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1997, Journal of Physics A: Mathematical and General
Diagonalization of uncertainty matrix and minimization of Robertson inequality for n observables are considered. It is proved that for even n this relation is minimized in states which are eigenstates of n/2 independent complex linear combinations of the observables. In case of canonical observables this eigenvalue condition is also necessary. Such minimizing states are called Robertson intelligent states (RIS). The group related coherent states (CS) with maximal symmetry (for semisimple Lie groups) are particular case of RIS for the quadratures of Weyl generators. Explicit constructions of RIS are considered for operators of su(1, 1), su(2), h N and sp(N, R) algebras. Unlike the group related CS, RIS can exhibit strong squeezing of group generators. Multimode squared amplitude squeezed states are naturally introduced as sp(N, R) RIS. It is shown that the uncertainty matrices for quadratures of q-deformed boson operators a q,j (q > 0) and of any k power of a j = a 1,j are positive definite and can be diagonalized by symplectic linear transformations.
A sufficient condition for a state |\psi> to minimize the Robertson-Schr\"{o}dinger uncertainty relation for two observables A and B is obtained which for A with no discrete spectrum is also a necessary one. Such states, called generalized intelligent states (GIS), exhibit arbitrarily strong squeezing (after Eberly) of A and B. Systems of GIS for the SU(1,1) and SU(2) groups are constructed and discussed. It is shown that SU(1,1) GIS contain all the Perelomov coherent states (CS) and the Barut and Girardello CS while the Bloch CS are subset of SU(2) GIS.
Journal of Mathematical Physics, 2002
States which minimize the Schrödinger-Robertson uncertainty relation are constructed as eigenstates of an operator which is a element of the h(1) ⊕ su(2) algebra. The relations with supercoherent and supersqueezed states of the supersymmetric harmonic oscillator are given. Moreover, we are able to compute gneneral Hamiltonians which behave like the harmonic oscillator Hamiltonian or are related to the Jaynes-Cummings Hamiltonian.
2005
States which minimize the Schr\"odinger--Robertson uncertainty relation are constructed as eigenstates of an operator which is a element of the $h(1) \oplus \su(2)$ algebra. The relations with supercoherent and supersqueezed states of the supersymmetric harmonic oscillator are given. Moreover, we are able to compute gneneral Hamiltonians which behave like the harmonic oscillator Hamiltonian or are related to the Jaynes--Cummings Hamiltonian.
Journal of Physics: Conference Series
New sum and product uncertainty relations, containing variances of up to five observables, but not containing explicitly their covariances, are derived. New inequalities for three observables, especially for the angular momentum and spin-1/2 operators, are also presented.
2000
Applications to several examples involving $SU(2),$ $SU(3),$ and the Heisenberg-Weyl group are presented, showing that there are simple examples of generalized coherent states which do not meet these conditions. Our results are relevant for phase-space description of quantum mechanics and quantum state reconstruction problems.
Journal of Physics A: Mathematical and Theoretical, 2010
We exploit the SU(N) irreducible Schwinger boson to construct SU(N) coherent states. This construction of SU(N) coherent state is analogous to the construction of the simplest Heisenberg-Weyl coherent states. The coherent states belonging to irreducible representations of SU(N) are labeled by the eigenvalues of the (N − 1) SU(N) Casimir operators and are characterized by (N − 1) complex orthonormal vectors describing the SU(N) group manifold.
Abstract. 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 and using the quantization the position and momentum operators are obtained by us in [1]. In this article, we show that the right quaternionic canonical coherent states saturate the Heisenberg uncertainty relation and thereby they form a set of intelligent states and also we show that they are a set of minimum uncertainty states.
