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  • 1
    Electronic Resource
    Electronic Resource
    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 13 (1981), S. 1-8 
    ISSN: 0066-4189
    Source: Annual Reviews Electronic Back Volume Collection 1932-2001ff
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  • 2
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 13 (1981), S. 79-95 
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  • 3
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 13 (1981), S. 189-216 
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  • 4
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 13 (1981), S. 351-378 
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  • 5
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 13 (1981), S. 379-397 
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  • 6
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 14 (1982), S. 1-12 
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  • 7
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 14 (1982), S. 13-37 
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  • 8
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 14 (1982), S. 61-85 
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  • 9
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 14 (1982), S. 153-187 
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  • 10
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 14 (1982), S. 189-212 
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  • 11
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 14 (1982), S. 261-283 
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  • 12
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 14 (1982), S. 235-259 
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  • 13
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 14 (1982), S. 365-393 
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  • 14
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 27 (1995), S. 45-88 
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  • 15
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 27 (1995), S. 335-373 
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  • 16
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 27 (1995), S. 17-43 
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  • 17
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 27 (1995), S. 257-292 
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  • 18
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 28 (1996), S. 83-128 
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  • 19
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 27 (1995), S. 293-334 
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  • 20
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 28 (1996), S. 11-43 
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  • 21
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 28 (1996), S. 187-213 
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  • 22
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 28 (1996), S. 215-248 
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    Source: Annual Reviews Electronic Back Volume Collection 1932-2001ff
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  • 23
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 28 (1996), S. 323-360 
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  • 24
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 28 (1996), S. 477-539 
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    Source: Annual Reviews Electronic Back Volume Collection 1932-2001ff
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  • 25
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 13 (1981), S. 399-423 
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  • 26
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 14 (1982), S. 87-130 
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  • 27
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 14 (1982), S. 131-151 
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  • 28
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 14 (1982), S. 213-234 
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  • 29
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 14 (1982), S. 285-311 
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  • 30
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 14 (1982), S. 313-345 
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  • 31
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 14 (1982), S. 347-364 
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  • 32
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 14 (1982), S. 395-442 
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  • 33
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 27 (1995), S. 89-113 
    ISSN: 0066-4189
    Source: Annual Reviews Electronic Back Volume Collection 1932-2001ff
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  • 34
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 27 (1995), S. 515-539 
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  • 35
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 28 (1996), S. 1-9 
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  • 36
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 28 (1996), S. 389-428 
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  • 37
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 28 (1996), S. 429-476 
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  • 38
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 13 (1981), S. 33-55 
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  • 39
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 13 (1981), S. 9-32 
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  • 40
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 13 (1981), S. 57-77 
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  • 41
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 13 (1981), S. 157-187 
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  • 42
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 13 (1981), S. 97-129 
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  • 43
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 13 (1981), S. 131-156 
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  • 44
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 13 (1981), S. 231-252 
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  • 45
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 13 (1981), S. 217-229 
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  • 46
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 13 (1981), S. 253-272 
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  • 47
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 13 (1981), S. 273-326 
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  • 48
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 13 (1981), S. 329-350 
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  • 49
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 13 (1981), S. 457-515 
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  • 50
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 14 (1982), S. 39-60 
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  • 51
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 27 (1995), S. 375-417 
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 27 (1995), S. 115-168 
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  • 53
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 28 (1996), S. 249-278 
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  • 54
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    Palo Alto, Calif. : Annual Reviews
    Annual Review of Fluid Mechanics 28 (1996), S. 361-387 
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    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 37 (1996), S. 3854-3881 
    ISSN: 1089-7658
    Source: AIP Digital Archive
    Topics: Mathematics , Physics
    Notes: The invariant imbedding technique, via the solution of a Riccati-type equation, is modified to calculate the wave fields inside and scattered from a strongly (laterally and vertically) heterogenous, anisotropic inclusion, which may be large but remains compact. The factorization underlying this approach is carried out with respect to direction of average power flow rather than the more conventional factorization with respect to local direction of propagation. The solution of the operator Riccati equation is related to the Dirichlet-to-Neumann map. The formulation is robust in the sense that it can handle a rather extreme range of modal wave speeds, and allows continuous as well as discontinuous medium variations on different (wave) length scales. It also, inherently, takes care of critical-angle phenomena. The algorithm, based on the invariant imbedding approach, yields the internal fields for a full survey of sources and receivers simultaneously. The wave field solution in the inclusion is coupled to the external field via a boundary element approach. © 1996 American Institute of Physics.
