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  • American Institute of Physics (AIP)  (9,520)
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  • 1
    Electronic Resource
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    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 34 (1993), S. 3867-3877 
    ISSN: 1089-7658
    Source: AIP Digital Archive
    Topics: Mathematics , Physics
    Notes: By introducing a suitable continuous-time regularization into a formal phase-space path integral it follows that the propagator is given by the limit of well-defined functional integrals involving standard stochastic processes and their associated probability measures. Such regularizations require pinning of both coordinate and momenta variables, and automatically lead to coherent-state representations. It is found that each standard independent increment process, involving a superposition of a Wiener and a Poisson process, is associated with a specific, generally non-Gaussian, fiducial vector with which the coherent states are defined.
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  • 2
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    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 34 (1993), S. 4273-4286 
    ISSN: 1089-7658
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    Topics: Mathematics , Physics
    Notes: The possible holonomy groups of compact, locally irreducible Riemannian manifolds are studied. Motivated by applications arising in physics, it is not required that these manifolds be simply connected. In this paper a complete classification up to dimension ten is given, with particular emphasis on the manifolds of dimension six or less. In this latter case, there exist actual examples for every class, so that the possible holonomy groups can be characterized exactly.
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  • 3
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    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 34 (1993), S. 4316-4329 
    ISSN: 1089-7658
    Source: AIP Digital Archive
    Topics: Mathematics , Physics
    Notes: The Clebsch–Gordan coefficients for the general Gel'fand basis of the quantum group SUq(N) are calculated from the induction coefficients of the Hecke algebra Hf(q) by the linear equation method. The advantage of this method is that the calculation of the SUq(N) Clebsch–Gordan coefficients is rank independent. The SUq(N) Clebsch–Gordan coefficients for the resulting irreps [f1,f2,f3] with f1+f2+f3≤4 are tabulated.
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  • 4
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    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 34 (1993), S. 4364-4369 
    ISSN: 1089-7658
    Source: AIP Digital Archive
    Topics: Mathematics , Physics
    Notes: A nonperturbative approximate analytical solution is derived for the Lane–Emden equation using the Adomian decomposition method. The solution is in the form of a power series with easily computable coefficients. The Padé approximants method is used to accelerate the convergence of the power series. Comparison with some known exact and numerical solutions shows that the present solution is highly accurate.
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  • 5
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    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 34 (1993), S. 3327-3342 
    ISSN: 1089-7658
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    Topics: Mathematics , Physics
    Notes: A discrete version of the quaternionic Cauchy–Riemann equation ∂A=F, where F is Gauss–Poisson white noise, is discussed. On the lattice δZ4 random variables Fδ(δn) and Aδ(δn) are constructed which approximate the corresponding random fields F and A, respectively, in the limit δ→0. In the Gaussian case the random variables Aδ(δn) can be interpreted as the lattice approximation of the free electromagnetic Euclidean potential field whereas in the non-Gaussian case one obtains an approximation of nonlinear interacting electromagnetic quantum fields. Convergence to the continuum limit is proven.
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  • 6
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    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 34 (1993), S. 3343-3350 
    ISSN: 1089-7658
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    Topics: Mathematics , Physics
    Notes: In the present article we discuss whether or not ansatzes more general than those considered hitherto, for the representation in terms of plane waves of eigensolutions of the Schrödinger equation for a free particle in a plane convex polygonal domain, lead to the construction of a complete set for a class of domains larger than the well-known one, containing the polygons for which such a complete set can be obtained in terms of a superposition of a finite number of plane waves. Our conclusion is in the negative. Comments are also made on some features of a representation in terms of analytic functions of two complex variables.
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  • 7
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    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 34 (1993), S. 3391-3404 
    ISSN: 1089-7658
    Source: AIP Digital Archive
    Topics: Mathematics , Physics
    Notes: The analytical expressions for the energy gain and transition probabilities between energy levels of a nonrelativistic quantum particle confined in a box with uniformly moving walls, including the cases of adiabatic motion and a sudden change of the size of the box was obtained.
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  • 8
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    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 34 (1993), S. 3405-3419 
    ISSN: 1089-7658
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    Topics: Mathematics , Physics
    Notes: Following the spectral methods established by Adler in his treatment of scattering and decay in the quaternionic quantum theory, it is shown that an anti-self-adjoint operator with quaternion defined spectrum in [0,∞) has a symmetrical effective spectrum, from the point of view of functional analysis, under quite general conditions. In the case of an operator with absolutely continuous spectrum in [0,∞), the effective spectrum is absolutely continuous in (−∞,∞), and a canonically conjugate operator exists. If the anti-self-adjoint operator is the generator of motion in time (Hamiltonian), the conjugate operator is a "time operator.'' Moreover, according to a theorem of Misra, Prigogine, and Courbage, such a system may admit a Lyapunov operator, and therefore describe irreversible behavior. It is shown directly that no evident contradiction (as is found in the semibounded case in complex quantum mechanics) arises from the definition of a Lyapunov operator in quaternionic quantum mechanics.
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  • 9
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    Journal of Mathematical Physics 34 (1993), S. 3471-3477 
    ISSN: 1089-7658
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    Topics: Mathematics , Physics
    Notes: The connections between the decompositions of the identity operator on L2(Rn) and the decompositions of the function 1 on the phase space R2n are considered. The phase space properties of various transformations (such as the Fourier transform, Gabor transform, and wavelet transform, etc.) are investigated.
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  • 10
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    Journal of Mathematical Physics 34 (1993), S. 4190-4198 
    ISSN: 1089-7658
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    Topics: Mathematics , Physics
    Notes: This article is the continuation of a series of articles about group theory and wavelet analysis [A. Grossmann, J. Morlet, and T. Paul, J. Math. Phys. 26, 2473 (1985)]. As is well-known in the case of the afine group, the reconstruction wavelet and the analyzing wavelet need not be identic. In this article it is shown that this holds for arbitrary groups. In addition it is shown that even for nonadmissible analyzing wavelets the wavelet transform may be inverted. Accordingly the image of the wavelet transform can be characterized by many different reproducing kernels.
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  • 11
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    Journal of Mathematical Physics 34 (1993), S. 4251-4272 
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    Topics: Mathematics , Physics
    Notes: A complete study of deformations of Lie group and Lie algebra representations, including differentiability and integrability results, is given. Adapted results are given in the semisimple case. A notion of induced deformations is introduced. Various examples are given, including deformations of indecomposable representations.
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  • 12
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    Journal of Mathematical Physics 34 (1993), S. 4305-4315 
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    Notes: A general procedure for evaluating the induction coefficients (IDCs) or the outer-product reduction coefficients of the Hecke algebra Hf(q) of the Af−1 type is formulated based on the linear equation method. Analytical expressions for the IDC's of Hf(q) are tabulated for f≤4. It is also proved that these IDCs are the Clebsch–Gordan coefficients for the special Gel'fand basis of the quantum group SUq(N).