Fortschritte der Physik, 1986
The hermitean oscillator-like realizations of classical algebras in terms of bosonic and fermionic creation and annihilation operators are given. The hermitean realizations of classical superalgebras using boson-fermion oscillators are explicitely described. The assumption of positive definite metric in a Hilbert space of the oscillators states is exploited. Due to this fact, the realizations of superalgebras in the Hilbert space can be constructed only for: the real orthosymplectic superalgebra osp ( N ; 2 M ; R); the unitary compact superalgebra su ( N ; M ) ; the unitary noncompact one S U ( N ; K , M ) ; and the quaternionic unitary superalgebra uu,(N; M ; H ) . classical Lie superalgebras (i.e. simple Lie superalgebras whose Lie subalgebra is reductive) can be divided into four classes : a) standard classical Lie superalgebras A(%, m), B(n, m ) , C(n) and B(n, m ) ; b) exceptional Lie superalgebras F(4), G(3) ; c ) strange Lie superalgebras P(n), &(n) ; d) one-parameter family of deformations of D(2, 1) denoted by . The standard classical Lie superalgebras are supersymmetric analogues of Cartan classical Lie algebras. The classification of real forms of classical Lie superalgebras are given in [3]. Recently, the realizations of supersymmetry algebras using the oscillator operators was proposed. It is connected with the problem of bosonization of the fermionic systems [4, 51 as well as the description of unitary irreducible representations of noncompact supersymmetries [6--81. By the oscillator method, using bosonic and fermionic oscillators there were constructed unitary irreducible representations of : i) anti-de Sitter superalgebra osp (2; 4 ; R) in [9]; ii) extended anti-de Sitter superalgebra osp ( N ; 4; R) in [lo]; *) On leave of absence from Institute of Teacher's Training-ODN, 50-527 Wroclaw, ul. Dawida la, Poland.
Reviews in Mathematical Physics, 1995
We present a survey of the theory of coherent states (CS) and some of their generalizations, with emphasis on the mathematical structure, rather than on physical applications. Starting from the standard theory of CS over Lie groups, we develop a general formalism, in which CS are associated to group representations which are square integrable over a homogeneous space. A further step allows us to dispense with the group context altogether, and thus obtain the so-called reproducing triples and continuous frames introduced in some earlier work. We discuss in detail a number of concrete examples, namely semisimple Lie groups, the relativity groups and various types of wavelets. Finally we turn to some physical applications, centering on quantum measurement and the quantization/dequantization problem, that is, the transition from the classical to the quantum level and vice versa.
Journal of Physics A: Mathematical and General, 2001
The boson representation of the sp(4, R) algebra and two distinct deformations of it, spq (4, R) and spt(4, R), are considered, as well as the compact and noncompact subalgebras of each. The initial as well as the deformed representations act in the same Fock space, H, which is reducible into two irreducible representations acting in the subspaces H + and H − of H. The deformed representation of spq (4, R) is based on the standard q-deformation of the boson creation and annihilation operators. The subalgebras of sp(4, R) (compact u(2) and noncompact u ε (1, 1) with ε = 0, ±) are also deformed and their deformed representations are contained in spq (4, R). They are reducible in the H + and H − spaces and decompose into irreducible representations. In this way a full description of the irreducible unitary representations of uq (2) of the deformed ladder series u 0 q (1, 1) and of two deformed discrete series u ± q (1, 1) are obtained. The other deformed representation, spt(4, R), is realized by means of a transformation of the qdeformed bosons into q-tensors (spinor-like) with respect to the suq (2) operators. All of its generators are deformed and have expressions in terms of tensor products of spinor-like operators. In this case, a deformed sut(2) appears in a natural way as a subalgebra and can be interpreted as a deformation of the angular momentum algebra so(3). Its representation in H is reducible and decomposes into irreducible ones that yields a complete description of the same. The basis states in H + , which require two quantum labels, are expressed in terms of three of the generators of the sp(4, R) algebra and are labeled by three linked integer parameters.
2012
It is the aim of this paper to show how to constructà la Perelomov andà la Barut-Girardello coherent states for a polynomial Weyl-Heisenberg algebra. This algebra depends on r parameters. For some special values of the parameter corresponding to r = 1, the algebra covers the cases of the su(1,1) algebra, the su(2) algebra and the ordinary Weyl-Heisenberg or oscillator algebra. For r arbitrary, the generalized Weyl-Heisenberg algebra admits finite or infinite-dimensional representations depending on the values of the parameters. Coherent states of the Perelomov type are derived in finite and infinite dimensions through a Fock-Bargmann approach based on the use of complex variables. The same approach is applied for deriving coherent states of the Barut-Girardello type in infinite dimension. In contrast, the construction ofà la Barut-Girardello coherent states in finite dimension can be achieved solely at the price to replace complex variables by generalized Grassmann variables. Finally, some preliminary developments are given for the study of Bargmann functions associated with some of the coherent states obtained in this work.