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    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 37 (1996), S. 3954-3972 
    ISSN: 1089-7658
    Source: AIP Digital Archive
    Topics: Mathematics , Physics
    Notes: In this paper we show that a quasi-exactly solvable (normalizable or periodic) one-dimensional Hamiltonian satisfying very mild conditions defines a family of weakly orthogonal polynomials which obey a three-term recursion relation. In particular, we prove that (normalizable) exactly solvable one-dimensional systems are characterized by the fact that their associated polynomials satisfy a two-term recursion relation. We study the properties of the family of weakly orthogonal polynomials defined by an arbitrary one-dimensional quasi-exactly solvable Hamiltonian, showing in particular that its associated Stieltjes measure is supported on a finite set. From this we deduce that the corresponding moment problem is determined, and that the kth moment grows like the kth power of a constant as k tends to infinity. We also show that the moments satisfy a constant coefficient linear difference equation, and that this property actually characterizes weakly orthogonal polynomial systems. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 4053-4061 
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    Notes: Expressions for the complete metric and vector potential perturbations of solutions of the Einstein–Maxwell equations with a null background electromagnetic field in terms of two complex scalar potentials are derived using Wald's method of adjoint operators. The perturbations of the Bell–Szekeres solution, in the regions prior to the collision of the plane-fronted waves, are obtained by this approach. We find that there exist nontrivial u-independent perturbations (where ∂u defines the direction of propagation of the colliding wave) which, when the electromagnetic perturbation vanishes, are exact solutions of the Einstein–Maxwell equations. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 3933-3953 
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    Notes: We discuss several aspects of second quantized scattering operators Sˆ for fermions in external time-dependent fields. We derive our results on a general, abstract level having in mind as a main application potentials of the Yang-Mills type and in various dimensions. We present a new and powerful method for proving the existence of Sˆ which is also applicable to other situations like external gravitational fields. We also give two complementary derivations of the change of phase of the scattering matrix under generalized gauge transformations which can be used whenever our method of proving the existence of Sˆ applies. The first is based on a causality argument, i.e., Sˆ (including phase) is determined from a time evolution, and the second exploits the geometry of certain infinite-dimensional group extensions associated with the second quantization of one-particle operators. As a special case we obtain a Hamiltonian derivation of the axial fermion-Yang-Mills anomaly and the Schwinger terms related to it via the descent equations, which is on the same footing and traces them back to a common root. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 3354-3374 
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    Notes: Description of the grand canonical Gibbs ensemble for classical continuous systems in terms of the nonlocally perturbed infinite-divisible generalized random fields is presented. The equivalence of the traditional description with the ones presented here on the level of DLR equations is established. The antiferromagnetism for the purely repulsive interactions has been observed. Finally, the usefulness of our description for an analysis of the high-temperature cluster expansion has been demonstrated. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 3415-3421 
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    Notes: A higher-order nonlocal evolution equation describing internal waves in a deep fluid is shown to be asymptotically integrable only if the coefficients of the higher-order terms satisfy certain constraints. In this case, the nonlocal equation can be transformed to the integrable Benjamin–Ono equation. The asymptotic integrability of the reductions of the higher-order evolution equation to a complex Burgers equation, to an envelope-wave equation, and to a finite-dimensional dynamical system is also considered. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 3483-3490 
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    Notes: Lie superalgebraic methods are used to establish a connection between the huge Lie superalgebra Xi of super- (pseudo-) differential operators and various super KP-hierarchies. We show in particular that Xi splits into 5=2×2+1 graded algebras expected to correspond to five classes of super-KP-hierarchies generalizing the well-known Manin–Radul and Figueroa–Mas–Ramos supersymmetric KP-hierarchies. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 3539-3547 
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    Notes: The massless spin 2 free-field equation is studied in the Robertson–Walker space–time via the Newman–Penrose formalism and separated by using a Chandrasekhar–Teukolski method. The resulting temporal and angular equations are explicitly integrated. The radial equations are solved in the flat universe case. The closed universe case shows, in principle, the existence of a discrete spectrum of the energy of the massless particles. In the general case of spin greater than 2 the massless field equations are shown to be separable by induction. The separated equations admit the same recurrence structure and analog interpretation properties of the spin 2 and less than 2 cases. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 3522-3538 
