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  • 101
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    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 28 (1987), S. 690-696 
    ISSN: 1089-7658
    Source: AIP Digital Archive
    Topics: Mathematics , Physics
    Notes: This paper generalizes the results obtained by Kotecky. The free energy of the gauge Potts model in the external field in the many component limit has been calculated. This is done in two cases: (a) the external field is switched on after the gauge fixing or (b) the external field is switched on before the gauge fixing. In both cases, the free energy can be calculated using the mean-field method, if, in case (b), the larger class of trial measures is allowed. The mechanism of phase transition is also discussed.
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  • 102
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    Journal of Mathematical Physics 28 (1987), S. 697-704 
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    Topics: Mathematics , Physics
    Notes: Let φ be a relativistic scalar field fulfilling canonical commutation relations (CCR). Furthermore it is assumed that the time zero fields and momenta form an irreducible set. Based on estimates given by Herbst [I. W. Herbst, J. Math. Phys. 17, 1210 (1976)], and by methods developed by Powers [R. T. Powers, Commun. Math. Phys. 4, 145 (1967)], it is shown that φ has to be a free field in n〉3 space dimensions. For n=3 (resp. n=2) restrictions that look similar to the restriction in a formal :φ4:3+1 (resp. :φ6:2+1) theory are obtained.
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  • 103
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    Journal of Mathematical Physics 28 (1987), S. 711-716 
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    Notes: It is shown that the stochastic quantization of a fermion introducing an anisotropy in the internal space so that this gives rise to two internal helicities corresponding to particle and antiparticle leads us to describe a fermion as a Skyrme soliton. The Skyrme term appears here as a consequence of this internal anisotropy and can be treated as a quantum effect. Some topological properties of this fermionization are then discussed.
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  • 104
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    Journal of Mathematical Physics 28 (1987), S. 425-427 
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    Notes: The conditional convergence of the lattice sum defining the Madelung constant gives rise to an ambiguity in its value. It is shown that this ambiguity is related, through a simple and universal integral, to the average charge density on the crystal surface. The physically correct value is obtained by setting the charge density to zero. A simple and universally applicable formula for the Madelung constant is derived as a consequence. It consists of adding up dipole–dipole energies together with a nontrivial correction term.
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  • 105
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    Journal of Mathematical Physics 28 (1987), S. 445-447 
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    Topics: Mathematics , Physics
    Notes: The radiative correction of nonlinear sigma models on supermanifolds that have invertible metrics is investigated. It will be shown that the equation of motion for Riemannian supergravity (nonstandard supergravity) is derived from a consistency condition. This condition can be satisfied in the case of supergroup manifolds. We shall explicitly construct the model following the methods of Braaten, Curtright, and Zachos [E. Braaten, T. L. Curtright, and C. K. Zachos, Nucl. Phys. B 260, 630 (1985)] and of Witten [E. Witten, Commun. Math. Phys. 92, 455 (1984)]. Finally, super-Kac–Moody algebras of these models are derived.
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  • 106
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    Journal of Mathematical Physics 28 (1987), S. 134-137 
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    Notes: The quasiperiodic solutions to the discrete nonlinear Schrödinger equation are obtained by a variant of a method due to Date and Tanaka [E. Date and S. Tanaka, Suppl. Prog. Theor. Phys. 59, 107 (1976)]. It is shown explicitly that the nonlinear field variable at the different lattice points can be determined in a recursive fashion in terms of combinations of Reimann's functions depending on lattice position and time.
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  • 107
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    Journal of Mathematical Physics 28 (1987), S. 142-145 
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    Topics: Mathematics , Physics
    Notes: It is shown that the proofs of a series of classical singularity theorems of general relativity can be modified such that these theorems also state the maximality of the incomplete nonspacelike geodesics. Since along maximal incomplete nonspacelike geodesics with affine parameter u certain parts of the tidal curvature cannot blow up faster than (u¯−u)−2, where u¯ is the parameter value until which the geodesics cannot be extended, the classical singularity theorems do restrict the behavior of the curvature.
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  • 108
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    Journal of Mathematical Physics 28 (1987), S. 174-177 
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    Notes: On the Hilbert space H=L 2 (0,L), where (0,L) is a bounded interval of R1, the domain for the canonical commutation relation (CCR) and the CCR quasi-*-algebra is constructed. It is shown that the Bogolubov inequality for a Bose gas (in a box) is fulfilled.
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  • 109
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    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 28 (1987), S. 736-743 
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    Topics: Mathematics , Physics
    Notes: The momentum-moment formulation [Ann. Phys. (NY), 164, 47 (1985)] of Goedert and Lewis [J. Math. Phys. 28, XXX (1987)] and the momentum-resonance formulation of Lewis and Leach are used to study one-dimensional, time-dependent potentials that admit invariants which are rational functions of momentum with two or three simple poles. New examples are presented.
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  • 110
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    Journal of Mathematical Physics 28 (1987), S. 744-746 
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    Notes: In an ideal two-dimensional incompressible fluid, θ statistics for a pair of identical quantum point vortices is not well defined.
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  • 111
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    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 28 (1987), S. 747-747 
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  • 112
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    Journal of Mathematical Physics 28 (1987), S. 251-257 
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    Notes: A large class of nonelementary indecomposable representations of G=SU(2,2) is constructed and the invariant integral operators are found. An example describing a photon and a linear Weyl graviton field along with some auxiliary fields is studied. A nonsingular Lagrangian for the system is given. The pure, linear Weyl gravity with a conformal invariant gauge fixing condition arises as a particular case.
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  • 113
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    Journal of Mathematical Physics 28 (1987), S. 272-291 
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    Notes: All nontypical irreducible representations of the special linear Lie superalgebra sl(1,3) are considered. Explicit expressions for the transformation of the basis under the action of the generators are given. The results of this paper together with those obtained in Paper I [T. D. Palev, J. Math. Phys. 26, 1640 (1985)] solve the problem of the finite-dimensional irreducible representations of sl(1,3). The results are compared with those obtained by the Young supertableau technique. A mapping of the supertableau basis on the Gel'fand–Zetlin basis is given.
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  • 114
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    Journal of Mathematical Physics 28 (1987), S. 292-301 
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    Topics: Mathematics , Physics
    Notes: Using the method of extended Cartan matrices and extended Dynkin diagrams, a classification of maximal regular semisimple subalgebras of the basic classical Lie superalgebras is obtained. Especially in the case of exceptional Lie superalgebras, some curious inclusion relations are discovered.
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  • 115
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    Journal of Mathematical Physics 28 (1987), S. 258-271 
    ISSN: 1089-7658
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    Topics: Mathematics , Physics
    Notes: The Clebsch–Gordan coefficients for the product (1001)⊗(1001), where (1001) is the adjoint representation of SU(5), with respect to the group basis and the subgroup basis in the reduction SU(5)&supuline;SU(3)×SU(2)×U(1) are computed. One of the basic tools in this computation is the exhaustive use of the Verma algorithm to find bases for the weight subspaces of dimension higher than 1. It allows for the construction of bases in a systematic way by using the so-called Verma inequalities. Only the coefficients for the dominant weights are calculated. The other ones can be obtained by using the elements of finite order (charge conjugation operators) of SU(5).
