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Infinitely many inequivalent field theories from one Lagrangian
Logarithmic time-like Liouville quantum field theory has a generalized PT invariance, where T is the time-reversal operator and P stands for an S-duality reflection of the Liouville field $\phi$. In Euclidean space the Lagrangian of such a theory, $L=\frac{1}{2}(\nabla\phi)^2-ig\phi\exp(ia\phi)$, is...
Autores principales: | , , , |
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Lenguaje: | eng |
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2014
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Acceso en línea: | https://dx.doi.org/10.1103/PhysRevLett.113.231605 http://cds.cern.ch/record/1748955 |
_version_ | 1780943016834367488 |
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author | Bender, Carl M. Hook, Daniel W. Mavromatos, Nick E. Sarkar, Sarben |
author_facet | Bender, Carl M. Hook, Daniel W. Mavromatos, Nick E. Sarkar, Sarben |
author_sort | Bender, Carl M. |
collection | CERN |
description | Logarithmic time-like Liouville quantum field theory has a generalized PT invariance, where T is the time-reversal operator and P stands for an S-duality reflection of the Liouville field $\phi$. In Euclidean space the Lagrangian of such a theory, $L=\frac{1}{2}(\nabla\phi)^2-ig\phi\exp(ia\phi)$, is analyzed using the techniques of PT-symmetric quantum theory. It is shown that L defines an infinite number of unitarily inequivalent sectors of the theory labeled by the integer n. In one-dimensional space (quantum mechanics) the energy spectrum is calculated in the semiclassical limit and the mth energy level in the nth sector is given by $E_{m,n}\sim(m+1/2)^2a^2/(16n^2)$. |
id | cern-1748955 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2014 |
record_format | invenio |
spelling | cern-17489552023-03-14T17:49:09Zdoi:10.1103/PhysRevLett.113.231605http://cds.cern.ch/record/1748955engBender, Carl M.Hook, Daniel W.Mavromatos, Nick E.Sarkar, SarbenInfinitely many inequivalent field theories from one LagrangianParticle Physics - TheoryLogarithmic time-like Liouville quantum field theory has a generalized PT invariance, where T is the time-reversal operator and P stands for an S-duality reflection of the Liouville field $\phi$. In Euclidean space the Lagrangian of such a theory, $L=\frac{1}{2}(\nabla\phi)^2-ig\phi\exp(ia\phi)$, is analyzed using the techniques of PT-symmetric quantum theory. It is shown that L defines an infinite number of unitarily inequivalent sectors of the theory labeled by the integer n. In one-dimensional space (quantum mechanics) the energy spectrum is calculated in the semiclassical limit and the mth energy level in the nth sector is given by $E_{m,n}\sim(m+1/2)^2a^2/(16n^2)$.<p>Logarithmic timelike Liouville quantum field theory has a generalized <inline-formula><mml:math display="inline"><mml:mi mathvariant="script">PT</mml:mi></mml:math></inline-formula> invariance, where <inline-formula><mml:math display="inline"><mml:mi mathvariant="script">T</mml:mi></mml:math></inline-formula> is the time-reversal operator and <inline-formula><mml:math display="inline"><mml:mi mathvariant="script">P</mml:mi></mml:math></inline-formula> stands for an <inline-formula><mml:math display="inline"><mml:mi>S</mml:mi></mml:math></inline-formula>-duality reflection of the Liouville field <inline-formula><mml:math display="inline"><mml:mi>ϕ</mml:mi></mml:math></inline-formula>. In Euclidean space, the Lagrangian of such a theory <inline-formula><mml:math