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Peter K. F. Kuhfittig - One of the best experts on this subject based on the ideXlab platform.

  • Stable wormholes on a noncommutative-geometry background admitting a one-Parameter Group of conformal motions
    Indian Journal of Physics, 2015
    Co-Authors: Peter K. F. Kuhfittig
    Abstract:

    When Morris and Thorne first proposed the possible existence of traversable wormholes, they adopted the following strategy: maintain complete control over the geometry, thereby leaving open the determination of the stress–energy tensor. In this paper we determine this tensor by starting with a noncommutative-geometry background and assuming that the static and spherically symmetric spacetime admits conformal motions. We have shown that the wormhole obtained can be made stable to linearized radial perturbations.

  • wormholes with a barotropic equation of state admitting a one Parameter Group of conformal motions
    Annals of Physics, 2015
    Co-Authors: Peter K. F. Kuhfittig
    Abstract:

    The theoretical construction of a traversable wormhole proposed by Morris and Thorne maintains complete control over the geometry by assigning both the shape and redshift functions, thereby leaving open the determination of the stress–energy tensor. This paper examines the effect of introducing the linear barotropic equation of state pr=ωρ on the theoretical construction. If either the energy density or the closely related shape function is known, then the Einstein field equations do not ordinarily yield a finite redshift function. If, however, the wormhole admits a one-Parameter Group of conformal motions, then both the redshift and shape functions exist provided that −3<ω<−1. In a cosmological setting, the equation of state p=ωρ, ω<−1, is associated with phantom dark energy, which is known to support traversable wormholes. The restriction −3<ω<−1 that arises in the present wormhole setting can be attributed to the assumption of conformal symmetry.

  • wormholes with a barotropic equation of state admitting a one Parameter Group of conformal motions
    arXiv: General Relativity and Quantum Cosmology, 2015
    Co-Authors: Peter K. F. Kuhfittig
    Abstract:

    The theoretical construction of a traversable wormhole proposed by Morris and Thorne maintains complete control over the geometry by assigning both the shape and redshift functions, thereby leaving open the determination of the stress-energy tensor. This paper examines the effect of introducing the linear barotropic equation of state $p_r=\omega\rho$ on the theoretical construction. If either the energy density or the closely related shape function is known, then the Einstein field equations do not ordinarily yield a finite redshift function. If, however, the wormhole admits a one-Parameter Group of conformal motions, then both the redshift and shape functions exist provided that $\omega <-1$. In a cosmological setting, the equation of state $p=\omega\rho$, $\omega <-1$, is associated with phantom dark energy, which is known to support traversable wormholes.

  • Wormholes with a barotropic equation of state admitting a one-Parameter Group of conformal motions
    Annals of Physics, 2015
    Co-Authors: Peter K. F. Kuhfittig
    Abstract:

    The theoretical construction of a traversable wormhole proposed by Morris and Thorne maintains complete control over the geometry by assigning both the shape and redshift functions, thereby leaving open the determination of the stress–energy tensor. This paper examines the effect of introducing the linear barotropic equation of state pr=ωρ on the theoretical construction. If either the energy density or the closely related shape function is known, then the Einstein field equations do not ordinarily yield a finite redshift function. If, however, the wormhole admits a one-Parameter Group of conformal motions, then both the redshift and shape functions exist provided that −3

Eva A. Gallardo-gutiérrez - One of the best experts on this subject based on the ideXlab platform.

  • Unitary equivalence of one-Parameter Groups of Toeplitz and composition operators
    Journal of Functional Analysis, 2011
    Co-Authors: Carl C. Cowen, Eva A. Gallardo-gutiérrez
    Abstract:

    Abstract The composition operators on H 2 whose symbols are hyperbolic automorphisms of the unit disk fixing ±1 comprise a one-Parameter Group and the analytic Toeplitz operators coming from covering maps of annuli centered at the origin whose radii are reciprocals also form a one-Parameter Group. Using the eigenvectors of the composition operators and of the adjoints of the Toeplitz operators, a direct unitary equivalence is found between the restrictions to z H 2 of the Group of Toeplitz operators and the Group of adjoints of these composition operators. On the other hand, it is shown that there is not a unitary equivalence of the Groups of Toeplitz operators and the adjoints of the composition operators on the whole of H 2 , but there is a similarity between them.

Joachim Toft - One of the best experts on this subject based on the ideXlab platform.

Saroj Kumbhare - One of the best experts on this subject based on the ideXlab platform.

Carl C. Cowen - One of the best experts on this subject based on the ideXlab platform.

  • Unitary equivalence of one-Parameter Groups of Toeplitz and composition operators
    Journal of Functional Analysis, 2011
    Co-Authors: Carl C. Cowen, Eva A. Gallardo-gutiérrez
    Abstract:

    Abstract The composition operators on H 2 whose symbols are hyperbolic automorphisms of the unit disk fixing ±1 comprise a one-Parameter Group and the analytic Toeplitz operators coming from covering maps of annuli centered at the origin whose radii are reciprocals also form a one-Parameter Group. Using the eigenvectors of the composition operators and of the adjoints of the Toeplitz operators, a direct unitary equivalence is found between the restrictions to z H 2 of the Group of Toeplitz operators and the Group of adjoints of these composition operators. On the other hand, it is shown that there is not a unitary equivalence of the Groups of Toeplitz operators and the adjoints of the composition operators on the whole of H 2 , but there is a similarity between them.