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  • 1
    Digitale Medien
    Digitale Medien
    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 32 (1991), S. 1788-1795 
    ISSN: 1089-7658
    Quelle: AIP Digital Archive
    Thema: Mathematik , Physik
    Notizen: It is shown that the two-body problem with action-at-a-distance interaction potential in the framework of a canonical manifestly covariant mechanics, for which there exists a consistent and well-developed quantum version, can be embedded in a Riemannian manifold (with conformal metric) where the curvature replaces the explicit appearance of the potential. The geodesic motion in the conformal space coincides with the solutions of the Hamilton equations of motion in the corresponding flat space problem. The reparametrization invariant form of the action principle which leads to the geodesic equation is shown to be equivalent to the underlying canonical mechanics with a particular choice of parameter. This program realizes the possibility of describing a class of nongravitational interactions in space-time by essentially geometrical means. A relation is proposed between the Einstein tensor in the conformal space and the (nonconserved) energy momentum tensor associated with relative motion, with the help of a Brans–Dicke type field. The structure of the result suggests a generalization of the principle of equivalence, for dealing, at least, with the two-body problem, which treats a manifold of relative space-time as the globally defined coordinates for which there exists, at every point, a local frame in which the metric is conformal (in the absence of nongravitational forces, this procedure reduces to the usual one). In this way, one can treat gravitational and a certain class of nongravitational forces in a unified way.
    Materialart: Digitale Medien
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  • 2
    Digitale Medien
    Digitale Medien
    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 30 (1989), S. 213-218 
    ISSN: 1089-7658
    Quelle: AIP Digital Archive
    Thema: Mathematik , Physik
    Notizen: It is shown that two-body relativistic scattering cross sections can be represented in terms of phase shift analysis in essentially the same form as that of nonrelativistic scattering theory. The representation is covariant; the variable that corresponds to the orbital quantum number (and approaches it in the nonrelativistic limit) is relativistically invariant. The Levinson theorem is valid, and provides a link between the bound states, which have support in an O(2,1) invariant subspace of the full spacelike region of relative coordinates, and the scattering states that contain resonant behavior. These scattering states consequently have support in the same restricted subspace, and the same procedure may be used for the separation of variables. As an example, the resonances of an O(3,1) invariant "square well'' are discussed.
    Materialart: Digitale Medien
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  • 3
    Digitale Medien
    Digitale Medien
    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 30 (1989), S. 59-59 
    ISSN: 1089-7658
    Quelle: AIP Digital Archive
    Thema: Mathematik , Physik
    Notizen: A complete proof of the equivalence of the star operation in the operator algebra isomorphic to quaternions and the adjoint operation in a quaternion Hilbert module is given.
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  • 4
    Digitale Medien
    Digitale Medien
    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 30 (1989), S. 66-80 
    ISSN: 1089-7658
    Quelle: AIP Digital Archive
    Thema: Mathematik , Physik
    Notizen: In the framework of a manifestly covariant quantum theory on space-time, it is shown that the ground state mass of a relativistic two-body system with O(3,1) symmetric potential is lower when represented by a wave function with support in an O(2,1) invariant subspace of the spacelike region. The wave functions for the relativistic bound states are obtained explicitly. Coulomb type binding, the harmonic oscillator, and the relativistic square well are treated as examples. The mass spectrum is determined by a differential equation in the invariant spacelike interval ρ, which can be put into correspondence with the radial part of a nonrelativistic Schrödinger equation with potential of the same form, where r is replaced by ρ. In the case that the binding is small compared to the particle masses, the mass spectrum (bounded below) is well-approximated by the results of the nonrelativistic theory. The eigenfunctions transform under the full Lorentz group as elements of an induced representation with O(2,1) little group. This representation is studied in a succeeding paper.
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  • 5
    Digitale Medien
    Digitale Medien
    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 37 (1996), S. 5429-5443 
    ISSN: 1089-7658
    Quelle: AIP Digital Archive
    Thema: Mathematik , Physik
    Notizen: It has recently been shown, by application of statistical mechanical methods to determine the canonical ensemble governing the equilibrium distribution of operator initial values, that complex quantum field theory can emerge as a statistical approximation to an underlying generalized quantum dynamics. This result was obtained by an argument based on a Ward identity analogous to the equipartition theorem of classical statistical mechanics. We construct here a microcanonical ensemble which forms the basis of this canonical ensemble. This construction enables us to define the microcanonical entropy and free energy of the field configuration of the equilibrium distribution and to study the stability of the canonical ensemble. We also study the algebraic structure of the conserved generators from which the microcanonical and canonical ensembles are constructed, and the flows they induce on the phase space. © 1996 American Institute of Physics.
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  • 6
    Digitale Medien
    Digitale Medien
    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 33 (1992), S. 3098-3104 
    ISSN: 1089-7658
    Quelle: AIP Digital Archive
    Thema: Mathematik , Physik
    Notizen: In the construction of a tensor product of quaternion Hilbert modules, given in a previous work (real, complex, and quaternionic), inner products were defined in the vector spaces formed from the tensor product of quaternion algebras H modulo an appropriate left ideal in each case. Under conditions that are necessary for the definition of a scalar product in the quaternionic Hilbert modules and a natural condition on the algebraic structure, it is proven that the scalar products which are defined are unique.