display="inline"><mml:mi>L</mml:mi><mml:mo>=</mml:mo><mml:mfrac><mml:mn>1</mml:mn><mml:mn>2</mml:mn></mml:mfrac><mml:mo stretchy="false">(</mml:mo><mml:mo>∇</mml:mo><mml:mi>ϕ</mml:mi><mml:msup><mml:mo stretchy="false">)</mml:mo><mml:mn>2</mml:mn></mml:msup><mml:mo>-</mml:mo><mml:mi>i</mml:mi><mml:mi>g</mml:mi><mml:mi>ϕ</mml:mi><mml:mi>exp</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>i</mml:mi><mml:mi>a</mml:mi><mml:mi>ϕ</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:math></inline-formula> is analyzed using the techniques of <inline-formula><mml:math display="inline"><mml:mi mathvariant="script">PT</mml:mi></mml:math></inline-formula>-symmetric quantum theory. It is shown that <inline-formula><mml:math display="inline"><mml:mi>L</mml:mi></mml:math></inline-formula> defines an infinite number of unitarily inequivalent sectors of the theory labeled by the integer <inline-formula><mml:math display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula>. In one-dimensional space (quantum mechanics), the energy spectrum is calculated in the semiclassical limit and the <inline-formula><mml:math display="inline"><mml:mi>m</mml:mi></mml:math></inline-formula>th energy level in the <inline-formula><mml:math display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula>th sector is given by <inline-formula><mml:math display="inline"><mml:msub><mml:mi>E</mml:mi><mml:mrow><mml:mi>m</mml:mi><mml:mo>,</mml:mo><mml:mi>n</mml:mi></mml:mrow></mml:msub><mml:mo>∼</mml:mo><mml:mo stretchy="false">(</mml:mo><mml:mi>m</mml:mi><mml:mo>+</mml:mo><mml:mn>1</mml:mn><mml:mo stretchy="false">/</mml:mo><mml:mn>2</mml:mn><mml:msup><mml:mo stretchy="false">)</mml:mo><mml:mn>2</mml:mn></mml:msup><mml:msup><mml:mi>a</mml:mi><mml:mn>2</mml:mn></mml:msup><mml:mo stretchy="false">/</mml:mo><mml:mo stretchy="false">(</mml:mo><mml:mn>16</mml:mn><mml:msup><mml:mi>n</mml:mi><mml:mn>2</mml:mn></mml:msup><mml:mo stretchy="false">)</mml:mo></mml:math></inline-formula>.</p>Logarithmic time-like Liouville quantum field theory has a generalized PT invariance, where T is the time-reversal operator and P stands for an S-duality reflection of the Liouville field $\phi$. In Euclidean space the Lagrangian of such a theory, $L=\frac{1}{2}(\nabla\phi)^2-ig\phi\exp(ia\phi)$, is analyzed using the techniques of PT-symmetric quantum theory. It is shown that L defines an infinite number of unitarily inequivalent sectors of the theory labeled by the integer n. In one-dimensional space (quantum mechanics) the energy spectrum is calculated in the semiclassical limit and the mth energy level in the nth sector is given by $E_{m,n}\sim(m+1/2)^2a^2/(16n^2)$.arXiv:1408.2432PREPRINT-KCL-PH-TH-2014-27LCTS-2014-26PREPRINT KCL-PH-TH-2014-27oai:cds.cern.ch:17489552014-08-11 |
spellingShingle | Particle Physics - Theory Bender, Carl M. Hook, Daniel W. Mavromatos, Nick E. Sarkar, Sarben Infinitely many inequivalent field theories from one Lagrangian |
title | Infinitely many inequivalent field theories from one Lagrangian |
title_full | Infinitely many inequivalent field theories from one Lagrangian |
title_fullStr | Infinitely many inequivalent field theories from one Lagrangian |
title_full_unstemmed | Infinitely many inequivalent field theories from one Lagrangian |
title_short | Infinitely many inequivalent field theories from one Lagrangian |
title_sort | infinitely many inequivalent field theories from one lagrangian |
topic | Particle Physics - Theory |
url | https://dx.doi.org/10.1103/PhysRevLett.113.231605 http://cds.cern.ch/record/1748955 |
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