Cargando…
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...
Autores principales: | , , |
---|---|
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 |
_version_ | 1780884946927222784 |
---|---|
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. |
id | cern-240712 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1992 |
record_format | invenio |
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 |
work_keys_str_mv | AT ellisjohnr thestringuniversehightcsuperconductororquantumhallconductor AT mavromatosne thestringuniversehightcsuperconductororquantumhallconductor AT nanopoulosdimitriv thestringuniversehightcsuperconductororquantumhallconductor AT ellisjohnr stringuniversehightcsuperconductororquantumhallconductor AT mavromatosne stringuniversehightcsuperconductororquantumhallconductor AT nanopoulosdimitriv stringuniversehightcsuperconductororquantumhallconductor |