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  • 13
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    Journal of Mathematical Physics 34 (1993), S. 4340-4363 
    ISSN: 1089-7658
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    Topics: Mathematics , Physics
    Notes: Representations for quantum groups at q an Nth root of 1 with a structure resembling the algebraic structure in the theory of the chiral Potts models are constructed in the Uq(sp(2n,C)), Uq(so(2n+1,C)), and Uq(so(2n,C)) cases. The dimensions of the given representations and their number of free parameters are N(1/2)(dim g-rank g), dim g, respectively.
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  • 14
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    Journal of Mathematical Physics 34 (1993), S. 3429-3439 
    ISSN: 1089-7658
    Source: AIP Digital Archive
    Topics: Mathematics , Physics
    Notes: It is shown that a physical primary field composed with the adjoint of a physical primary field is single valued only for the unitary conformal models with central charge 0〈c〈1.
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  • 15
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    Journal of Mathematical Physics 34 (1993), S. 3463-3470 
    ISSN: 1089-7658
    Source: AIP Digital Archive
    Topics: Mathematics , Physics
    Notes: A general class of exact solutions for the Minkowskian σ model of the hyperbolic Grassmanian manifold, which was considered earlier by Lambert and Piette, are constructed. The energy momentum tensor associated with these solutions can be made finite with a suitable choice of the arbitrary functions involved in their construction.
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  • 16
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    Journal of Mathematical Physics 34 (1993), S. 3676-3682 
    ISSN: 1089-7658
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    Topics: Mathematics , Physics
    Notes: The analysis of the equations vtt=f(x,vx)vxx+g(x,vx) initiated by Ibragimov et al. [J. Math. Phys 32, 2988 (1991)] is continued. The preliminary group classification of these equations with respect to a countable-dimensional subalgebra of their equivalence algebra is presented. This subalgebra is an extension of the 10-dimensional subalgebra considered by Ibragimov et al. The result of the work is a table of nonequivalent equations possessing an additional symmetry.
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  • 17
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    Journal of Mathematical Physics 34 (1993), S. 3768-3774 
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    Topics: Mathematics , Physics
    Notes: The process to obtain a geodesic as a limit from a sequence of geodesics in a Lorentzian manifold is analyzed in detail. It is found that the limit of incomplete geodesics in a compact manifold is not incomplete in general. A new class of incomplete compact Lorentzian manifolds, one of them showing this anomalous behavior, is constructed. Thus, a counterexample to the proof, given by U. Yurtsever [J. Math. Phys. 33, 1295 (1992)] to the result originally proven by Y. Carrière [Invent. Math. 95, 615 (1989)] (in a quite different way) is given. That proof should imply that an incomplete compact Lorentzian manifold must be null incomplete. It is not known if this assertion is true, and, hence, remains as an open question.
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  • 18
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    Journal of Mathematical Physics 34 (1993), S. 3809-3824 
    ISSN: 1089-7658
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    Topics: Mathematics , Physics
    Notes: Degenerations of Lie algebras of meromorphic vector fields on elliptic curves (i.e., complex tori) which are holomorphic outside a certain set of points (markings) are studied. By an algebraic geometric degeneration process certain subalgebras of Lie algebras of meromorphic vector fields on P1, the Riemann sphere, are obtained. In case of some natural choices of the markings these subalgebras are explicitly determined. It is shown that the number of markings can change.
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  • 19
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    Journal of Mathematical Physics 34 (1993), S. 3856-3862 
    ISSN: 1089-7658
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    Topics: Mathematics , Physics
    Notes: It is shown that the spin-weighted cylindrical harmonics s Jαm(ρ,φ), which are functions defined on the plane, are related to representation matrices of the group of rigid motions on the plane. It is also shown that the raising and lowering operators of the spin weight and of the z component of the angular momentum are related to two copies of the Lie algebra of the Euclidean group of the plane.
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  • 20
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    Journal of Mathematical Physics 34 (1993), S. 2713-2717 
    ISSN: 1089-7658
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    Topics: Mathematics , Physics
    Notes: A fast and absolute converging sequence, for the Thomas–Fermi (TF) initial slope, was obtained by applying a perturbative approach [C. M. Bender et al., J. Math. Phys. 30, 1447 (1989)] to the TF equation written in terms of the electronic density. By this procedure the truncated series does not alternate, in contrast to a previous work [B. J. Laurenzi, J. Math Phys. 31, 2535 (1990)] based in the traditional TF equation.
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  • 21
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    Journal of Mathematical Physics 34 (1993), S. 2742-2756 
    ISSN: 1089-7658
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    Notes: New solutions for the mode functions of the electromagnetic field in ideal cavity which boundary oscillates at a resonance frequency are obtained in the long-time limit. The rate of photons creation from initial vacuum state is shown to be time independent and proportional to the amplitude of oscillations and the resonance frequency. Temperature corrections are evaluated. The squeezing coefficients for the quantum states of the field generated are calculated, as well as the backward reaction of the field on the vibrating wall.
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  • 22
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    Journal of Mathematical Physics 34 (1993), S. 2757-2778 
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    Notes: Reducible gauge theories with constraints linear in the momenta are quantized. The equivalence of the reduced phase space quantization, Dirac quantization, and BRST quantization is established, provided one transforms appropriately the Dirac wave functions under changes of representation of the constraint surface and of the reducibility functions. The ghosts of ghosts are found to play a crucial role in the equivalence proof.
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  • 23
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    Journal of Mathematical Physics 34 (1993), S. 2691-2712 
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    Notes: The construction of Euclidean Majorana fermions on a two-dimensional cylindrical space–time is discussed, based on a given real-time theory. After a review of the basics of defining Euclidean fermions in the free theory, a functional integral formulation for the Euclidean theory is introduced. This functional integral connects the expectation values of the Euclidean fields with the theory of relative Pfaffians. A proof, which draws on these ideas, is given for the Feynman–Kac formula of a general interacting theory.
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    Journal of Mathematical Physics 34 (1993), S. 2789-2806 
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    Notes: A supersymmetric quantum mechanics on SO(3) is examined. It was found that instanton solutions and the normal coordinate expansions around them allow the explicit path integration. The Witten complex is obtained by calculating the matrix elements of the generalized exterior derivative.