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  • 116
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    Journal of Mathematical Physics 28 (1987), S. 319-322 
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    Topics: Mathematics , Physics
    Notes: A modified form of the anisotropic Heisenberg spin chain has been considered. By use of the prolongation structure technique of Wahlquist and Estabrook, the elliptic Lax pair associated with this equation has been deduced. A variant of the Reimann–Hilbert problem on the torus is used to indicate the way to the solution of the inverse problem.
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  • 117
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    Journal of Mathematical Physics 28 (1987), S. 302-306 
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    Notes: The well-known evolution equations associated to the homogeneous Heisenberg algebras of Kac–Moody algebras g(1) (AKNS systems) are extended by differential-difference equations that can be written in zero curvature form.
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  • 118
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    Journal of Mathematical Physics 28 (1987), S. 2951-2960 
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    Notes: A simple criterion for colliding gravitational plane waves is developed. This colliding wave condition is preserved by a new realization of the Geroch group augmented by a Kramer–Neugebauer involution. A three-parameter generalization of a two-parameter family of solutions with noncollinear polarization discovered recently by Ferrari, Ibañez, and Bruni is presented, and two additional solutions are derived that demonstrate that much larger families are likely to be constructed in the near future.
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  • 119
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    Journal of Mathematical Physics 28 (1987), S. 2975-2976 
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    Notes: By taking the electron densities of semi-infinite electron gases in one and in three dimensions, and forming the Slater sum by the Laplace transform, it is shown that the Slater sum is the classical partition function in d dimensions, times a function independent of dimensionality. The electron density is thereby calculated for general dimensionality, as is the kinetic energy density. As a by-product, the dimensionality dependence of Friedel oscillations emerges in general form.
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  • 120
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    Journal of Mathematical Physics 28 (1987), S. 2984-2989 
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    Notes: Matrix elements with respect to a discrete "Sturmian'' basis set of the operator r1/2gr1/2, where g is the Coulomb Green's function of the "second-order'' Dirac equation, are investigated. Closed expressions, involving Gaussian hypergeometric functions, can be obtained for the matrix elements. This calculation illustrates contour integration techniques capable of yielding closed expressions for a number of overlap integrals associated with the relativistic Kepler problem.
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  • 121
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    Journal of Mathematical Physics 28 (1987), S. 2994-2998 
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    Notes: The quark propagator in massless quantum chromodynamics (QCD) is analyzed using the gauge technique. In both the Feynman and Landau gauges with a Pauli–Villars cutoff, a chirally symmetric solution is found, while a nonsymmetric solution appears at a critical coupling λc〉0. As the cutoff is removed, λc tends to 0 but the nonsymmetric solution vanishes in the continuum limit, so that chiral symmetry is then restored.
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  • 122
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    Journal of Mathematical Physics 28 (1987), S. 2999-3005 
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    Notes: It is shown that streamfunctions g(k), k=1,2, can be defined to describe the two ionic states of a weakly dissociated electrolyte in the presence of a uniform applied electric field. These states comprise the dissociated state and the associated state and the g(k) are shown to be governed by a second-order partial differential equation. By consideration of characteristic numbers describing the two ionic states this equation is solved using similarity solutions. The association rate constant and relative increase in the dissociation constant due to the applied electric field are shown to have simple expressions in terms of the g(k). It is suggested that the streamfunctions are more natural functions with which to describe the mathematical properties of a weak electrolyte than the corresponding distribution functions. Some important mathematical properties of the streamfunctions are discussed.
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  • 123
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    Journal of Mathematical Physics 28 (1987), S. 412-424 
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    Notes: Using the Dyson equation repeatedly, starting with the Green's function for the infinite medium, the Green's function for the semi-infinite medium and finally the Green's function for a slab of a diatomic NaCl-type crystal using the Montroll–Potts model of nearest-neighbor central and noncentral forces are obtained.
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  • 124
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    Journal of Mathematical Physics 28 (1987), S. 428-437 
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    Notes: In this paper a generalized dynamical description of classical Yang–Mills theory will be presented. As a consequence of this work, a firm dynamical underpinning to the Batalin–Fradkin–Vilkovisky (BFV) formalism will emerge. This in turn will supply a precise geometric characterization of the ghost and conjugate ghost fields.
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  • 125
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    Journal of Mathematical Physics 28 (1987), S. 463-467 
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    Notes: In the context of quaternion valued fields spontaneous symmetry breaking and the Higgs mechanism are investigated. In particular, for the potential −(μ2/2)φ¯φ−(λ/4)(φ¯φ)2, Goldstone's theorem is studied and, for the gauge theory of automorphisms of the quaternions, a Higgs mechanism investigated.
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  • 126
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    Journal of Mathematical Physics 28 (1987), S. 468-471 
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    Notes: The classical improvement program in lattice gauge theory is examined from the geometric point of view. Improved actions are derived for pure gauge theories as well as for fermions.
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  • 127
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    Journal of Mathematical Physics 28 (1987), S. 2579-2585 
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    Notes: The multi-Hamiltonian structure of a class of nonlinear wave equations governing the propagation of finite amplitude waves is discussed. Infinitely many conservation laws had earlier been obtained for these equations. Starting from a (primary) Hamiltonian formulation of these equations the necessary and sufficient conditions for the existence of bi-Hamiltonian structure are obtained and it is shown that the second Hamiltonian operator can be constructed solely through a knowledge of the first Hamiltonian function. The recursion operator which first appears at the level of bi-Hamiltonian structure gives rise to an infinite sequence of conserved Hamiltonians. It is found that in general there exist two different infinite sequences of conserved quantities for these equations. The recursion relation defining higher Hamiltonian structures enables one to obtain the necessary and sufficient conditions for the existence of the (k+1)st Hamiltonian operator which depends on the kth Hamiltonian function. The infinite sequence of conserved Hamiltonians are common to all the higher Hamiltonian structures. The equations of gas dynamics are discussed as an illustration of this formalism and it is shown that in general they admit tri-Hamiltonian structure with two distinct infinite sets of conserved quantities. The isothermal case of γ=1 is an exceptional one that requires separate treatment. This corresponds to a specialization of the equations governing the expansion of plasma into vacuum which will be shown to be equivalent to Poisson's equation in nonlinear acoustics.
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    Journal of Mathematical Physics 28 (1987), S. 2741-2752 
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    Notes: For the stationary case the canonical formalism of thermally dissipative fields with both positive- and negative-frequency parts is constructed. This formulation enables one to follow the self-consistent renormalization scheme which creates the dissipation spontaneously. The self-interacting cursive-phi3 model is examined as an example of the spontaneous creation of dissipation. The parameter α appearing in the thermal state conditions as well as observables independent of the choice of α are discussed.
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  • 129
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    Journal of Mathematical Physics 28 (1987), S. 2614-2617 
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    Notes: It is shown within the Hilbert space formulation of quantum mechanics that the total noncommutativity of any two physical quantities is necessary for their satisfying the uncertainty relation or for their being complementary. The importance of these results is illustrated with the canonically conjugate position and momentum of a free particle and of a particle closed in a box.