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    Notes: The perennial formalism is applied to the real, massive Klein–Gordon field on a globally-hyperbolic background space–time with compact Cauchy hypersurfaces. The parametrized form of this system is taken over from the accompanying paper. Two different algebras Scan and Sloc of elementary perennials are constructed. The elements of Scan correspond to the usual creation and annihilation operators for particle modes of the quantum field theory, whereas those of Sloc are the smeared fields. Both are shown to have the structure of a Heisenberg algebra, and the corresponding Heisenberg groups are described. Time evolution is constructed using transversal surfaces and time shifts in the phase space. Important roles are played by the transversal surfaces associated with embeddings of the Cauchy hypersurface in the space–time, and by the time shifts that are generated by space–time isometries. The automorphisms of the algebras generated by this particular type of time shift are calculated explicitly. The construction of the quantum theory using the perennial formalism is shown to be equivalent to the Segal quantization of a Weyl system if the time shift automorphisms of the algebra Scan are used. In this way, the absence of any timelike Killing vector field in the background space–time leads naturally to the "problem of time'' for quantum field theory on a background space–time. Within the perennial formalism, this problem is formally identical to the problem of time for any parametrized system, including general relativity itself. Two existing strategies—the "scattering'' approach, and the "algebraic'' approach—for dealing with this problem in quantum field theory on a background space–time are translated into the language of the perennial formalism in the hope that this may give some insight into how the general problem can be solved. The non-unitary time evolution typical of the Hawking effect is shown to be due to global properties of the corresponding phase space: specifically, the time shifts map a global transversal surface to a non-global one. Thus, the existence of this effect is closely related to the global time problem. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 2569-2584 
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    Notes: The most general Skyrme–Sigma models in two and three Euclidean dimensions described by O(3) and O(4) fields, respectively, are studied first by numerical methods, and analytic proofs of existence are subsequently given. Particular emphasis is given to the special cases of these models, where the topological inequalities can be saturated by self-duality equations. The O(d+1) models in d dimensions exhibit qualitatively similar features. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 2637-2642 
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    Notes: Sufficient conditions for the existence of the infimum AΛB of two quantum effects A and B are given. The existence of AΛB is characterized for commuting A and B with pure point spectrum. Properties of a generalized infimum and supremum are studied. Some previous finite dimensional, commutative results are extended to the infinite dimensional and noncommutative case. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 2674-2681 
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    Notes: We derive a general expression for the transformation brackets between the chains U(ν+1)&supuline;U(ν)&supuline;SO(ν) and U(ν+1)&supuline;SO(ν+1)&supuline;SO(ν) for ν≥2. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 2694-2730 
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    Notes: A class of free quantum fields defined on the Poincaré group is described by means of their two-point vacuum expectation values. They are not equivalent to fields defined on the Minkowski space–time and they are "elementary'' in the sense that they describe particles that transform according to irreducible unitary representations of the symmetry group, given by the product of the Poincaré group and of the group SL(2,C) considered as an internal symmetry group. Some of these fields describe particles with positive mass and arbitrary spin and particles with zero mass and arbitrary helicity or with an infinite helicity spectrum. In each case the allowed SL(2,C) internal quantum numbers are specified. The properties of local commutativity and the limit in which one recovers the usual field theories in Minkowski space–time are discussed. By means of a superposition of elementary fields, one obtains an example of a field that presents a broken symmetry with respect to the group Sp(4,R) that survives in the short-distance limit. Finally, the interaction with an accelerated external source is studied and it is shown that, in some theories, the average number of particles emitted per unit of proper time diverges when the acceleration exceeds a finite critical value. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 2787-2795 
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    Notes: After reviewing the complete Lie group for the full Boltzmann equation, it is shown that projective transformations play a special role in the general case, and the class of invariant solutions giving rise to homoenergetic affine flows is presented. Homoenergetic affine flows in the two-dimensional case [potential U(r)∝r−2] are considered in detail: It is shown that the general solution of this problem can be essentially simplified by projective transformations. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 2824-2850 
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    Notes: A discrete system of coupled waves (with nonanalytic dispersion relation) is derived in the context of the spectral transform theory for the Ablowitz–Ladik spectral problem (discrete version of the Zakharov–Shabat system). This 3-wave evolution problem is a discrete version of the stimulated Raman scattering equations, and it is shown to be solvable for arbitrary boundary value of the two radiation fields and initial value of the medium state. The spectral transform is constructed on the basis of the ∂-approach. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 2872-2891 