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  • 7
    Digitale Medien
    Digitale Medien
    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 30 (1989), S. 380-392 
    ISSN: 1089-7658
    Quelle: AIP Digital Archive
    Thema: Mathematik , Physik
    Notizen: It was shown in I [J. Math. Phys. 30, 66 (1989)] that the eigenfunctions for the reduced motion of the quantum relativistic bound state with O(3,1) symmetric potential have support in an O(2,1) invariant subregion of the full spacelike region. They form irreducible representations of SU(1,1) [in the double covering of O(2,1)] parametrized by the unit spacelike vector nμ, taken in I as the direction of the z axis (the spectrum is independent of this choice), for which this O(2,1) is the stabilizer. Lorentz transformations move these representations on an orbit whose range is the single-sheeted hyperboloid covered by this spacelike vector, providing a set of induced representations of SL(2,C). From linear combinations of functions from the irreducible representations of SU(1,1), the representations of the SU(2) subgroup of SL(2,C) on the orbit are extracted and the differential equations that are the eigenvalue equations for the Casimir operators of SL(2,C) are solved. It is found that these SU(2) representations form a basis for the principal series in the canonical representations of Gel'fand. There is a natural scalar product, obtained from group integration on SL(2,C), for which the canonical basis forms an orthogonal set, and the representation is unitary. Since the scalar product [over the O(2,1) invariant measure space] of SU(1,1) irreducible representations is invariant under the action of the little group, the remaining group measure [on the coset space SL(2,C)/SU(1,1)] is the volume on the hyperboloidal spacelike hypersurface dμn=d4n δ(n2−1). The family of Hilbert spaces (Hn) that carries the representations of O(3,1) is therefore embedded in a larger Hilbert space H with measure d4y dμn, where the { y} are the space-time coordinates of the restricted region associated with nμ. The representations with nonrelativistic limit coinciding with the known Schrödinger solutions for corresponding spherically symmetric potential problems are in the double covering (half-integer values for the lowest L level) of O(3,1).
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  • 8
    Digitale Medien
    Digitale Medien
    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 35 (1994), S. 2743-2760 
    ISSN: 1089-7658
    Quelle: AIP Digital Archive
    Thema: Mathematik , Physik
    Notizen: The Lee–Friedrichs model has been very useful in the study of decay-scattering systems in the framework of complex quantum mechanics. Since it is exactly soluble, the analytic structure of the amplitudes can be explicitly studied. It is shown in this article that a similar model, which is also exactly soluble, can be constructed in quaternionic quantum mechanics. The problem of the decay of an unstable system is treated here. The use of the Laplace transform, involving quaternion-valued analytic functions of a variable with values in a complex subalgebra of the quaternion algebra, makes the analytic properties of the solution apparent; some analysis is given of the dominating structure in the analytic continuation to the lower half plane. A study of the corresponding scattering system will be given in a succeeding article.
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  • 9
    Digitale Medien
    Digitale Medien
    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 34 (1993), S. 3405-3419 
    ISSN: 1089-7658
    Quelle: AIP Digital Archive
    Thema: Mathematik , Physik
    Notizen: Following the spectral methods established by Adler in his treatment of scattering and decay in the quaternionic quantum theory, it is shown that an anti-self-adjoint operator with quaternion defined spectrum in [0,∞) has a symmetrical effective spectrum, from the point of view of functional analysis, under quite general conditions. In the case of an operator with absolutely continuous spectrum in [0,∞), the effective spectrum is absolutely continuous in (−∞,∞), and a canonically conjugate operator exists. If the anti-self-adjoint operator is the generator of motion in time (Hamiltonian), the conjugate operator is a "time operator.'' Moreover, according to a theorem of Misra, Prigogine, and Courbage, such a system may admit a Lyapunov operator, and therefore describe irreversible behavior. It is shown directly that no evident contradiction (as is found in the semibounded case in complex quantum mechanics) arises from the definition of a Lyapunov operator in quaternionic quantum mechanics.
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  • 10
    Digitale Medien
    Digitale Medien
    College Park, Md. : American Institute of Physics (AIP)
    Journal of Mathematical Physics 35 (1994), S. 2761-2771 
    ISSN: 1089-7658
    Quelle: AIP Digital Archive
    Thema: Mathematik , Physik
    Notizen: In a previous article, it was shown that a soluble model can be constructed for the the description of a decaying system in analogy to the Lee–Friedrichs model of complex quantum theory. It is shown here that this model also provides a soluble scattering theory, and therefore constitutes a model for a decay-scattering system. Generalized second resolvent equations are obtained for quaternionic scattering theory. It is shown explicitly for this model, in accordance with a general theorem of Adler, that the scattering matrix is complex subalgebra valued. It is also shown that the method of Adler, using an effective optical potential in the complex sector to describe the effect of the quaternionic interactions, is equivalent to the general method of Green's functions described here.
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