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  • 130
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    Journal of Mathematical Physics 28 (1987), S. 2781-2785 
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    Notes: It is well known that, in doing light-cone gauge calculations, it is mandatory to regularize the unphysical (q n)−β poles by use of the Leibbrandt–Mandelstam prescription. This technique is also applied to general axial gauges and it is proved that it is a suitable regularization procedure for these gauges as well. In order to find the relation between the Leibbrandt prescription and the more familiar principal value prescription with its simpler Lorentz structure the temporal gauge limit n→0 is performed (within dimensional regularization). Although this limit is found to be singular for multiple poles, the analytically regularized one-loop integrals agree with the results obtained within the principal value technique for the temporal gauge.
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    Journal of Mathematical Physics 28 (1987), S. 2259-2267 
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    Notes: When expressed in terms of the trace, the characters of SU(2) are known to be related with the Chebyshev polynomials of second kind. It is shown that those of the first kind also play a fundamental role. If A∈SU(2) and t=Tr A, then fn(t)=Tr(An), fn (2 cos θ)=sin nθ/sin θ, ln(t) =Tr(An), ln (2 cos θ)=2 cos nθ, where An denotes the representative of A in the irrep of dimension n. Other polynomials related with them are of interest. They are (i) the "primordial'' polynomials Pn (every fn or ln can be expressed in a unique way in terms of Pd, where d is a divisor of n), (ii) the "factorial'' polynomials fn!=f1 f2⋅⋅⋅fn which occur in a natural way in the representations, (iii) the gn polynomials appearing in the generating functions of powers of fn.
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    Journal of Mathematical Physics 28 (1987), S. 2801-2803 
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    Notes: Kalita and Bujarbarua [J. Phys. A: Math. Gen. 16, 439 (1983)] obtained a set of equations to describe the nonlinear propagation of ion acoustic waves in a warm magnetoplasma and made a numerical study of these equations for particular values of the physical parameters. In this paper a rigorous and general analytical study is presented. Some simple necessary and sufficient conditions for solitary wave solutions are derived and it is also shown that cavity solutions are not possible.
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    Journal of Mathematical Physics 28 (1987), S. 2317-2322 
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    Notes: A systematic method for constructing particular solutions of the nonlinear Klein–Gordon and Liouville equations in four-spatial dimensions is developed. The method of solution presented here first consists of reducing nonlinear partial differential equations to ordinary differential equations (ODE's) by introducing symmetry variables and then seeking exact solutions for more tractable ODE's. Various exact solutions are presented, in which new solutions with nonspherical symmetries are included. Furthermore, the exact method is applied to the above equations in general n-spatial dimensions. Among them, a conformally invariant nonlinear Klein–Gordon equation is particularly interesting from the viewpoint of field theories. The exact solutions for these equations are generalizations of those for the corresponding equations in four-spatial dimensions.
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    Journal of Mathematical Physics 28 (1987), S. 2323-2324 
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    Notes: Faithful icosahedral symmetry exists only for tensors of rank higher than 5. The most relevant tensor of this type is the one for third-order elastic constants C(3)ijklmn defined by the series expansion Tij=C(2)ijklεkl+ 1/2 C(3)ijklmnεklεmn +⋅⋅⋅ of the stress tensor T in terms of the deformation tensor ε. A basis for those tensors in (R3)⊗6 that are invariant under a certain action of both the icosahedral group S2×A5 and the wreath product S2∼S3 of the symmetric groups S2 and S3 are evaluated.
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    Journal of Mathematical Physics 28 (1987), S. 2705-2713 
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    Notes: Kinematic and dynamic expressions are derived for the Lie derivative of vorticity along a particle world line in a rigid motion. It is found that the evolution of vorticity in a rigid motion is governed by the electric part of the Weyl tensor. Necessary and sufficient kinematic and dynamic conditions are established for a rotating rigid motion to be isometric.
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    Journal of Mathematical Physics 28 (1987), S. 2726-2730 
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    Notes: In quantum statistics there are four categories of quantum degeneracy: nondegenerate, weak, intermediate, and strong. These are associated with the Fermi–Dirac and Bose–Einstein integrals, which are difficult to evaluate over the entire range of the activity parameter r defined as the particle density divided by the quantum concentration. In this paper (I), four classical systems with r(very-much-less-than)1, and four weakly degenerate systems with r(approximately-less-than)1 are examined. In the former, the Maxwell–Boltzmann distribution is sufficient. In the latter, the treatment of Landau and Lifschitz is extended. Physically realistic systems, like electrons in intrinsic and impurity semiconductors, and noble gases at different pressures and temperatures, are investigated. The neutrino and neutral pion systems are illustrative, albeit esoteric. Expressions for the quantum concentration for different dimensions and particle velocities are useful in predicting the onset of degeneracy. In the companion paper (II), intermediate and strong degeneracies are studied for r≥1.
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    Journal of Mathematical Physics 28 (1987), S. 2753-2762 
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    Notes: Grassmannian σ models are reexamined in the light of a new geometrical result. Namely, the Cartan immersion of a Riemannian symmetric space G/H into its isometry group G is not always a diffeomorphism onto the set Mσ introduced by Eichenherr and Forger [Nucl. Phys. B 164, 528 (1980)]. This is the case, in particular, for Grassmann manifolds of all types: their set Mσ is shown to be disconnected and its structure is completely analyzed. As a consequence, a new constraint must be introduced in the Bäcklund transformation (BT) method proposed by Harnad, Saint-Aubin, and Shnider [Commun. Math. Phys. 92, 329 (1984)]. It is shown, however, to always be satisfied for Grassmann manifolds of compact type (i.e., G compact), but the problem remains open in most other cases. On the other hand, the BT method is extended to the Euclidean regime.
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    Journal of Mathematical Physics 28 (1987), S. 2731-2738 
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    Notes: Interaction of a small system S with a large reservoir R amounts to thermal relaxation of the reduced system density operator ρS(t). The presence of the reservoir enters the equation of motion for ρS(t) through the reservoir correlation functions fkl(τ) (defined in the text), which decay to zero for τ→∞ on a time scale τc. Commonly, this τc is much smaller than the inverse relaxation constants for the time evolution of ρS(t). Then a series of approximations can be made, which lead to a Markovian equation of motion for ρS(t). In this paper the assumption of a small reservoir correlation time is removed. The equation of motion for ρS(t) is solved, and it appears that the memory effect, due to τc(approximately-equal-to)(Slashthrough accent mark)0, can be incorporated in a frequency dependence of the relaxation operator Γ˜(ω). Subsequently, (unequal-time) quantum correlation functions of two system operators are considered, where explicit expressions for (the Laplace transform of) the correlation functions are obtained. They involve again the relaxation operator Γ˜(ω), which accounts for the time regression. Additionally it is found that an initial-correlation operator Υ˜(ω) arises, as a consequence of the fact that the equal-time correlation functions do not factorize as ρS(t) times the reservoir density operator. It is pointed out that the frequency dependence of Γ˜(ω) and the occurrence of a nonzero T˜(ω) both arise as a result of τc(approximately-equal-to)(Slashthrough accent mark)0, and should therefore be treated on an equal footing. Explicit evaluation of Γ˜(ω) and Υ˜(ω) shows that their matrix elements can be expressed entirely in f˜kl(ω), just as in the Markov approximation. Hence no essential complications appear if one should go beyond the limits of a small reservoir correlation time τc.
