$ Perelomov number coherent states. The Schr\"odinger's uncertainty relationship is evaluated for a position and momentum-like operators (constructed from the Lie algebra generators) in these number…

Mathematical Physics · Physics 2016-11-01 D. Ojeda-Guillén , M. Salazar-Ramirez , R. D. Mota , V. D. Granados

New quantal states which interpolate between the coherent states of the Heisenberg_Weyl and SU(1,1) algebras are introduced. The interpolating states are obtained as the coherent states of a closed and symmetric algebra which interpolates…

Quantum Physics · Physics 2009-11-07 S. Sivakumar

We extend recent results on expectation values of coherent oscillator states and SU(2) coherent states to the case of the discrete representations of su(1,1). Systematic semiclassical expansions of products of arbitrary operators are…

Quantum Physics · Physics 2016-02-22 John Schliemann

Entangled SU(2) and SU(1,1) coherent states are developed as superpositions of multiparticle SU(2) and SU(1,1) coherent states. In certain cases, these are coherent states with respect to generalized su(2) and su(1,1) generators, and…

Quantum Physics · Physics 2009-11-06 Xiao-Guang Wang , Barry C. Sanders , Shao-hua Pan

Robertson intelligent states which minimize the Schr\" odinger-Robertson uncertainty relation are constructed as eigenstates of a linear combination of Weyl generators of the $su(3)$ algebra. The construction is based on the analytic…

Mathematical Physics · Physics 2015-06-26 M. Daoud
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