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  • 25
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    Journal of Mathematical Physics 34 (1993), S. 2779-2788 
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    Notes: It is shown that the discrete spectrum of Schrödinger Hamiltonians of the form H=−Δ+vf may be represented by the semiclassical expression Enl=minr(approximately-greater-than)0 {K(f)nl(r) + vf(r)}. The K functions are found to be invariant with respect to coupling and shifts: K(Af+B)=K(f). For pure power laws, f(r)=sgn(q)rq, and the log potential, they are also invariant with respect to scale, and have the simple forms (Pnl(q)/r)2 and (Lnl/r)2, respectively. K functions are also derived for sech-squared and Hulthén potentials. If f=g(h), where g is a smooth transformation, then the envelope approximation is expressed in terms of K by the relation K(f)(approximately-equal-to)K(h). When the transformation g has definite convexity, then the approximation immediately yields eigenvalue bounds for all n and l. The theory is used to prove the log-power theorem Lnl = Pnl(0), which, in turn, generates a simple eigenvalue formula for the log potential.
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    Journal of Mathematical Physics 34 (1993), S. 2827-2851 
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    Notes: Quantum mechanics on SD is formulated. The algebra of (D+1)-dimensional Euclidean group is set up as fundamental commutation relation, which plays the role of the ordinary canonical algebra on the flat space. Compared to the standard procedure of using Dirac's formalism for quantization of the constrained system, our method leads to more general results. Monopolelike structure appears inside the SD, which becomes visible when the space is cut by 3-dimensional hyperplane. Gauge potential for this structure is obtained. We also show, that no higher dimensional singularity can appear inside the SD.
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    Journal of Mathematical Physics 34 (1993), S. 2875-2892 
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    Notes: The inverse of paraboson annihilation and creation operators is introduced. The properties of these operators, their number state representation and commutation relations are discussed. Also introduced are the family of eigenstates of bilinears in paraboson operators and their inverses; and study the nonclassical properties, namely, squeezing and fluctuations in number of parabosons in these eigenstates. It is observed that a family of the eigenstates of a+−1a is the parasqueezed vacuum, S(σ)||0,α〉. Similarly, a family of the eigenstates of aa+−1 is the parasqueezed first state, S(σ)||n=1,α〉.
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    Journal of Mathematical Physics 34 (1993), S. 2965-2967 
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    Notes: Crystallographers use x-ray spectra to understand the structure of solids and ergodic theorists use spectra of abstract dynamical systems for structural studies; the relation of the two is shown here.
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  • 29
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    Journal of Mathematical Physics 34 (1993), S. 3273-3291 
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    Notes: The Yang–Baxter equation can be recast as a triple product equation. Assuming the triple product to satisfy some algebraic relations, new solutions of the Yang–Baxter equation can be found. This program has been completed here for the simplest triple systems which are called octonionic and quaternionic. The solutions are of rational type.
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    Journal of Mathematical Physics 34 (1993), S. 2107-2114 
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    Notes: We show explicitly that the eigenvalue equation describing the normal modes of the sphalerons in the 1+1 Abelian Higgs model is a quasi-exactly-solvable system.
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    Journal of Mathematical Physics 34 (1993), S. 2119-2131 
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    Notes: Associated with the q-deformation of the harmonic oscillator algebra we define an infinite dimensional braid group representation on the Hilbert space of the harmonic oscillator, and an extended Yang–Baxter system in the sense of Turaev. The corresponding link invariant is computed in some particular cases and coincides with the inverse of the Alexander–Conway polynomial. The R matrix of Uq(h4) can be interpreted as defining a baxterization of the intertwiners for semicyclic representations of SU(2)q at q=e2πi/N in the N→∞ limit. Finally we define new multicolored braid group representations and study their relation to the multivariable Alexander–Conway polynomial.
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    Journal of Mathematical Physics 34 (1993), S. 2132-2152 
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    Notes: The Batalin–Vilkovisky formalism is studied in the framework of perturbation theory by analyzing the antibracket Becchi–Rouet–Stora–Tyutin (BRST) cohomology of the proper solution S0. It is concluded that the recursive equations for the complete proper solution S can be solved at any order of perturbation theory. If certain conditions on the classical action and on the gauge generators are imposed the solution can be taken local.
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    Journal of Mathematical Physics 34 (1993), S. 3121-3132 
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    Notes: Fackerell–Crossman's solutions to a generalized spheroidal wave equation are extended for the case in which there is no free parameter in that equation. The results, together with Leaver's expansions in series of Coulomb wave functions, are used to find the time dependence of massive scalar test fields in nonflat Friedmann–Robertson–Walker models of universes with dust.
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    Journal of Mathematical Physics 34 (1993), S. 3162-3196 
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    Notes: This article describes an intrinsic tensor technique for solving boundary value problems in electrodynamics of moving media, which entails considerable notational simplification and calculational advantages. On the basis of generalized impedance and characteristic matrix methods, the reflection and transmission operators of a multilayer structure consisting of anisotropic media uniformly moving with different velocities are found. A general solution to the problem of reflection and transmission at the interface between two moving isotropic media is obtained, and explicit expressions for Doppler shifts, Snell's laws, critical and Brewster angles, reflection and transmission coefficients, and the radiation pressure force are found. The material tensor of a uniformly moving linear medium is expressed through its reflection and transmission operators.
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    Journal of Mathematical Physics 34 (1993), S. 2317-2330 
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    Notes: The eigenvalue correlation functions of the Laguerre ensembles (exponential ensembles) of real symmetric and self-dual quaternion random matrices are calculated. It is shown that in certain intervals of the spectrum the renormalized correlations are not universal. A physical example in the transmission spectrum of a disordered conductor where such nonuniversality occurs is given.
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    Journal of Mathematical Physics 34 (1993), S. 3292-3315 
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    Notes: The result of Paper I in this set is generalized and the Yang–Baxter equation is solved in terms of triple systems called orthogonal and symplectic ternary systems. In this way, several other new solutions are found.
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    Journal of Mathematical Physics 34 (1993), S. 2115-2118 
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    Notes: We solve the modified Toda molecule equation by use of a Laplace transform technique for the Lie algebras An, Bn, Cn, and G2 with the appropriate boundary conditions for obtaining magnetic monopole solutions.
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    Journal of Mathematical Physics 34 (1993), S. 2089-2106 
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    Notes: Working directly from a covariant equation for two interacting fermions with equal masses and opposite charges, energy eigenvalues and eigenfunctions are calculated to order α6 and α4, respectively, where α is the fine structure constant. The eigenvalues agree with those determined previously by perturbative techniques, including relativistic, recoil and spin corrections, for all the energy levels of orthopositronium. The eigenvalue problems that arise in the present approach are of Sturm–Liouville-type, but involve one, or two coupled, second-order ordinary differential equations in the radial variable r, with up to four singular points. The method used has two key steps. For values of r of the order of the Bohr radius, the equations are transformed by suitable changes of variable into equations which are equivalent, to the appropriate order of approximation, but which are exactly soluble. The second step involves adjusting the behavior at r=0 of the resultant solutions to match the known behavior of the (unknown) exact eigenfunctions. This approach enables approximate eigenvalues to be determined directly, and corresponding approximate eigenfunctions to be obtained for the first time in simple closed form.
