Cubic action in double field theory

We study target space theory on a torus for the states with NL+NR=2 through Double Field Theory. The spin-two Fierz-Pauli fields are not allowed when all spatial dimensions are non-compact. The massive states provide both non-vanishing momentum and winding numbers in the target space theory. To deri...

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Main Author: Chen-Te Ma
Format: Article
Language:English
Published: Elsevier 2021-10-01
Series:Nuclear Physics B
Online Access:http://www.sciencedirect.com/science/article/pii/S055032132100225X
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spelling doaj-1cbaec77883e4d46a8e870147a157fc52021-10-01T04:50:55ZengElsevierNuclear Physics B0550-32132021-10-01971115528Cubic action in double field theoryChen-Te Ma0Guangdong Provincial Key Laboratory of Nuclear Science, Institute of Quantum Matter, South China Normal University, Guangzhou 510006, Guangdong, China; School of Physics and Telecommunication Engineering, South China Normal University, Guangzhou 510006, Guangdong, China; Guangdong-Hong Kong Joint Laboratory of Quantum Matter, Southern Nuclear Science Computing Center, South China Normal University, Guangzhou 510006, Guangdong, China; The Laboratory for Quantum Gravity and Strings, Department of Mathematics and Applied Mathematics, University of Cape Town, Private Bag, Rondebosch 7700, South Africa; Department of Physics and Center for Theoretical Sciences, National Taiwan University, Taipei 10617, Taiwan, ROC; Correspondence to: Guangdong Provincial Key Laboratory of Nuclear Science, Institute of Quantum Matter, South China Normal University, Guangzhou 510006, Guangdong, China.We study target space theory on a torus for the states with NL+NR=2 through Double Field Theory. The spin-two Fierz-Pauli fields are not allowed when all spatial dimensions are non-compact. The massive states provide both non-vanishing momentum and winding numbers in the target space theory. To derive the cubic action, we provide the unique constraint for NL≠NR compatible with the integration by part. We first make a correspondence of massive and massless fields. The quadratic action is gauge invariant by introducing the mass term. We then proceed to the cubic order. The cubic action is also gauge invariant by introducing the coupling between the one-form field and other fields. The massive states do not follow the consistent truncation. One should expect the self-consistent theory by summing over infinite modes. Hence the naive expectation is wrong up to the cubic order. In the end, we show that the momentum and winding modes cannot both appear for only one compact doubled space.http://www.sciencedirect.com/science/article/pii/S055032132100225X
collection DOAJ
language English
format Article
sources DOAJ
author Chen-Te Ma
spellingShingle Chen-Te Ma
Cubic action in double field theory
Nuclear Physics B
author_facet Chen-Te Ma
author_sort Chen-Te Ma
title Cubic action in double field theory
title_short Cubic action in double field theory
title_full Cubic action in double field theory
title_fullStr Cubic action in double field theory
title_full_unstemmed Cubic action in double field theory
title_sort cubic action in double field theory
publisher Elsevier
series Nuclear Physics B
issn 0550-3213
publishDate 2021-10-01
description We study target space theory on a torus for the states with NL+NR=2 through Double Field Theory. The spin-two Fierz-Pauli fields are not allowed when all spatial dimensions are non-compact. The massive states provide both non-vanishing momentum and winding numbers in the target space theory. To derive the cubic action, we provide the unique constraint for NL≠NR compatible with the integration by part. We first make a correspondence of massive and massless fields. The quadratic action is gauge invariant by introducing the mass term. We then proceed to the cubic order. The cubic action is also gauge invariant by introducing the coupling between the one-form field and other fields. The massive states do not follow the consistent truncation. One should expect the self-consistent theory by summing over infinite modes. Hence the naive expectation is wrong up to the cubic order. In the end, we show that the momentum and winding modes cannot both appear for only one compact doubled space.
url http://www.sciencedirect.com/science/article/pii/S055032132100225X
work_keys_str_mv AT chentema cubicactionindoublefieldtheory
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