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The string universe: high T$_{c}$ superconductor or quantum Hall conductor?

Our answer is the latter. Space-time singularities, including the initial one, are described by world-sheet topological Abelian gauge theories with a Chern-Simons term. Their effective $N=2$ supersymmetry provides an initial fixed point where the Bogomolny bound is saturated on the world-sheet, corr...

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Detalles Bibliográficos
Autores principales: Ellis, John R., Mavromatos, N.E., Nanopoulos, Dimitri V.
Lenguaje:eng
Publicado: 1992
Materias:
Acceso en línea:https://dx.doi.org/10.1016/0370-2693(92)90801-A
http://cds.cern.ch/record/240712
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author Ellis, John R.
Mavromatos, N.E.
Nanopoulos, Dimitri V.
author_facet Ellis, John R.
Mavromatos, N.E.
Nanopoulos, Dimitri V.
author_sort Ellis, John R.
collection CERN
description Our answer is the latter. Space-time singularities, including the initial one, are described by world-sheet topological Abelian gauge theories with a Chern-Simons term. Their effective $N=2$ supersymmetry provides an initial fixed point where the Bogomolny bound is saturated on the world-sheet, corresponding to an extreme Reissner-Nordstrom solution in space-time. Away from the singularity the gauge theory has world-sheet matter fields, bosons and fermions, associated with the generation of target space-time. Because the fermions are complex (cf the Quantum Hall Effect) rather than real (cf high-$T_c$ superconductors) the energetically-preferred vacuum is not parity or time-reversal invariant, and the associated renormalization group flow explains the cosmological arrow of time, as well as the decay of real or virtual black holes, with a monotonic increase in entropy.
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institution Organización Europea para la Investigación Nuclear
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publishDate 1992
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spelling cern-2407122020-07-23T02:45:42Zdoi:10.1016/0370-2693(92)90801-Ahttp://cds.cern.ch/record/240712engEllis, John R.Mavromatos, N.E.Nanopoulos, Dimitri V.The string universe: high T$_{c}$ superconductor or quantum Hall conductor?General Theoretical PhysicsOur answer is the latter. Space-time singularities, including the initial one, are described by world-sheet topological Abelian gauge theories with a Chern-Simons term. Their effective $N=2$ supersymmetry provides an initial fixed point where the Bogomolny bound is saturated on the world-sheet, corresponding to an extreme Reissner-Nordstrom solution in space-time. Away from the singularity the gauge theory has world-sheet matter fields, bosons and fermions, associated with the generation of target space-time. Because the fermions are complex (cf the Quantum Hall Effect) rather than real (cf high-$T_c$ superconductors) the energetically-preferred vacuum is not parity or time-reversal invariant, and the associated renormalization group flow explains the cosmological arrow of time, as well as the decay of real or virtual black holes, with a monotonic increase in entropy.Our answer is the latter. Space-time singularities, including the initial one, are described by world-sheet topological Abelian gauge theories with a Chern-Simons term. Their effective $N=2$ supersymmetry provides an initial fixed point where the Bogomolny bound is saturated on the world-sheet, corresponding to an extreme Reissner-Nordstrom solution in space-time. Away from the singularity the gauge theory has world-sheet matter fields, bosons and fermions, associated with the generation of target space-time. Because the fermions are complex (cf the Quantum Hall Effect) rather than real (cf high-$T_c$ superconductors) the energetically-preferred vacuum is not parity or time-reversal invariant, and the associated renormalization group flow explains the cosmological arrow of time, as well as the decay of real or virtual black holes, with a monotonic increase in entropy.Our answer is the latter. Space-time singularities, including the initial one, are described by world-sheet topological abelian gauge theories with a Chern-Simons term. Their effective N = 2 supersymmetry provides an initial fixed point where the Bogomolny bound is saturated on the world-sheet, corresponding to an extreme Reissner-Nordstrom solution in space-time. Away from the singularity the gauge theory has world-sheet matter fields, bosons and fermions, associated with the generation of target space-time. Because the fermions are complex (cf. the quantum Hall effect) rather than real (cf. high- T c superconductors) the energetically-preferred vacuum is not parity or time-reversal invariant, and the associated renormalization group flow explains the cosmological arrow of time, as well as the decay of real or virtual black holes, with a monotonic increase in entropy.CERN-TH-6536-92ACT-13-92CTP-TAMU-48-92hep-th/9209013CERN-TH.6536-92ACT-1992-13CERN-TH-6536-92CTP-TAMU-92-48oai:cds.cern.ch:2407121992
spellingShingle General Theoretical Physics
Ellis, John R.
Mavromatos, N.E.
Nanopoulos, Dimitri V.
The string universe: high T$_{c}$ superconductor or quantum Hall conductor?
title The string universe: high T$_{c}$ superconductor or quantum Hall conductor?
title_full The string universe: high T$_{c}$ superconductor or quantum Hall conductor?
title_fullStr The string universe: high T$_{c}$ superconductor or quantum Hall conductor?
title_full_unstemmed The string universe: high T$_{c}$ superconductor or quantum Hall conductor?
title_short The string universe: high T$_{c}$ superconductor or quantum Hall conductor?
title_sort string universe: high t$_{c}$ superconductor or quantum hall conductor?
topic General Theoretical Physics
url https://dx.doi.org/10.1016/0370-2693(92)90801-A
http://cds.cern.ch/record/240712
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AT ellisjohnr stringuniversehightcsuperconductororquantumhallconductor
AT mavromatosne stringuniversehightcsuperconductororquantumhallconductor
AT nanopoulosdimitriv stringuniversehightcsuperconductororquantumhallconductor