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    Journal of Mathematical Physics 34 (1993), S. 2153-2165 
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    Notes: The coherent states for the quantum complex plane are introduced. It is demonstrated that the Bargmann representation corresponding to these states involves both the standard integral with respect to the Gaussian measure and the Berezin integral over Grassmann variables. The quantum generalizations of many constructions developed for classical coherent states are described.
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    Journal of Mathematical Physics 34 (1993), S. 2206-2214 
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    Notes: The finite temperature correction to the electron mass in a quantum electrodynamics framework is computed in the high-temperature regime by Matsubaralike sums. As pointed out by other authors, it is confirmed that the leading term is of the type ΔM∝T, contrary to what one might expect by naïve reasonings.
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    Journal of Mathematical Physics 34 (1993), S. 2242-2256 
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    Notes: In this work is presented a generalization of Poncelet's theorem to n dimensions which is refered to as the full Poncelet's theorem. The theorem states that if the reflections of a trajectory by a sequence of confocal quadrics lead to a closed skew polygon, then there exists an (n−1)-parameter family of polygons having the same property. A physical realization and a projective geometrical proof of this theorem are given. If all the reflecting quadrics coincide, the above theorem reduces to the n-dimensional Poncelet's theorem presented by Chang and Friedberg. The geometrical proof is a finite construction based on a preliminary theorem which extends Hart's lemma. The full Poncelet's theorem may thus be extended to projective geometries over most fields, including discrete ones.
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    Journal of Mathematical Physics 34 (1993), S. 2290-2316 
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    Notes: The domain of applicability of one-point kinetic theory is enlarged by admitting two-point distribution functions or some of their moments as extra state variables. Kinetic equations governing the time evolution in the extended state space are introduced as particular realizations of the nonlinear Onsager–Casimir equation. This abstract equation collects the common structure of equations arising in the analysis of compatibility of two levels of description (e.g., kinetic theory and equilibrium thermodynamics or kinetic theory and hydrodynamics). The structure consists of a Poisson bracket and two potentials. The Poisson bracket expresses kinematics, the first potential, called the thermodynamic potential, generates the time evolution and links the theory with thermodynamics. The second potential, called the dissipative potential, introduces dissipation into the time evolution that is compatible with the kinematics and thermodynamics. To find a particular realization of the nonlinear Onsager–Casimir equation means to identify kinematics (Poisson bracket) and the two potentials, that correspond to a particular system and situations under consideration. This way of introducing kinetic equations has two advantages. First, the kinetic equations are guaranteed to be intrinsically consistent and compatible with more macroscopic theories. Second, the clear physical meaning of kinematics and the two potentials, together with the possibility of discussing them separately, allows one to use a broad range of physical insights and considerations to specify them for particular systems and situations of interest.
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    Journal of Mathematical Physics 34 (1993), S. 1757-1772 
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    Notes: On a Fock superspace, a linear canonical supertransformation is implemented by an inner-product-preserving operator which is necessarily not continuous.
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    Journal of Mathematical Physics 34 (1993), S. 1807-1817 
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    Notes: As shown by Kovner and Rosenstein, the O(N) invariant nonlinear sigma model, which in Dirac's language of constrained systems presents only second-class type of constraints, possess a hidden U(1) gauge symmetry. The presence of this symmetry is investigated, in this work, with the introduction of a Wess–Zumino term that implements Faddeev's idea of changing second-class constraints into gauge generating first-class constraints. The resulting theory exhibits the embedding of the O(N) invariant model into a gauge theory which presents an enlarged phase-space with the inclusion of a Wess–Zumino field.
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    Journal of Mathematical Physics 34 (1993), S. 1884-1891 
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    Notes: The Adler, Kostant, and Syms theorem has been used to construct integrable nonlinear dynamical systems involving both bosonic and fermionic variables. Explicit forms of the equations are displayed in case of two super Lie Algebra OSPU(1,1/1) and Sl(2/2). Integrability is proved by explicit construction of higher order conserved quantities.
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    Journal of Mathematical Physics 34 (1993), S. 1914-1926 
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    Notes: The recent result that there is no Bekenstein black hole at D(approximately-greater-than)4 is confirmed by the direct integration of the field equations of the self-gravitating conformal scalar field. The case D=3 where the result turns out to be same is also solved. The curvature singularities of the obtained solutions are analyzed and it is shown that there do exist special (critical) space-times which, however, are of the black hole type only at D=4.
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    Journal of Mathematical Physics 34 (1993), S. 1964-1985 
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    Notes: Starting with the SU(2)q⊗SU(2)q basis and using q-CG coefficients the closest possible q deformation of the classical canonical Gelfand–Zetlin formalism is constructed explicitly for SO(4)q. Simple introduction of q brackets for each factor of the classical matrix elements, valid for SU(n)q, is shown to need significant and unexpected modifications for SO(n)q even when n=4. Contraction to E(3)q and continuation to SO(3,1)q are studied, making explicit the possibilities and the problems that arise. Periodic representations for q, a root of unity, are commented upon briefly.
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    Journal of Mathematical Physics 34 (1993), S. 1986-1994 
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    Notes: A sequence of infinitely generated p-adic Banach superalgebras and their locally convex projective and inductive limits were constructed; their spectral properties are characterized herein and by studying the algebras of matrices constructed with these superalgebras an exponential map and its inverse can be defined. Some examples of superalgebra with pathological spectral properties are discussed.
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    Journal of Mathematical Physics 34 (1993), S. 2541-2553 
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    Notes: A noncanonical parametrization for the graded group U(1/1) is introduced similar to the Euler angles for the ordinary group SU(2). Two differential representations for the underlying algebra of U(1/1) are constructed on the full and the restricted, i.e., coset, parameter space, respectively. A space of functions living on the latter is found exhibiting close formal similarities to a Hilbert space. Remarkably, the indices of those functions and thus the orthogonality and completeness relations involve anticommuting variables. Using this Hilbert space a representation of U(1/1) is evaluated which shows analogies to the Wigner functions for SU(2).
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    Journal of Mathematical Physics 34 (1993), S. 1519-1522 
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    Notes: The super-rotation algebra is realized as differential operators acting on functions defined on the E(1/2) superspace.
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    Journal of Mathematical Physics 34 (1993), S. 1548-1556 
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    Notes: Translation normalizers of Euclidean groups are introduced as normalizers with respect to the translation subgroup of the full Euclidean group. It is shown that the concept can be easily generalized to translation normalizers of affine groups; the results for normalizers of Euclidean groups can be at once adopted for those affine groups which have orthogonalizable point groups. Some of elementary and basic properties of translation normalizers are proved. The translation normalizer is identical for all groups of the generalized arithmetic class—a concept borrowed from mathematical crystallography, because such a generalization is quite natural. It is further shown, how to use translation normalizers in consideration of sets of conjugate subgroups or supergroups and hence also of normal subgroups of Euclidean groups. For that purpose is derived the space shift diagram and normality criterion. The exposition is closed by a brief discussion of the connection of translation normalizers with location properties of Euclidean motion groups.