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    Journal of Mathematical Physics 28 (1987), S. 1864-1874 
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    Notes: A system of charged zero-spin bosons in the presence of a uniform magnetic field is studied using a relativistic spinor formalism. Equations of motion for the relevant operators are developed. The eigenfunctions of two different sets of commuting operators are obtained by the use of ladder operators and also by direct solution of the Klein–Gordon equation in both coordinate and momentum representations. Matrix elements are calculated which will be required in later consideration of the collisionless conductivity and dielectric tensors for the boson–antiboson plasma in a strong magnetic field (see papers II and III in this series).
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    Journal of Mathematical Physics 28 (1987), S. 1912-1919 
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    Notes: The occurrence of variables at infinity in the dynamics of gauge models (in positive gauges) as a result of the Coulomb-type interaction is rigorously shown in two-dimensional quantum electrodynamics, in the Coulomb gauge. The general structures associated to the algebraic dynamics of systems with long-range interactions, like the removal of the infrared cutoff, the effective dynamics, the classical motion of the variables at infinity, and their relevance for the generalization of the Goldstone theorem and the spectrum of the generalized Goldstone bosons, are explicitly shown in this model; in particular, the chiral symmetry breaking and the associated mass generation is discussed in detail. The analogous results for the chiral Schwinger model are briefly summarized.
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    Journal of Mathematical Physics 28 (1987), S. 893-900 
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    Notes: The field equations for axially symmetric gravitational fields in 4+K dimensions with K-dimensional toroidal compatification can be reduced to those of a generalized nonlinear sigma model. The dual symmetry of this model is considered first. Then the soliton transformations for these equations are derived using the method of Belinskii and Zakharov consequently generalizing their results to the higher-dimensional case. From the result of one-soliton transformation, a series of discrete symmetries generalizing the Neugebauer–Kramer transformation in the four-dimensional case are obtained. The basic properties of these new transformations are studied.
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    Journal of Mathematical Physics 28 (1987), S. 901-904 
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    Notes: The solutions of vacuum Einstein equations in 4+K dimensions with 2+K commuting Killing vectors under the Abelian Kaluza–Klein ansatz are considered. This system admits Belinskii–Zakharov-type soliton transformations. The explicit formulas for general N-soliton transformations are obtained by iterating the formulas for one-soliton transformation.
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    Journal of Mathematical Physics 28 (1987), S. 929-934 
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    Notes: The quantum mass corrections to static periodic solitons are considered and expressed in terms of a functional quantity, the discriminant of the Hill's operator appearing. Several general expansions for this and hence the mass corrections are given. In particular, the connection with integrable systems and inverse scattering is clearly seen; this enables one to obtain simple expressions for these corrections.
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    Journal of Mathematical Physics 28 (1987), S. 921-928 
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    Notes: Coexistence of periodic points is investigated in area-preserving reversible dynamical systems on a plane which are not necessarily close to an integrable one. It is shown that on the symmetry axis a higher cycle implies a lower cycle and any cycle implies an infinite number of higher cycles. The standard map is investigated as an example. It is shown that k-cycles for any k≥2 densely fill the phase plane of the map as the parameter goes to infinity. In addition, the number of these cycles are estimated.
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    Journal of Mathematical Physics 28 (1987), S. 1972-1977 
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    Notes: The method of formal series is applied to the construction of nonlinear representations of Poincaré's group in three dimensions. The first term of the series must be a linear massless representation. In the special case of discrete helicities, the cocycles of extension of these representations by their tensor product with a nonzero quadratic term are determined. It turns out that a nonlinear representation must have a helicity zero representation as leading term. It is proved by induction how to avoid the successive obstructions to the computation of each term in the series.
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    Journal of Mathematical Physics 28 (1987), S. 1697-1699 
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    Notes: The prolongation structure approach of Wahlquist and Estabrook [J. Math. Phys. 16, 1 (1975)] is used effectively in a new situation in relation to the integrodifferential type BO equation (the Benjamin–Ono equation). The main clue lies in the possible differential equation representation of such equations in three dimensions. Here it is shown how the usual analysis of prolongation structure can be utilized to deduce a Lax pair for a BO type equation in three dimensions. Effectiveness of the present approach is further demonstrated by an independent derivation of some conservation laws associated with the equation. Last, the whole formalism is reduced to two dimensions to make contact with known results.
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    Journal of Mathematical Physics 28 (1987), S. 1700-1708 
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    Notes: Distinguished involutions called transposition and conjugation in the algebra of complex supernumbers are introduced. On the base of these involutions an analysis is developed over complex superspaces. Consistency of integration under supertransformations between two complex superspaces is shown.
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    Journal of Mathematical Physics 28 (1987), S. 1729-1731 
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    Notes: The head-wave contribution to a reflection is investigated by two different methods and it is shown that the new result presented by Lerche and Hill [J. Math. Phys. 26, 1420 (1985)] for the head-wave amplitude is in error due to the use of an inappropriate mathematical method.
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    Journal of Mathematical Physics 28 (1987), S. 1732-1742 
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    Notes: In this paper the results of a search for bilinear equations of the type P(Dx, Dt)F ⋅ F=0, which have three-soliton solutions, are presented. Polynomials up to order 8 have been studied. In addition to the previously known cases of KP, BKP, and DKP equations and their reductions, a new polynomial P=DxDt(Dx2 +(square root of)3DxDt+Dt2) +aDx2+bDxDt +cDt2 has been found. Its complete integrability is not known, but it has three-soliton solutions. Infinite sequences of models with linear dispersion manifolds have also been found, e.g., P=DxMDtNDyP, if some powers are odd, and P=DxMDtN(Dx2 −1)P, if M and N are odd.
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    Journal of Mathematical Physics 28 (1987), S. 1761-1763 
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    Notes: The proof of a result analogous to that in Koelman and de Muynck [Phys. Lett. A 98, 1 (1983)] is given for the case of unbounded observables. If two, not necessarily bounded, observables are represented by a positive operator-valued measure, then the measurement of any of them is undisturbed if and only if they commute. The Naimark theorem on dilations of spectral functions is exploited. A stronger version of Wigner's theorem is given.
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    Journal of Mathematical Physics 28 (1987), S. 1801-1808 
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    Notes: The energy eigenvalues for the Hulthén, Yukawa, and exponential-cosine screened Coulomb potentials are calculated in the 1/N expansion. States with up to three nodes in the wave functions are considered. We obtain the perturbative results up to the order of λ8, where λ is the screening parameter.