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    Notes: We define a complete set of supertraces on the algebra SHN(ν), the algebra of observables of the N-body rational Calogero model with harmonic interaction. This result extends the previously known results for the simplest cases of N=1 and N=2 to arbitrary N. It is shown that SHN(ν) admits q(N) independent supertraces, where q(N) is a number of partitions of N into a sum of odd positive integers, so that q(N)(approximately-greater-than)1 for N≥3. Some consequences of the existence of several independent supertraces of SHN(ν) are discussed, such as the existence of ideals in associated W∞-type Lie superalgebras. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 2955-2968 
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    Notes: We reformulate Special Relativity by a quaternionic algebra on reals. Using real linear quaternions, we show that previous difficulties, concerning the appropriate transformations on the 3+1 space–time, may be overcome. This implies that a complexified quaternionic version of Special Relativity is a choice and not a necessity. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 2815-2823 
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    Notes: The free streaming operator T is considered in a convex three dimensional region V, with diffusive multiplying boundary conditions. Some mathematical properties of T are examined by writing the particle density as an infinite series which takes into account successive reflections on ∂V, and by introducing an operator which in some sense annihilates the multiplying effect of ∂V. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 2602-2627 
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    Notes: In this paper we investigate the canonical quantization of a non-Abelian topologically massive Chern–Simons theory in which the gauge fields are minimally coupled to a multiplet of scalar fields in such a way that the gauge symmetry is spontaneously broken. Such a model produces the Chern–Simons–Higgs mechanism in which the gauge excitations acquire mass both from the Chern–Simons term and from the Higgs–Kibble effect. The symmetry breaking is chosen to be only partially broken, in such a way that in the broken vacuum there remains a residual non-Abelian symmetry. We develop the canonical operator structure of this theory in the broken vacuum, with particular emphasis on the particle-content of the fields involved in the Chern–Simons–Higgs mechanism. We construct the Fock space and express the dynamical generators in terms of creation and annihilation operator modes. The canonical apparatus is used to obtain the propagators for this theory, and we use the Poincaré generators to demonstrate the effect of Lorentz boosts on the particle states. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 3022-3031 
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    Notes: A new set of polynomial states (to be called character states) are derived for Sp(4) reduced to its SU(2)×U(1) subgroup, and the relevant generator matrix elements are evaluated for generic representations (a,b) of Sp(4). [The degenerate representations (a,0) and (0,b) were treated in our previous work and are also given in this paper]. The group–subgroup in question is that of the seniority model of nuclear physics. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 3050-3061 
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    Notes: The preliminary classification of qt=f(q,qx,qxx,qxxx) is given. The results are compared with Fokas's symmetry and Mikhailov–Shabat–Sokolov formal symmetry approaches. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 2682-2693 
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    Notes: In the Bayesian theory of statistical inference, as first suggested by Harold Jeffreys in highly influential work, one can employ the square root of the determinant of an n×n Fisher information matrix as a reparametrization-invariant prior (generally unnormalized) measure over an n-dimensional family (Riemannian manifold) of probability distributions. Jeffreys' ansatz is adopted here to the quantum context, that is, with regard to density matrices rather than probability distributions, by computing the quantum Fisher information matrices (associated with Helstrom and Holevo) for the three-, five-, and eight-dimensional convex sets of two-level complex, two-level quaternionic, and three-level complex systems, respectively. In both the two-level cases, the priors have been normalized to probability distributions over the 2×2 density matrices, while, in the much more computationally demanding three-level situation, no such normalization has been accomplished. An argument is made for the general form, in terms of eigenvalues, that the (unnormalized) prior should assume over the (n2−1)-dimensional convex set of n×n density matrices. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 2748-2761 
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    Notes: The Manev problem (a two-body problem given by a potential of the form A/r+B/r2, where r is the distance between particles and A,B are positive constants) comprises several important physical models, having its roots in research done by Isaac Newton. We provide its analytic solution, then completely describe its global flow using McGehee coordinates and topological methods, and offer the physical interpretation of all solutions. We prove that if the energy constant is negative, the orbits are, generically, precessional ellipses, except for a zero-measure set of initial data, for which they are ellipses. For zero energy, the orbits are precessional parabolas, and for positive energy they are precessional hyperbolas. In all these cases, the set of initial data leading to collisions has positive measure. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 2796-2814 
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    Notes: We discuss how to apply the dimer method to Ising models on group lattices having nontrivial topological genus g. We find that the use of group extension and the existence of both external and internal group isomorphisms greatly reduces the number of distinct Pfaffians and leads to explicit topological formulas for their sign and weight in the expansion of the partition function. The complete solution for the Ising model on the Klein lattice group L(2,7) with g=3 is given. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 2851-2862 