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    Journal of Mathematical Physics 34 (1993), S. 1557-1576 
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    Notes: A method of calculation of translation normalizers is described which can be used in any dimension and which consists in three steps: (i) In the first step is determined the continuous part of the normalizer, which is a linear envelope of a stability space of the point group and of the continuous part of translation subgroup of the Euclidean group in question. (ii) In the second step are determined translation normalizers of irreducible components. (iii) And finally there is a theorem which gives an upper and lower limit for the translation normalizer of a reducible arithmetic class in terms of normalizers of its irreducible components. A check of coset representatives in resolution of the upper limit with respect to the lower limit concludes the calculation. The method is used to derive a table of translation normalizers of discrete, continuous, and semicontinous Euclidean groups up to three dimensions; all these groups are of interest in material physics. The consideration of translation normalizers is preceded by an extension and amendment of concepts used in crystallography which aim to specify the groups for which the tables are finally given.
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    Journal of Mathematical Physics 34 (1993), S. 1007-1015 
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    Notes: A solution of the Einstein field equations for a rotating radiating body was presented by Carmeli and Kaye in 1977 [Ann. Phys. 103, 97 (1977)]. Their paper presented a new line element along with the corresponding energy-momentum tensor for the radiation field. The Newman–Penrose formalism [J. Math. Phys. 3, 566 (1962)] was used to solve and analyze the new solution which lead to the tetrad components of the Ricci, Maxwell, and Weyl tensors. However, no attempt was made to solve the geodesic equation in this new metric. The present paper starts with a linearized form of the Carmeli and Kaye line element and solves the resulting differential equations to a particular order for a null geodesic. The deflection angle is found from the equations of motion and compared in detail for the two cases of a rotating, highly luminous quasar and our sun.
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    Journal of Mathematical Physics 34 (1993), S. 1277-1294 
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    Notes: The various aspects of parasupersymmetric quantum mechanics of one boson and one parafermion of (arbitrary) order p are discussed in some detail. In particular it is shown that the parasupersymmetry algebra is given by Q1pQ1++Q1p−1Q1+Q1+...+Q1Q1+ Q1p−1+Q1+Q1p =2pQ1p−1H, [H,Q1]=0; Q1p+1=0 and the Hermitian conjugated relations where Q1 is the parasupercharge and H the Hamiltonian. It is also shown that such a system always possesses (p−1) other conserved parasupercharges and p bosonic constants. Further, a special case is pointed out when the above algebra takes a very simple form as given by Q1Q1+Q1=2Q1H, Q1pQ1++Q1+Q1p= 2Q1p−1H. A model of conformal parasupersymmetry of degree p is discussed and it is shown that in this case one has p supercharges, p conformal supercharges, and p bosonic constants which along with H, dilatation generator D, and conformal generator K form a closed algebra. A model of parasupersymmetry of degree p is discussed which is not conformal invariant and yet whose spectrum can be algebraically obtained by using the above conformally invariant supersymmetry model. Finally a model of parasupersymmetric quantum mechanics of one paraboson of (arbitrary) order q and one parafermion of order p is discussed.
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    Journal of Mathematical Physics 34 (1993), S. 1370-1392 
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    Notes: Wave splitting of the time dependent Maxwell's equations in three dimensions with and without dispersive terms in the constitutive equation is treated. The procedure is similar to the method developed for the scalar wave equation except as follows. The up- and down-going wave condition is expressed in terms of a linear relation between the tangential components of E and H. The resulting system of differential-integral equations for the up- and down-going waves is directly obtained from Maxwell's equations. This splitting (arising from the principal part of Maxwell's equations) is applied to the case where there is dispersion. A formal derivation of the imbedding equation for the reflection operator in a medium with no dispersion is obtained.
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    Journal of Mathematical Physics 34 (1993), S. 1421-1428 
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    Notes: The Jaulent–Miodek hierarchy [M. Jaulent and I. Miodek, Lett. Math. Phys. 1, 243 (1976)] and its two-dimensional analog are considered from the point of view of Darboux transforms structures. A new form of those transforms as well as old fashioned forms are presented. The determinant form of solitons is obtained. The combination of different transforms in the 2+1 case allows the buildup of localized solutions in both spatial dimensions, including the two-dimensional Korteweg-de Vries (KdV) equation.
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    Journal of Mathematical Physics 34 (1993), S. 1480-1486 
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    Notes: A family of static multicentered solutions to modified Einstein–Maxwell equations coupled with a dilaton is constructed in (1+N) dimensional space–time (N≥2). For N≥3, the solutions are generalizations of the Majumdar–Papapetrou solution. We also find the solution in (1+2) dimensions, where the scalar and vector forces cancel each other in the static case. The interaction between two extreme charged dilaton black holes in the low-energy limit is investigated in (1+N) dimensions (N≥3). We find that there remains the residual velocity-dependent force in general cases, except for the case with N=a2.
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    Journal of Mathematical Physics 34 (1993), S. 622-644 
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    Notes: In this paper a description, à la Tulczyjew, of constrained time-dependent dynamical systems in terms of special symplectic manifolds is first developed. Next, this description is combined with the constraint algorithm for time-dependent constrained systems.
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    Journal of Mathematical Physics 34 (1993), S. 649-673 
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    Notes: Starting with a two-cocycle globally defined on a Lie group G, the Lagrangian system on G is constructed whose Lagrangian is quasi-invariant under a right translation canonically lifted to the tangent bundle TG. A direct consequence of the quasi-invariance is the appearance of central extensions in the Noether-symmetry algebra. Then, it is shown that the kinematical sector of such a model realizes, through a symplectic reduction, the Kirillov–Kostant symplectic structure on the coadjoint orbit of the Lie group with the central extensions. The generalization to a "higher-dimensional'' theory of the Wess–Zumino–Witten-type is also discussed herein.
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    Journal of Mathematical Physics 34 (1993), S. 674-680 
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    Notes: The Yang–Mills equations for gauge fields of an arbitrary semisimple Lie group G in Euclidean spaces Rn with dimension n≥4 is considered. For gauge fields Aa we introduce the ansätze which reduce the Yang–Mills equations in Rn to a set of nonlinear differential matrix equations (Rouhani–Ward equations). This permits us to write out the explicit form of cosmological, plane-wave, and other types of solutions.
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    Journal of Mathematical Physics 34 (1993), S. 737-748 
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    Notes: The gauge theoretical formulation of a frustrated Ising model is studied here. In this formulation the Chern–Simons term has played the key role. The inherent anisotropic feature of the system is associated with the order parameter which violates the commutativity of translation.