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    Journal of Mathematical Physics 28 (1987), S. 1809-1812 
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    Notes: The Painlevé criterion has been applied to the supersymmetric nonlinear Schrödinger equation. This particular system of fermionic and bosonic fields shows up a rich spectrum of resonances and it can be explicitly proved that the expansion coefficients at the resonance positions can remain arbitrary. At this point is is worth noting that even when the extra nonlinear field (which is fermionic in this case) is considered to be bosonic, the resulting system turns out to satisfy the Painlevé test so that this second system may be thought of as a new completely integrable system whose Lax pair is still to be found.
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    Journal of Mathematical Physics 28 (1987), S. 1840-1843 
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    Notes: Any theory constructed out of the metric tensor and its derivatives can also be regarded as a theory constructed out of a frame field and its derivatives. In general, the converse is not true. It is shown that with the additional assumption that the theories are Lorentz invariant the converse is true. Theories involving the metric spinor and its derivatives are then included in this equivalence and the various interrelationships are studied.
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    Journal of Mathematical Physics 28 (1987), S. 1858-1863 
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    Notes: Using techniques of quantum stochastic calculus, a dilation scheme is developed to describe the evolution of a two-level atom, which is initially in a (nontracial) Gibbs state, through a radiation field. The Wigner–Weisskopf approximation is assumed but not the rotating wave approximation, the latter being shown to be equivalent to the requirement that the dilation satisfies the quantum detailed balance condition with respect to the initial state.
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    Journal of Mathematical Physics 28 (1987), S. 1875-1882 
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    Notes: The field-diffeomorphism anomalies in the nonlinear σ model are explicitly discussed, using the spectral sequences technique. The role of the Riemannian constraints is analyzed for low space-time dimensions.
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    Journal of Mathematical Physics 28 (1987), S. 1883-1885 
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    Notes: Fibers of the exterior bundle over a Lorentzian manifold can be given the structure of a Clifford algebra. The minimal left ideals of this Clifford algebra may be interpreted as spinors. In order to better understand spinorial properties of the Kähler equation in a curved space-time, conditions for the Lorentzian connection to preserve these ideals are examined.
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    Journal of Mathematical Physics 28 (1987), S. 1924-1927 
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    Notes: A near-field approximation dealing with the cosmological field near a typical freely falling observer is developed within the framework established in the preceding paper [J. Math. Phys. 28, xxxx(1987)]. It is found that for the matter-dominated era the standard cosmological model of general relativity contains the Newtonian cosmological model, proposed by Zel'dovich, as its near-field approximation in the observer's globally geodesic coordinate system.
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    Journal of Mathematical Physics 28 (1987), S. 1471-1472 
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    Notes: A new uniqueness theorem is established for the inverse Sturm–Liouville problem. It is shown that the measurement of a particular eigenvalue for an infinite set of different boundary conditions is sufficient to determine the unknown potential.
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    Journal of Mathematical Physics 28 (1987), S. 1473-1476 
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    Notes: A plausibility argument presented by the first two authors in an earlier paper [J. Math. Phys. 26, 3042 (1985)] concerning the existence of partially invariant solutions for some equations of the Fokker–Planck type is made precise by the explicit construction of one such solution. In the process a substantial simplification of Ovsiannikov's method for finding partially invariant solutions is achieved. In addition, the class of partially invariant solutions obtained by Ovsiannikov for the equations of transonic flow of a gas is enlarged.
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    Journal of Mathematical Physics 28 (1987), S. 1492-1498 
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    Notes: It is proved that, in the context of a conformal causal structure, (a) any acceleration field decomposes uniquely into the sum of an affine structure that is compatible with the conformal structure and an n-force, and (b) any directing field, such that the n-force of the corresponding family of acceleration fields is due to tensor fields and is orthogonal to the n-velocity, uniquely decomposes into a projective structure that is compatible with the conformal structure and an (n−1)-force. Moreover, if there are no second clock effects and variable rest masses do not exist, there exists a unique pseudo-Riemannian metric on space-time that determines the unique standard of no acceleration for all massive monopoles. It follows from this that a non-null result for the Eötvös experiment entails the existence of a fifth force rather than a violation of the universality of free fall.
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    Journal of Mathematical Physics 28 (1987), S. 1508-1511 
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    Notes: For particles of spin 1/2 a class of distributions closely related to Wigner's is introduced on dynamical grounds. It is found that they may be refined to give correct expectation values of higher powers of spin components, but depart somewhat from a criterion that has been used in characterizing the Wigner distribution. For a special choice amongst this class, a more subtle refinement is possible satisfying this criterion exactly. This requires, however, a dubious distinction at every point between positive spin about a direction and negative spin about the reverse direction.
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    Journal of Mathematical Physics 28 (1987), S. 1526-1534 
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    Notes: A model Hamiltonian for a many-electron system which unifies superconductivity, charge density waves, and spin density waves is analyzed. It is shown that the spectrum generating algebra for this system is su(8), and all 63 generators of this Lie algebra are identified. The seven symmetry operators that are broken in transition to the condensed state are identified, together with 56 order operators, whose expectations give the order parameters of the various phases present in the model. The discrete symmetry properties of these operators are tabulated. A chain of subalgebras of submodels with corresponding decoupled phases is constructed. Finally, how the finite temperature Green's functions may be obtained and used to solve the problem of self-consistency of the order parameters in the model is indicated.
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    Journal of Mathematical Physics 28 (1987), S. 573-583 
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    Notes: In geometric quantization it is well known that, if f is an observable and F a polarization on a symplectic manifold (M,ω), then the condition "Xf leaves F invariant'' (where Xf denotes the Hamiltonian vector field associated to f ) is sufficient to guarantee that one does not have to compute the BKS kernel explicitly in order to know the corresponding quantum operator. It is shown in this paper that this condition on f can be weakened to "Xf leaves F+F° invariant''and the corresponding quantum operator is then given implicitly by formula (4.8); in particular when F is a (positive) Kähler polarization, all observables can be quantized "directly'' and moreover, an "explicit'' formula for the corresponding quantum operator is derived (Theorem 5.8). Applying this to the phase space R2n one obtains a quantization prescription which ressembles the normal ordering of operators in quantum field theory. When we translate this prescription to the usual position representation of quantum mechanics, the result is (a.o) that the operator associated to a classical potential is multiplication by a function which is essentially the convolution of the potential function with a Gaussian function of width (h-dash-bar), instead of multiplication by the potential itself.
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    Journal of Mathematical Physics 28 (1987), S. 592-597 
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    Notes: The d-dimentional space-continuous time-discrete Markovian random walk with a distribution of step lengths, which behaves like x−(α+d) with α〉0 for large x, is studied. By studying the density–density correlation function of these walks, it is determined under what conditions the walks are fractal and when they are nonfractal. An ensemble average of walks is considered and the lower entropy dimension D of the set of stopovers of the walks in this ensemble is calculated, and D=min{2,α,d} is found. It is also found that the fractal nature of the walks is related to a finite value of the mean first passage time. The crossover of the correlation function from the fractal to nonfractal regimes is studied in detail. Finally, it is conjectured that these results for the lower entropy dimension apply to a wide class of symmetric Markov processes.