2000
This paper is concerned with the uncertainty principle in the context of the ane-W eyl-Heisenberg group in one and two dimensions. As the representation of this group fails to be square integrable, we explore various admissible sections of this group, and calculate the resulting uncertainty principles as well as its minimizers with respect to these sections. Previous studies have shown
Journal of Physics A: Mathematical and Theoretical, 2012
The aim of this article is to constructà la Perelomov andà la Barut-Girardello coherent states for a polynomial Weyl-Heisenberg algebra. This generalized Weyl-Heisenberg algebra, noted A {κ} , depends on r real parameters and is an extension of the A κ one-parameter algebra (Daoud M and Kibler M R 2010 J. Phys. A: Math. Theor. 43 115303) which covers the cases of the su(1, 1) algebra (for κ > 0), the su(2) algebra (for κ < 0) and the h 4 ordinary Weyl-Heisenberg algebra (for κ = 0). For finite-dimensional representations of A {κ} and A {κ},s , where A {κ},s is a truncation of order s of A {κ} in the sense of Pegg-Barnett, a connection is established with k-fermionic algebras (or quon algebras). This connection makes it possible to use generalized Grassmann variables for constructing certain coherent states. Coherent states of the Perelomov type are derived for infinitedimensional representations of A {κ} and for finite-dimensional representations of A {κ} and A {κ},s through a Fock-Bargmann analytical approach based on the use of complex (or bosonic) variables. The same approach is applied for deriving coherent states of the Barut-Girardello type in the case of infinite-dimensional representations of A {κ} . In contrast, the construction ofà la Barut-Girardello coherent states for finite-dimensional representations of A {κ} and A {κ},s can be achieved solely at the price to replace complex variables by generalized Grassmann (or k-fermionic) variables. Some of the results are applied to su(2), su(1, 1) and the harmonic oscillator (in a truncated or not truncated form).
Journal of Mathematical Physics, 2011
U q [gl(2|1)] in a coherent state basis and generalization
Considering the equality sign in Robertson-Schrödinger uncertainty relation, the generalized intelligent spin states are derived. Applying different sets of parameters, several classes of generalized intelligent states are introduced. The generalized coherent spin states and the generalized squeezed spin states are introduced as their subgroups.
Journal of Physics A: Mathematical and Theoretical, 2007
Based on the nonlinear coherent states method, a general and simple algebraic formalism for the construction of 'f-deformed intelligent states' has been introduced. The structure has the potentiality to apply to systems with a known discrete spectrum as well as the generalized coherent states with known nonlinearity function f (n). As some physical appearance of the proposed formalism, a few new classes of intelligent states associated with 'center of-mass motion of a trapped ion', 'harmonious states' and 'hydrogen-like spectrum' have been realized. Finally, the nonclassicality of the obtained states has been investigated. To achieve this purpose the quantum statistical properties using the Mandel parameter and the squeezing of the quadratures of the radiation field corresponding to the introduced states have been established numerically.
Journal of Physics A: Mathematical and General, 2001
Considering the equality sign in Robertson-Schrödinger uncertainty relation, the generalized intelligent spin states are derived. Applying different sets of parameters, several classes of generalized intelligent states are introduced. The generalized coherent spin states and the generalized squeezed spin states are introduced as their subgroups.
Communications in Physics, 2013
In recent years, one of the new applications of the coherent state method was to construct representation of superalgebras and quantum superalgebras. Following this stream, we had a contribution to working out explicit representation of Uq[gl(2|1)]. Up to now, Uq[gl(2|1) is still the biggest quantum superalgebra representations in coherent state basis of which can be built. In this article, we will show some detailed techniques used in our previous work but useful for our further investigations. The newest results on building representations in a coherent state basis of Uq[osp(2|2)], which has the same rank as Uq[gl(2|1)], are also briefly exposed.
Physical Review A, 1996
A class of squeezed states for the su(1,1) algebra is found and expressed by the exponential and Laguerre-polynomial operators acting on the vacuum states. As a special case it is proved that the Perelomov's coherent state is a ladder-operator squeezed state and therefore a minimum uncertainty state. The theory is applied to the two-particle Calogero-Sutherland model. We find some new squeezed states and compared them with the classical trajectories. The connection with some su(1,1) quantum optical systems (amplitude-squared realization, Holstein-Primakoff realization, the two mode realization and a four mode realization) is also discussed.
Journal of Physics A General Physics
The problem of how to obtain quasi-classical states for quantum groups is examined. A measure of quantum indeterminacy is proposed, which involves expectation values of some natural quantum group operators. It is shown that within any finite dimensional irreducible representation, the highest weight vector and those unitarily related to it are the quasi-classical states.
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