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    Journal of Mathematical Physics 34 (1993), S. 785-800 
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    Notes: The Luttinger model is revised with the emphasis on its infinite-volume formulation. The study poses the ground state problem for the model and shows the solvability of its associated collective excitations (zero-sound) equation.
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    Journal of Mathematical Physics 34 (1993), S. 805-817 
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    Notes: A method is developed that extends the nonlinearization procedure of eigenvalue problems to the discrete case, from which the finite-dimensional discrete systems and finite-dimensional completely integrable systems associated with the Toda hierarchy are obtained. A new model for solving discrete soliton equations is proposed, which enables one to get the solutions of the Toda lattice equations by solving the compatible systems of discrete equations and nonlinear ordinary differential equations.
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    Journal of Mathematical Physics 34 (1993), S. 885-885 
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    Journal of Mathematical Physics 34 (1993), S. 5441-5450 
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    Notes: Conditions are formulated under which a representation of an intrinsic C*- algebra of (often quasilocal) observables of an infinite system is appropriate to describe measurement-type processes: such a representation should allow for the description of robust experiments, it should be separable, and the pointer observable should be in its weak closure. If the pointer values are discrete the existence of such a measurement representation can be proven. If the pointer can take continuously many values, then the existence can only be proven under the additional assumptions of having an asymptotically Abelian system or dealing with type I representations. In the constructed measurement representations the pointer observable turns out to be classical. The structure of the representation suggests that spontaneous symmetry breaking might be a physical explanation of the emergence of the classical pointer.
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    Journal of Mathematical Physics 34 (1993), S. 5476-5492 
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    Notes: A q-deformation of the transformation of the Chevalley basis to an odd basis of generators of the universal enveloping of the Lie superalgebra G(n)≡osp(1||2n) is presented. It is shown that one thus obtains a reasonable quantum deformation of the algebra of n para-Bose oscillators.
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    Journal of Mathematical Physics 34 (1993), S. 5509-5532 
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    Notes: Techniques of Erickson and Yennie [Ann. Phys. N.Y. 35, 271 (1965)] are applied in an investigation of a simple Taylor's series which involves products of commutators and nested commutators and which represents the self-energy operator Σ of an electron in an external potential. A technique of "moving the parameter integrals to the mass'' leads to a relatively simple representation of all terms as a one-dimensional integral over a common virtual electron mass squared parameter. Although not a true expansion in powers of the external field, the method provides a window on the higher-order terms in the self-energy operator. Mass eigenfunction expansion concepts are shown to be quite useful in a discussion of infrared divergences.
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    Journal of Mathematical Physics 34 (1993), S. 610-621 
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    Notes: By means of some reasonable rules the operators that can represent arbitrary powers of the D'Alembertian and their corresponding Green's functions are defined. It is found which powers lead to the validity of Huygens' principle. The specially interesting case of powers that are half an odd integer in spaces of odd dimensionality, obey Huygens' principle, and can be expressed as iterated D'Alembertians of the retarded potential are discussed. Arbitrary powers of the Laplacian operator as well as their corresponding Green's functions are also discussed.
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    Journal of Mathematical Physics 34 (1993), S. 5596-5624 
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    Notes: In order to generalize the Wigner formula for the joint probability distribution of successive canonical measurements of discrete observables to continuous observables, a mathematical model is investigated of a canonical approximate measurement of an arbitrary observable, which generalizes von Neumann's model of measuring interaction and Davies's covariant instrument for approximate position measurement. Calculations of two types of root-mean-square errors show that this model clears certain requirements for good approximate measurements. A modified Wigner formula for successive canonical approximate measurements of arbitrary observables is established. It is also shown that the canonical approximate measurement of a discrete observable is reduced to the conventional measurement satisfying the von Neumann–Lüders collapse postulate by a minor modification in the process of measurement.
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    Journal of Mathematical Physics 34 (1993), S. 5770-5780 
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    Notes: The domain of attraction is determined in a small neigborhood of the tridimensional massless Gaussian fixed point, obtaining a critical surface in a manifold with one marginal and two relevant directions (besides the marginal direction due to the field strengh renormalization). The results are proven within the context of a hierarchical approximation.
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    Journal of Mathematical Physics 34 (1993), S. 5851-5871 
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    Notes: In this article the interrelationship between the integrable Kadomtsev–Petviashvili (KP) hierarchy, nonlinear Wˆ∞ algebra, and the conformal noncompact SL(2,R)/U(1) coset model at the classical level is studied. The Poisson brackets of the second Hamiltonian structure of the KP hierarchy is derived first explicitly, then the Wˆ1+∞ algebra and its reduction Wˆ∞ are defined. Then it is shown that the latter is realized in the SL(2,R)/U(1) coset model as a hidden current algebra, through a free field realization of Wˆ∞, in closed form for all higher-spin currents, in terms of two bosons. An immediate consequence is the existence of an infinite number of KP flows in the coset model, which preserve the Wˆ∞-current algebra.
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    Journal of Mathematical Physics 34 (1993), S. 5724-5746 
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    Notes: An analysis of a Green's function approach (based on wave splitting) to the one-dimensional electromagnetic inverse problem is given. The Green's functions refer to split components of the fundamental solution. The linear system of equations for the Green's functions is shown to be well-posed for the inverse problem and stability estimates, theorems on existence, uniqueness, local correctness, and convergence are given.
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    Journal of Mathematical Physics 34 (1993), S. 5801-5809 
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    Notes: Tzitzeica's class of surfaces in R3 is considered in connection with the inverse scattering method for the associated equation uxy=eu−e−2u. The Bäcklund transformation for this equation is derived from Tzitzeica's Darboux transformation for it.
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    Journal of Mathematical Physics 34 (1993), S. 5832-5842 
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    Notes: Motivated by Harish–Chandra theory, starting from a simple CDD-pole S matrix, a hierarchy of new S matrices involving ever "higher'' (in the sense of Barnes) gamma functions are constructed. These new S matrices correspond to scattering of excitations in ever more complex integrable models. From each of these models, new ones are obtained either by "q deformation,'' or by considering the Selberg-type Euler products of which they represent the "infinite place.'' A hierarchic array of integrable models is thus obtained. A remarkable diagonal link in this array is established. Though many entries in this array correspond to familiar integrable models, the array also leads to new models. Setting up this array led to new results on the q-gamma function and on the q-deformed Bloch–Wigner function.
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    Journal of Mathematical Physics 34 (1993), S. 5872-5896 
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    Notes: This article is devoted to constructing a quantum version of the famous Kadomtsev–Petviashvili (KP) hierarchy by deforming its second Hamiltonian structure, namely, the nonlinear Wˆ∞ algebra. This is achieved by quantizing the conformal noncompact SL(2,R)k/U(1) coset model, in which Wˆ∞ appears as a hidden current algebra. For the quantum Wˆ∞ algebra at level k=1, an infinite set of commuting quantum charges in explicit and closed form was successfully constructed. Using them, a completely integrable quantum KP hierarchy is constructed in the Hamiltonian form. A two-boson realization of the quantum Wˆ∞ currents has played a crucial role in this exploration.