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    Notes: In this paper, a class of degenerate (i.e., associated to a degenerate Poisson structure) completely integrable systems is studied which generalizes the so-called odd and even master systems introduced and studied by Mumford and by Vanhaecke. It is shown that all these completely integrable systems, called the generalized master systems, admit a multi-Hamiltonian formulation, and a systematic construction of this multi-Hamiltonian structure is described. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 2892-2905 
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    Notes: The relationship between the two well-behaved coordinate systems of Lemaiˆtre–Tolman–Novikov, and Kruskal–Szekeres–Penrose indicates that the Schwarzschild R=0 singularity is intrinsically nonsimultaneous. It follows that the simultaneous synchronous coordinates of Wald and Yip do not exist on the complete Schwarzschild manifold. In the process, the coordinate transformations between the Schwarzschild exterior model in its various common coordinate systems and the vacuum Lemaiˆtre–Tolman model (which includes Novikov coordinates and the closed Kantowski–Sachs model) is derived. It is also shown that, contrary to statements in the literature, the closed Kantowski–Sachs model is well-behaved limit of the Lemaiˆtre–Tolman model. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 2969-2978 
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    Notes: The solutions of a system of homogeneous first-order quasilinear evolution equations for which the propagation velocity depends only on the field value are characterized by their invariance under a particular type of flow. All simple wave solutions are shown to have this property. The local images of simple wave solutions are the integral curves of a system of ordinary differential equations on the field space. The model for barotropic compressible flow is an example of a system that has invariant solutions of higher rank. A solution of this system is invariant under the flow of the convective derivative if and only if it is divergence-free. The evolution of initial data is shown to be divergence-free if and only if its differential is nilpotent. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 3014-3021 
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    Notes: It is well known that knots are countable in ordinary knot theory. Recently, knots with intersections have raised a certain interest, and have been found to have physical applications. We point out that such knots—equivalence classes of loops in R3 under diffeomorphisms—are not countable; rather, they exhibit a moduli-space structure. We characterize these spaces of moduli and study their dimension. We derive a lower bound (which we conjecture being actually attained) on the dimension of the (nondegenerate components) moduli spaces, as a function of the valence of the intersection. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 2376-2387 
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    Notes: The unitary irreducible representations of the central extension of the Poincaré group in 1+1 dimensions are constructed by an application of the Kirillov theory. These are then lifted to projective unitary irreducible representations of the Poincaré group. The 1+1 Galilean group is treated separately in an appendix. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 2426-2456 
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    Notes: Induced invariant forms and the multiplicity labeling problem are investigated for typical summands of the tensor product of an arbitrary finite dimensional irreducible representation and a typical one, for the type I quantum superalgebras. The results are applied to obtain a general eigenvalue formula for Casimir invariants, corresponding to an arbitrary finite dimensional irreducible reference representation. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 2400-2425 
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    Notes: A point group symmetrized boson representation (SBR) is introduced that is particularly convenient for describing molecular vibrations. In this paper the SBR is elucidated using the example of the molecule SF6 with Oh symmetry. The advantages of the SBR are that its basis vectors have a clear physical picture, their number is very small (equal to one-eighth of the dimension of the reducible representation for Oh), and the irreducible bases for any concrete cases can be obtained trivially from those for the general case without any projection. All the irreducible bases for the group chains Oh&supuline;D4&supuline;C4 or Oh&supuline;D4&supuline;D2 are tabulated once and for all. As an application, the Hamiltonian in the algebraic model of Iachello and Oss for stretching vibrations of the molecule SF6 is diagonalized in the symmetry adapted bases. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 2472-2483 
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    Notes: The recipe of Weyl has been applied to two crystallographically distinct realizations of a regular orbit of the cyclic group of order N: the linear chain and the n-dimensional toroidal crystal, with n being the number of different prime integers dividing N, and Sylow factors of N being the Born–von Kármán periods. It follows that some fractallike symmetries of the linear chain are isomorphic images of multidimensional inversions, which are purely geometric operators. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 2510-2526 
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    Notes: In this article, it is shown how to obtain objects called Eichler integrals in the mathematical literature that can be used for calculating scattering amplitudes in string theory. These Eichler integrals are also new examples of Eichler integrals with poles. © 1996 American Institute of Physics.