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    Journal of Mathematical Physics 28 (1987), S. 598-604 
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    Notes: The Hamiltonian of the three-dimensional hydrogen atom is reduced, in parabolic coordinates, to the Hamiltonians of two bidimensional harmonic oscillators, by doing several space-time transformations,separating the movement along the three parabolic directions (ξ,η,φ), and introducing two auxiliary angular variables ψ and ψ', 0≤ψ, ψ'≤2π. The Green's function is developed into partial Green's functions, and expressed in terms of two Green's functions that describe the movements along both the ξ and η axes. Introducing auxiliary Hamiltonians allows one to calculate the Green's function in the configurational space, via the phase-space evolution function of the two-dimensional harmonic oscillator. The auxiliary variables ψ and ψ' are eliminated by projection. The thus-obtained Green's function, save for a multiplicating factor, coincides with that calculated following the path-integral formalism.
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    Journal of Mathematical Physics 28 (1987), S. 605-611 
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    Notes: A family of the Morse oscillators with certain quantized coupling constants are described as composite objects in the framework of the SO(4,2) dynamical group scheme. Although a single Morse oscillator can be solved by the subgroup SO(2,1) of SO(4,2) this SO(2,1) is not the spectrum generating group], the set of all energy levels is given by the representation of another particular one-parameter subgroup of SO(4,2), which is the dynamical group of a single Morse oscillator. The continuous spectra of this oscillator and other variations of the Morse potential are also discussed by making an analytic continuation from the Morse potential well to the Morse barrier.
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    Journal of Mathematical Physics 28 (1987), S. 1237-1242 
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    Notes: The universal enveloping algebra U=U+U−H of the Poincaré algebra iso(3,1) is considered. Infinite-dimensional induced modules U+(Γ) are studied. Explicit formulas are obtained for U+(Γ) in the Poincaré–Birkhoff–Witt basis. Then a change of basis is performed to an energy-cyclic angular momentum basis. For any Γ∈C2, U+(Γ) turns out to be indecomposable. It can be represented as an infinite family of interacting Verma modules of the Lorentz algebra so(3,1). Finite-dimensional modules can be obtained as quotient modules of U+(Γ) if 2Γ∈Z2.
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    Journal of Mathematical Physics 28 (1987), S. 1243-1249 
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    Notes: A systematic procedure is presented to solve analytically differential equations for Grassmann variables with the most general nonlinearity. The method consists in the reduction of the original equation to its simplest form (normal form). The classes of solvable normal forms are determined only by the structure of the linear part of the original equation and are parametrized in terms of the number of critical eigenvalues.
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    Journal of Mathematical Physics 28 (1987), S. 1250-1260 
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    Notes: The application of Lie-group methods to a system of coupled nonlinear partial differential equations representing what is usually called a Madelung fluid is shown. The generating operators of the transformation group that depends on five arbitrary group constants will be constructed, and all subclasses of systems of ordinary differential equations derived by similarity reduction will be presented in tabular form. Two subclasses of physical interest are investigated in detail and the similarity solutions are compared with solutions found earlier by the application of inverse scattering transform techniques to the cubic nonlinear Schrödinger equation. Similarity solutions for the Madelung equations with linear external potential Γ(x)=−f0x are presented.
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    Journal of Mathematical Physics 28 (1987), S. 1283-1286 
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    Notes: Nonlinear equations defined by a positive definite, elliptic operator and nonlinear functions are considered. It is proved that a unique solution exists for a wider class of problems than previously determined, which may be approximated by an iterative method. These results are shown to hold for an equation arising in some reaction-diffusion phenomena.
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    Journal of Mathematical Physics 28 (1987), S. 1265-1274 
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    Notes: When xt and xt+1 represent two random variables, each belonging to a real interval [0,1] and being related by a first-order difference equation xt+1=F(xt), called a discrete-time map, the probability density distribution connected with xt can be translated into that associated with xt+1. This yields an evolution equation by means of which one can construct an infinite sequence {wt(x)||t∈N, x∈[0,1]} starting from an integrable function w0(x) normalized to unity on [0,1]. The question of the convergence of the sequence toward a so-called invariant density function w(x) as t→+∞ and the problem of finding this limit were examined by a number of authors, mostly studying isolated cases. The present paper solves the problem for a class of discrete-time maps characterized by xt+1 =f(||sn[l sn−1f−1(xt)]||), l∈{2,3,...}, whereby f is a real, continuous, monotonically increasing function mapping [0,1] onto itself and sn is the usual symbol for the sinelike Jacobian elliptic function with modulus k∈[0,1] (including the sine function). Convergence is proven under very general conditions on w0(x) and an explicit formula to calculate w(x) is established. Some properties of w(x) are discussed. A necessary and sufficient condition for the symmetry of w(x) about x= 1/2 is obtained and attention is also devoted to the inverse problem, leading to a reformulation of the discrete-time map of the type cited above which corresponds to a given invariant density. The examples of practical application considered here cover almost all special cases which were treated in the literature thus far, as well as new cases.
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    Journal of Mathematical Physics 28 (1987), S. 1293-1314 
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    Notes: The problem of the scattering of an electromagnetic plane wave with arbitrary polarization and angle of incidence from a perfectly conducting spherical shell with a circular aperture is solved with a generalized dual series approach. This canonical problem encompasses coupling to an open spherical cavity and scattering from a spherical reflector. In contrast to the closed sphere problem, the electromagnetic boundary conditions couple the TE and TM modes. A pseudodecoupling of the resultant dual series equations system into dual series problems for the TE and TM modal coefficients is accomplished by introducing terms that are proportional to the associated Legendre functions P−m0. The solutions of the TE and TM dual series problems require the further introduction of terms proportional to P−mn, where 0≤n〈m. These functions effectively complete the standard spherical harmonic basis set when an aperture is present and guarantee the satisfaction of Meixner's edge conditions. Having generated the modal coefficients, all desired electromagnetic quantities follow immediately. Numerical results for the currents induced on the open spherical shell and for the energy density of the field at its center are presented for the case of normal incidence.
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    Journal of Mathematical Physics 28 (1987), S. 1315-1326 
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    Notes: Quantum mechanics for internal motions of the three-body system is set up on the basis of the complex vector bundle theory. The three-body system is called a triatomic molecule in the Born–Oppenheimer approximation. The internal states of the molecule are described as cross sections in the complex vector bundle assigned by an eigenvalue of the square of the total angular momentum operator. This bundle is equipped with a linear connection, which is a natural consequence of a geometric interpretation of the so-called Eckart condition. The coupling of the internal motion with the rotation is understood naturally in terms of this connection. The internal Hamiltonian operator is obtained which includes the internal motion–rotation coupling and a centrifugal potential. The complex vector bundle for the triatomic molecule proves to be a trivial bundle, though the geometric setting for the internal motion is independent of whether the bundle is trivial or not.
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    Journal of Mathematical Physics 28 (1987), S. 1287-1289 
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    Notes: It has been well proved that there are infinitely many resonances in the scattering problem provided the potential V(t) satisfies the moment conditions ∫∞0||V(t)||tn dt =O(n(1−ε)n), ε〉0, n=0,1, ... . In particular, if V(t) has a compact support then the result of Rollnik [H. Rollnik, Z. Phys. 145, 654 (1956)] and Regge [T. Regge, Nuovo Cimento, 8, 671 (1958)] is obtained and if ||V(t)||∼exp(−τt1+ε), τ,ε〉0, we have the results of Sartori [L. Sartori, J. Math. Phys. 4, 1408 (1963)].