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    Journal of Mathematical Physics 34 (1993), S. 5916-5923 
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    Notes: An exact spherically symmetric thin shell solution to the Einstein equations is obtained in the Weyl–Dirac theory with an oscillating scalar field. Boundary conditions are chosen such that the conformal invariance is broken in the interior space and the bubble has a scalar-field-induced surface stress-energy tensor that causes the thin shell to oscillate.
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    Journal of Mathematical Physics 34 (1993), S. 5159-5180 
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    Notes: This article studies a generalization of the Drinfel'd and Sokolov hierarchies for sln+1 and shows how the dressing transformation [as interpreted by Segal and Wilson, Publ. Math. IHES 61, 5 (1985)] produces a large class of almost globally analytic solutions. Many of these solutions are "of finite type,'' i.e., related to the Jacobian of a complete algebraic curve.
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    Journal of Mathematical Physics 34 (1993), S. 5781-5800 
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    Notes: A new method for solving the Hausdorff moment problem is presented which makes use of Pollaczek polynomials. This problem is severely ill posed; a regularized solution is obtained without any use of prior knowledge. When the problem is treated in the L2 space and the moments are finite in number and affected by noise or round-off errors, the approximation converges asymptotically in the L2 norm. The method is applied to various questions of statistical mechanics and in particular to the determination of the density of states. Concerning this latter problem the method is extended to include distribution valued densities. Computing the Laplace transform of the expansion a new series representation of the partition function Z(β) (β=1/kBT) is obtained which coincides with a Watson resummation of the high-temperature series for Z(β).
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    Journal of Mathematical Physics 34 (1993), S. 5320-5332 
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    Notes: The * isomorphism between algebraic extensions of the Lie fields of SO0(1,4) and the Poincaré group are considered herein. It is shown that the principal series of unitary ray representations of SO0(1,4) are associated, via the * isomorphism, with real mass, positive and negative energy representations of the Poincaré Lie algebra with arbitrary spin. Results on the most degenerate exceptional series of SO0(1,4) representations are also given.
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    Journal of Mathematical Physics 34 (1993), S. 4377-4420 
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    Notes: An algorithm for projecting a microscopic nuclear Hamiltonian with a central interaction onto the enveloping algebra of the Sp(6,R) group is presented in parallel with the development of a practical procedure for constructing the corresponding part of the Sp(6,R)&supuline;SO(3) integrity basis. The latter is shown to consist of the invariants of the monopole–quadrupole tensor and its polynomial analogs, coupling the collective and vortex spin degrees of freedom. The algorithm uses vector coherent-state techniques and is displayed on the basis of a generic Sp(6,R) irreducible representation. The collective Hamiltonian is also shown to be expandable in terms of the enveloping algebra of the (A−1)-dimensional rotational group, where A is the total number of nucleons.
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    Journal of Mathematical Physics 34 (1993), S. 4441-4454 
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    Notes: A general deformation of the Heisenberg algebra is introduced with two deformed operators instead of just one. This is generalized to many variables, and permits the simultaneous existence of coherent states, and the transposition of creation operators.
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    Journal of Mathematical Physics 34 (1993), S. 4478-4518 
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    Notes: This article gives a solution to an open problem in the paper by Arai [J. Math. Phys. 31, 2653 (1990)]. In it is presented an abstract asymptotic theory of families of unitary operators {U(κ)}κ(approximately-greater-than)0 and self-adjoint operators {Hκ}κ(approximately-greater-than)0 acting in the tensor product of two Hilbert spaces. It is proven that Hεren(V,κ), which represents a scaled total Hamiltonian of a coupled system of a one electron atom and a quantized radiation field, with parameters 0≤ε≤1, κ(approximately-greater-than)0, and the electron mass renormalized, is unitarily equivalent to an operator H˜εren(V,κ), which can be regarded as a decoupled Hamiltonian. Applying the abstract asymptotic theory and the unitary equivalence, it is proven that the resolvent of Hεren(V,κ) strongly converges as κ→∞ to an operator which defines an effective potential of the electron. The effective potential is compared with that obtained in the paper mentioned above.
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    Journal of Mathematical Physics 34 (1993), S. 5089-5108 
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    Notes: For an imperfect Bose gas consisting of massive particles and interacting through a long-range pair potential in a mean-field approximation, both in equilibrium and far from equilibrium, the dynamics are derived in the thermodynamic limit. This is done in the framework of the operator algebraic quantum theory. The limiting dynamics is formulated in the Schrödinger picture as a group of affine transformations of certain folia of physical states. Similar to the mean-field models for spin lattices, the algebra of quasilocal observables is not invariant under the Heisenberg dynamics in the GNS representation of general time invariant states. It is known that above critical density the infinite system exhibits condensation, and the condensate is characterized by the classical parameters density and phase. For these parameters a classical nonlinear equation of motion is derived.
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    Journal of Mathematical Physics 34 (1993), S. 4834-4839 
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    Notes: The fiber bundles and global rotations arising in the Kustaanheimo–Stiefel and Hurwitz transformations are studied. Generalized Cayley–Klein parameterization is introduced in a functional form and is used for the analysis of fibration in Hurwitz transformations. Essential differences in fibration structure between these transformations similar in Cartesian description are established in the angular map.
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    Journal of Mathematical Physics 34 (1993), S. 4857-4871 
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    Notes: Complex symplectic geometry is the study of complex manifolds admitting a global closed nondegenerate holomorphic two-form. Compact, simply connected complex symplectic manifolds are of interest for various reasons; for example, they always admit a Ricci-flat metric. In this work, the close relationship between the complex geometry of such manifolds and their Riemannian structures is exploited in order to obtain results in both directions: Riemannian techniques are used to obtain results on the complex automorphism group, and the problem of constructing examples of compact locally hyper-Kählerian manifolds with prescribed holonomy groups is discussed.
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    Journal of Mathematical Physics 34 (1993), S. 4898-4913 
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    Notes: A theory of Finslerian structures is presented using an unpublished method of Clifton. It consists of using Cartan's moving frame method with fields of special bases, and the Cartan calculus of tensor-valued forms with nonredundant coordinates on sphere bundles (which are the base spaces of the Finsler bundles). The formulation only requires a modicum of new concepts and does not involve Lagrangians at any fundamental level, including the definitions of metrics and connections. Finslerian connections on Riemannian (and even flat) metrics are discussed. The invariant forms of the sphere bundle of Minkowski space are obtained. The possibility of describing equations of motion through autoparallels, rather than extremals, is illustrated.