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    Journal of Mathematical Physics 37 (1996), S. 2566-2566 
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    Journal of Mathematical Physics 37 (1996), S. 1602-1616 
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    Notes: The algebra of observables of SOq(3)-symmetric quantum mechanics is extended to include the inverse 1/R of the radial coordinate and used to obtain eigenvalues and eigenfunctions of a q-deformed Coulomb Hamiltonian. © 1996 American Institute of Physics.
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    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 37 (1996), S. 1642-1649 
    ISSN: 1089-7658
    Source: AIP Digital Archive
    Topics: Mathematics , Physics
    Notes: The discrete spectrum solutions corresponding to dually charged mesoatom on the space of constant negative curvature are obtained. The discrete spectrum of energies is finite and vanishes when the magnetic charge of the nucleus exceeds the critical value. © 1996 American Institute of Physics.
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  • 91
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    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 37 (1996), S. 1668-1712 
    ISSN: 1089-7658
    Source: AIP Digital Archive
    Topics: Mathematics , Physics
    Notes: We present an exactly solvable quantum field theory which allows rearrangement collisions. We solve the model in the relevant sectors and demonstrate the orthonormality and completeness of the solutions, and construct the S-matrix. In light of the exact solutions constructed, we discuss various issues and assumptions in quantum scattering theory, including the isometry of the Möller wave matrix, the normalization and completeness of asymptotic states, and the nonorthogonality of basis states. We show that these common assertions are not obtained in this model. We suggest a general formalism for scattering theory which overcomes these and other shortcomings and limitations of the existing formalisms in the literature. © 1996 American Institute of Physics.
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  • 92
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    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 37 (1996), S. 1772-1775 
    ISSN: 1089-7658
    Source: AIP Digital Archive
    Topics: Mathematics , Physics
    Notes: It is shown that the complete symmetry group for the Kepler problem, as introduced by Krause, can be derived by Lie group analysis. The same result is true for any autonomous system. © 1996 American Institute of Physics.
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  • 93
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    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 37 (1996), S. 1790-1811 
    ISSN: 1089-7658
    Source: AIP Digital Archive
    Topics: Mathematics , Physics
    Notes: We consider the quantum thermal statistics à la Gibbs–Shannon–Szilard–Jaynes based on q-entropies Sq[ρ]=(q−1)−1(1−tr(ρq)) (0〈q≠1) and the non-standard "internal energy'' functionals Uq[ρ]=tr(ρqH) proposed by C. Tsallis [J. Stat. Phys. 52, 479–487 (1988)]. © 1996 American Institute of Physics.
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  • 94
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    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 37 (1996), S. 1106-1114 
    ISSN: 1089-7658
    Source: AIP Digital Archive
    Topics: Mathematics , Physics
    Notes: It is shown that for the Calogero–Cohn-type upper bounds on the number of bound states of a negative spherically symmetric potential V(r), in each angular momentum state, that is, bounds containing only the integral ∫∞0||V(r)||1/2 dr, the condition V′(r)≥0 is not necessary, and can be replaced by the less stringent condition (d/dr)[r1−2p(−V)1−p]≤0, 1/2≤p〈1, which allows oscillations in the potential. The constants in the bounds are accordingly modified, depend on p and l, and tend to the standard value for p=1/2. © 1996 American Institute of Physics.