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    Journal of Mathematical Physics 28 (1987), S. 1290-1292 
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    Notes: The trilinear commutation relations involving coordinates and momenta introduced by Wigner [E. P. Wigner, Phys. Rev. 77, 711 (1950)] are generalized to three dimensions. It is shown that the only realizable coordinate space representation of the momenta implies the usual bilinear commutation relations.
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    Journal of Mathematical Physics 28 (1987), S. 1327-1340 
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    Notes: An observer whose instantaneous "here-now'' has Minkowski coordinates zλ(λ=0,1,2,3) can only be aware of events within or on the past light cone with vertex at zλ. In conventional quantum mechanics his current quantum state would refer to some spacelike surface containing zλ, for example, x0=z0. This is, however, a region of space-time about which the observer can know nothing except the single event zλ, his current here-now. The aim of the present paper is to give a version of quantum mechanics in which the intrinsically unknowable "quantum state at the present time'' is replaced by the "quantum state on the past light cone.'' The theory is an extension and adaptation of Dirac's point mechanics [Rev. Mod. Phys. 21, 392 (1949)].
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    Journal of Mathematical Physics 28 (1987), S. 1344-1350 
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    Notes: The structure of the Korteweg–de Vries hierarchy of evolution equations, generating isospectral transformations, is elucidated by means of a study of its recurrence relations. For the mth member of the KdV hierarchy, which can be written in the form Vt=−2Am+1,x, where the Ai satisfy the recurrence relation Am+1,x=VAm,x+ 1/2 AmVx− 1/4 Am,xxx, it is shown that Am is a homogeneous polynomial in ∂iV/∂xi. A general combinatorial formula for the coefficients of all the monomials entering Am, up to a set of constants determined by means of a recurrence relation, is derived.
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    Journal of Mathematical Physics 28 (1987), S. 1364-1369 
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    Notes: A mechanism by which space-time topological modifications could have been controlled, in the early universe or at the Planck length, to enable onset of spinor structure is investigated. This mechanism (based on a reshuffling of topological charges and related modification of characteristic classes) could provide a gravitational analog of the Aharonov–Susskind Gedankenexperiment proposed to detect relative rotation in the universe, spinor behavior, or to keep track of the two homotopy classes of the Lorentz Lie group. The space-time topology [and in particular the trivial (nontrivial) bundle structure at conformal null infinity] provide a labeling of the asymptotic Lorentz homotopy classes which originates in the first Chern class (enclosed magnetic mass) or in the parametrization of the second homology group, and gives rise to a necessary (and sufficient) condition for the existence of spinor structure. This underlines the intertwined roles of topology and curvature. The mechanism could also be viewed as an "unwinding'' of gravitational magnetic monopoles with one asymptotic region into electric mass (black-hole) solutions with two asymptotic regions. In such situations a discrete PT symmetry could emerge from a continous transformation. Possible implications on the CPT theorem are mentioned.
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    Journal of Mathematical Physics 28 (1987), S. 1383-1384 
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    Notes: For the special case when the scalar field is massless and conformally invariant, it is shown that there do not exist spherically symmetric conformally flat solutions in a new scalar–tensor theory proposed by Schmidt et al. [Phys. Rev. D 24, 1484 (1981)] representing disordered radiation and in the presence of a source-free electromagnetic field except for the trivial empty flat space-time of Einstein's theory. The solution in the vacuum case is also only a flat space-time of Einstein's theory.
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    Journal of Mathematical Physics 28 (1987), S. 1389-1393 
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    Notes: In two previous papers [J. Math. Phys. 27, 1 (1986) (I); 28, (square, solid) (square, solid) (square, solid) (1987) (II)] simple mathematical procedures are developed for averaging the particle energy ε, raised to any power p≥1 over Maxwell–Boltzmann, Bose–Einstein, and Fermi–Dirac distributions. In I, the particle energy is treated nonrelativistically: ε=p2/2m. In II, the particle energy is treated ultrarelativistically: ε=pc. Here, the particle energy is treated relativistically ε2=p2c2+m20c4. For each distribution function, expressions are obtained for the chemical potential, internal energy, and heat capacity for two cases: (kT/m0c2)2(very-much-less-than)1 and (m0c2/kT)2(very-much-less-than)1.
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    Journal of Mathematical Physics 28 (1987), S. 1416-1419 
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    Notes: Properties of a mode announced in a previous paper are proved. This involves some complicated calculations in linear algebra, and observation of the structure of a function of several complex variables.
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    Journal of Mathematical Physics 28 (1987), S. 1430-1439 
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    Notes: A class of non-Markovian stochastic processes is defined; it generalizes several anterior models, and allows a trajectorial description of collisions in dense fluids when the system loses all memory at each collision. The abstract formalism is studied here: an integral evolution equation is derived, as well as an integrodifferential equation that generalizes the master equation; some asymptotic properties of these processes are established. Applications to specific models will be treated in other articles.
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    Journal of Mathematical Physics 28 (1987), S. 1005-1015 
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    Notes: The theory of R-separation of variables is developed for the time-dependent Hamilton–Jacobi and Schrödinger equations on a Riemannian manifold V n where time-dependent vector and scalar potentials are permitted. As an application it is shown how to obtain all R-separable coordinates for the n-sphere and Euclidean n-space.
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    Journal of Mathematical Physics 28 (1987), S. 1023-1029 
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    Notes: Expressions are found for homogeneous and inhomogeneous propagators for vector fields of arbitrary mass in anti-de Sitter space-time using a generalization of Stueckelberg's Lagrangian for a massive vector field. The massless case (quantum electrodynamics) is also considered by taking the appropriate zero-mass limit.
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    Journal of Mathematical Physics 28 (1987), S. 1036-1051 
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    Notes: A general method is presented for analytically calculating linear stability limits for symplectic maps of arbitrary dimension in terms of the coefficients of the characteristic polynomial and the Krein signatures. Explicit results are given for dimensions 4, 6, and 8. The codimension and unfolding are calculated for all cases having a double eigenvalue on the unit circle. The results are applicable to many physical problems, including the restricted three-body problem and orbital stability in particle accelerators.
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    Journal of Mathematical Physics 28 (1987), S. 1052-1055 
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    Notes: In Hirota's [Hiroshima University Technical Report Nos. A 6, A 9, 1981; J. Phys. Soc. Jpn. 50, 3785 (1981)] bilinear difference equation which is satisfied by solutions to the Kadomtsev–Petviashvili (KP) hierarchy, gauge and dual symmetries are found, which enable one to reduce the problem of solving the nonlinear equation to solving a single linear equation.