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    Journal of Mathematical Physics 34 (1993), S. 5283-5291 
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    Notes: Quasi exactly solvable equations are spectral equations which possess a finite number of algebraic eigenvectors. For a few of these equations, such as the Lamé equation, the number of algebraic solutions is larger than predicted by the general theory. A class of quasi exactly solvable equations in one variable is considered and the conditions under which a rich algebraization occurs is discussed. Families of equations, which by themselves are not quasi exactly solvable, but can be transformed into systems of coupled quasi exactly solvable equations, are discussed. These results suggest a scheme for the classification of quasi exactly solvable systems in one variable.
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    Journal of Mathematical Physics 34 (1993), S. 5357-5366 
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    Notes: An evolution equation of integro-differential type for a one-dimensional probability distribution of a linear process driven by additive randomly interrupted Gaussian white noise is exactly solved. A family of propagators for a probability distribution of the process is obtained. Selected examples of a time-dependent distribution are presented.
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    Journal of Mathematical Physics 34 (1993), S. 5407-5408 
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    Notes: The main formulas of the previous article are rewritten in a new and simple form. From the new form, the relation between the conservation laws of the quantized Davey–Stewartson I (DSI) system in (2+1) dimensions and that of the related systems in (1+1) dimensions can be very clearly seen. References and notations are the same.
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    Journal of Mathematical Physics 34 (1993), S. 4436-4440 
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    Notes: The phase-integral method is applied to the problem of quantum-mechanical tunneling in one-dimensional double-well potentials. Thus the results for the energy splitting of the nth level Δn up to the seventh-order of phase-integral approximation in the closed form in terms of the complete elliptic integrals are obtained. Furthermore the asymptotic approximations of the complete elliptic integrals to the first-order phase-integral result are used to calculate the quantity W(0) which appears in the expression for Δn obtained applying the LSZ procedure to the instanton-dominated Green function with 2n legs. Thus it is confirmed that the instanton calculus gives a correct value for the energy splitting of the nth level.
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    Journal of Mathematical Physics 34 (1993), S. 4469-4477 
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    Notes: An important example of characters on two-summable Fredholm modules are Schwinger terms arising in the commutators between charge and axial-charge operators. 1+1-dimensional massive fermions are discussed using the language of quasifree second quantization and for a large class of models the usual δ'-Schwinger term is obtained. The results confirm calculations within the massive Schwinger model at finite temperature but disagree with a conjecture concerning anomaly meltdown. The dependence of the Virasoro cocycle in the quasifree second-quantization framework on traceclass perturbations (like charging and thermalizing) are also investigated.
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    Journal of Mathematical Physics 34 (1993), S. 4562-4574 
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    Notes: An arbitrary Feynman graph for string field theory interactions is analyzed and the homeomorphism type of the corresponding world sheet surface is completely determined even in the nonorientable cases. Algorithms are found to mechanically compute the topological characteristics of the resulting surface from the structure of the signed oriented graph. Whitney's permutation-theoretic coding of graphs is utilized.
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    Journal of Mathematical Physics 34 (1993), S. 4601-4616 
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    Notes: On the basis of the Schwinger–Dyson variational method the recursion relations of the character expansion coefficients of the SU(N) gauge action are derived. Three recursion relations that are associated with the Casimir invariants of the second, third, and fourth orders are shown to be enough to determine the character expansion coefficient of every representation recursively in SU(N).
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    Journal of Mathematical Physics 34 (1993), S. 4755-4759 
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    Notes: It is shown that solutions of the exact reduced generalized Liouville-like equation, determining Petrov-type III gravitational fields within the Robinson–Trautman family of metrics, possess movable critical points, that is, they do not exhibit the Painlevé property.
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    Journal of Mathematical Physics 34 (1993), S. 89-99 
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    Notes: On the basis of the Schwinger–Dyson variational method the recursion relations of the character expansion coefficients of the U(N) gauge action are derived. Three recursion relations that are associated with the Casimir invariants are shown to be enough to determine the coefficients completely.
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    Journal of Mathematical Physics 34 (1993), S. 3878-3886 
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    Notes: The spectral properties of a Hamiltonian dependent on a parameter α are investigated. Due to the linearity in momentum and periodicity it was possible to strengthen some known results for the analogous kicked model. It is rigorously shown that, for any potential in a "large'' set, the spectrum is pure for each fixed value of α. Depending on the arithmetic character of α the spectrum is pure absolutely continuous, pure singular continuous, or pure point. It is also shown that in some sense the classical dynamics is identical to the quantum one.
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    Journal of Mathematical Physics 34 (1993), S. 3901-3917 
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    Notes: Covariant anomalies are studied in terms of the theory of secondary characteristic classes of the universal bundle of the Yang–Mills theory. A new set of descent equations is derived which contains the covariant current anomaly and the covariant Schwinger term. The counterterms relating consistent and covariant anomalies are determined. A geometrical realization of the Becchi–Rouet–Stora (BRS)/anti-BRS algebra is presented which is used to understand the relationship between covariant anomalies in different approaches.
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    Journal of Mathematical Physics 34 (1993), S. 3964-3979 
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    Notes: A representation of invariants in quantum mechanics for a general time-dependent Hamiltonian is provided. The main properties of these operators and their relevance for solving the Schrödinger equation are discussed in light of this representation. In particular, the well-known Lewis and Riesenfeld's method is shown to be recovered quite directly by the present approach. A detailed analysis is concerned with Hamiltonians which at each instant are elements of a finite dimensional Lie algebra. Exploiting the Wei and Norman's theory for such Hamiltonians, it is found that the evolution of a quantum system is always determined, in part or fully, by an invariant which belongs to the same algebra.
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    Journal of Mathematical Physics 34 (1993), S. 4014-4024 
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    Notes: It is proved that all bounded subsets of Rn with nonempty interior are cutable. Also found is an if and only if classification of when a nontrivial absolute steady state (ASS) of the sandpile-type cellular automata model will exist. The classification helps one to narrow down the geometrical structure of the ASS and is applicable to both Abelian and non-Abelian models. It is important for the future studies of self-organized criticality.
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    Journal of Mathematical Physics 34 (1993), S. 4050-4063 
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    Notes: The N=2 super W4 algebra is constructed as a certain reduction of the second Gel'fand–Dikii bracket on the dual of the Lie superalgebra of N=1 super pseudodifferential operators. The algebra is put in manifestly N=2 supersymmetric form in terms of three N=2 superfields Φi(X), with Φ1 being the N=2 energy momentum tensor and Φ2 and Φ3 being conformal spin 2 and 3 superfields, respectively. A search for integrable hierarchies of the generalized Korteweg-de Vries (KdV) variety with this algebra as Hamiltonian structure gives three solutions, exactly the same number as for the W2 (super KdV) and W3 (super Boussinesq) cases.
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