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  • 95
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    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 37 (1996), S. 1115-1127 
    ISSN: 1089-7658
    Source: AIP Digital Archive
    Topics: Mathematics , Physics
    Notes: Fractional supersymmetry denotes a generalization of supersymmetry which may be constructed using a single real generalized Grassmann variable, θ=θ¯,θn=0, for arbitrary integer n=2,3,.... An explicit formula is given in the case of general n for the transformations that leave the theory invariant, and it is shown that these transformations possess interesting group properties. It is shown also that the two generalized derivatives that enter the theory have a geometric interpretation as generators of left and right transformations of the fractional supersymmetry group. Careful attention is paid to some technically important issues, including differentiation, that arise as a result of the peculiar nature of quantities such as θ. © 1996 American Institute of Physics.
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  • 96
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    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 37 (1996), S. 1197-1203 
    ISSN: 1089-7658
    Source: AIP Digital Archive
    Topics: Mathematics , Physics
    Notes: The concept of geometric phase for a closed circuit in the ray space is applied to the manifold of generalized coherent states defined as the eigenstates of isotopic spin charges. The geometry of the state manifold is elucidated through a calculation of the Gaussian curvature. © 1996 American Institute of Physics.
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  • 97
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    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 37 (1996), S. 1171-1181 
    ISSN: 1089-7658
    Source: AIP Digital Archive
    Topics: Mathematics , Physics
    Notes: Nonstationary Schrödinger equation with a periodic finite band potential p(x) is considered. The Green's function G(x,x′,t) of this equation is investigated when t→∞. Asymptotics for G(x,x′,t) are specified. It is shown that for large "velocities'' v=(x−x′)/t the principal term in asymptotics of G(x,x′,t), t→∞ coincides with the Green's function for p=0. The principal term in the asymptotics of G(x,x′,t) in the case v→∞ is equal to a sum of Green's functions of unperturbed problems for particles whose masses are equal to effective masses of the Hill operator under investigation. © 1996 American Institute of Physics.
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  • 98
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    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 37 (1996), S. 1244-1252 
    ISSN: 1089-7658
    Source: AIP Digital Archive
    Topics: Mathematics , Physics
    Notes: Mechanics is developed over a differentiable manifold as space of possible positions. Time is considered to fill a one-dimensional Riemannian manifold, so having the metric as lapse. Then the system is quantized with covariant instead of partial derivatives in the Schrödinger operator. © 1996 American Institute of Physics.
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  • 99
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    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 37 (1996), S. 1234-1243 
    ISSN: 1089-7658
    Source: AIP Digital Archive
    Topics: Mathematics , Physics
    Notes: The both lower and upper estimates of the lower bound λ20 of the essential spectrum σess(H2) of the square of the Dirac Hamiltonian H for a spin 1/2 neutral particle with an anomalous magnetic moment in an asymptotically constant magnetic field are obtained. It is found that in a restricted case, λ20≤m2, where m is the mass of the particle. Moreover, it is proven that σess(H2)=[λ20,∞). In particular, in the case where the space dimension d is odd and d≥3, σess(H)=(−∞,−λ0]∪[λ0,∞). In the case where d=2 and 3, σess(H) is exactly identified. © 1996 American Institute of Physics.
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  • 100
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    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 37 (1996), S. 1268-1286 
    ISSN: 1089-7658
    Source: AIP Digital Archive
    Topics: Mathematics , Physics
    Notes: The modular structure of the free Bose gas in the critical regime of couplings is completely described by certain Gaussian Markovian (on a circle) nonergodic thermal process. Gentle perturbations of the arising Gaussian stochastic structure are controlled rigorously and the arising non-quasi-free W* KMS structure is shown to be nonergodic in certain range of couplings. The preserved nonergodicity seems to be connected to the presence of the Bose–Einstein condensate in the constructed models of interacting bosons. © 1996 American Institute of Physics.
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