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    Journal of Mathematical Physics 28 (1987), S. 1061-1068 
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    Notes: The factorization of the wave equation into a coupled system involving up-and down-going wave components is obtained for the case where the field quantities are multivariate functions of spatial variables, but the velocity c is a function of the z variable only. The form of the reflection operator is derived and the quadratic differential-integral equation satisfied by its kernel is obtained.
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    Journal of Mathematical Physics 28 (1987), S. 1080-1088 
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    Notes: Two-cluster–two-cluster scattering amplitudes for N-body quantum systems are studied. Our attention is restricted to energies below the lowest three-cluster threshold. For potentials falling off like r−1−δ it is proved that in this energy range these amplitudes exist, are continuous, and that the asymptotic completeness holds. Moreover, if the potentials fall off exponentially it is proved that these amplitudes can be meromorphically continued in the energy, with square root or logarithmic branch points at the two-cluster thresholds.
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    Journal of Mathematical Physics 28 (1987), S. 1094-1096 
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    Notes: Using Madelung's hydrodynamical variables, it is shown that the bi-Hamiltonian structure of the nonlinear Schrödinger equation goes over to a bi-Hamiltonian structure of the shallow water wave equations in the classical limit.
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    Journal of Mathematical Physics 28 (1987), S. 1069-1074 
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    Notes: The old problem of light scattering from a perfectly conducting surface is addressed. An electromagnetic field is incident upon the boundary, where it induces a charge and current distribution. These charges and currents emit the reflected fields. A set of equations for the charges and currents on the surface is derived by eliminating the E and B fields from Maxwell's equations with the aid of the appropriate boundary conditions. An explicit and general solution is achieved, which reveals the confinement and redistribution of the charge and the current on the surface by the external field. Expressions are obtained for the surface resolvents, or the redistribution matrices, which represent the surface geometry. Action of a surface resolvent on the incident field, evaluated at the surface, then yields the charge and current distributions. The Faraday induction appears as an additional contribution to the charge density. Subsequently, the reflected fields are expanded in spherical waves, which have the surface-multipole moments as a source. Explicit expressions are presented for the surface-multipole moments, and it is pointed out that charge conservation on the surface sets constraints on these moments. The results apply to arbitrarily shaped surfaces and to any incident field. For a specific choice of the surface structure and the external field, the solutions for the charge, the current, and the reflected fields are amenable to numerical evaluation.
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    Journal of Mathematical Physics 28 (1987), S. 2977-2981 
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    Notes: The concepts of void and cluster for an arbitrary point distribution in a domain D are defined and characterized by some parameters such as volume, density, number of points belonging to them, shape, etc. After assigning a weight to each void and cluster—which is a function of its characteristics—the concept of distance between two point configurations S1 and S2 in D is introduced, both with and without the help of a lattice in the domain D. This defines a topology for the point distributions in D, which is different for the different characterizations of the voids and clusters.
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    Journal of Mathematical Physics 28 (1987), S. 2990-2993 
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    Notes: Using dimensional regularization, the lowest-order electron self-energy function in an arbitrary covariant gauge is derived. For off-mass-shell electrons, the usual expression for the finite portion Σ f of the self-energy as the number of space-time dimensions n approaches 4 is recovered. In the case of on-mass-shell electrons, the condition (p(Slashthrough accent mark)−m)Σ f→0 as p(Slashthrough accent mark)→m, which is necessary to make the usual separation of the renormalization constant unambiguous, requires that n approach 4 from above, i.e., n→4+. This necessary condition on Σ f is not satisfied by the off-mass-shell expression in the limit p2→m2 due to a branch point in the self-energy operator.
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    Journal of Mathematical Physics 28 (1987), S. 1146-1158 
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    Notes: The results of numerical investigations based on series analysis indicate clearly that the method of phantom fields constructs nontrivial, self-interacting scalar Euclidean boson field theories. It is found that these continuum theories arise as the scaling limit to normal critical points of lattice statistical mechanical models. The character of these theories is numerically indistinguishable from that of a classical theory on the lambda line near the tricritical point.
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    Journal of Mathematical Physics 28 (1987), S. 1114-1117 
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    Notes: Two new exact analytical solutions to Einstein's field equations representing static fluid spheres with anisotropic pressures are presented. One solution has a maximum value of mass of about 0.42 times the radius of the fluid sphere, dictated by causality and the corresponding values for the surface red shift and the central red shift are 1.58 and 9.03, respectively. The other solution has a maximum mass of about 0.435 times the radius of the fluid sphere and the corresponding red shifts from the surface and from the center are 1.77 and 16.28, respectively. In the low mass limit both solutions reduce to the constant density Schwarzschild interior solution.
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    Journal of Mathematical Physics 28 (1987), S. 1137-1139 
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    Notes: The counterterms in the Lagrangian of a renormalizable quantum field theory that involve the Riemann curvature tensor are considered. It is proved that for six or fewer dimensions the counterterms not containing derivatives of the Riemann tensor are linearly independent. It is shown that there appears to be a maximum space-time dimension for which identities can exist among invariants involving the product of n Riemann tensors (without derivatives acting on them.) Space-times that would require these products as counterterms for a renormalizable theory have a dimensionality which is one higher than this maximum dimension. This makes it plausible that the required set of counterterms not involving derivatives of the Riemann tensor is linearly independent in arbitrary dimensions. In the Appendix, a relation cubic in the Weyl tensor, which relates invariants cubic in the Riemann tensor in five dimensions, is proved.
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    Journal of Mathematical Physics 28 (1987), S. 1192-1197 
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    Notes: The embedding of the dynamical algebra U(M/N) of nuclear supersymmetries in larger algebraic structures is studied. A noncompact Z2⊕Z2 graded color superalgebra SpO(2M/1/2N/0) is identified as a receptacle for various chains containing boson and fermion (super) algebras. The existence of a generalized quasispin algebra is demonstrated and discussed.
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    Journal of Mathematical Physics 28 (1987), S. 1206-1208 
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    Notes: A "rigorous proof'' is presented that the critical exponent γ of the susceptibility χ takes its mean field value in d〉4 dimensions for ferromagnets with single spin measure in the Brydges–Fröhlich–Spencer class, modulo a numerical calculation of a certain function I(d) of dimension d. This class of ferromagnets contains, for example, the Ising spin model and lattice scalar cursive-phi4 model.
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    Journal of Mathematical Physics 28 (1987), S. 1209-1209 
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    Journal of Mathematical Physics 28 (1987), S. 2639-2649 
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    Notes: It is well known that the n-fermion algebra is a complex Clifford algebra of dimension 22n with the orthogonal group O(2n,C) as group of automorphisms. The n-boson algebra viewed similarly as a complex "symplectic Clifford'' algebra is investigated. It is of infinite dimension and has the symplectic group Sp(2n,C) as a group of automorphisms. Special attention is given to the case n=1 and various bases. In particular, the matrix elements of the bases between harmonic oscillator states and their relation with special functions are investigated.
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    Journal of Mathematical Physics 28 (1987), S. 2655-2661 
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    Notes: The probability is estimated that at a given frequency ω the action of an external, monochromatic radiation field acting on a hydrogen atom yields a fixed positive convergence radius of the Rayleigh-Schrödinger perturbation expansion for the quasienergy resonances.
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