(Phenomenology/Lattice-Compatible) SU(3) MχPT HD up to O $$ \mathcal{O} $$ (p4) and the O $$ \mathcal{O} $$ (R4)-Large-N Connection
Abstract Obtaining the values of the coupling constants of the low energy effective theory corresponding to QCD, compatible with experimental data, even in the (vector) mesonic sector from (the M $$ \mathcal{M} $$ -theory uplift of) a UV-complete string theory dual, has thus far been missing in the...
| Main Authors: | , , |
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| Format: | Article |
| Language: | English |
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SpringerOpen
2021-08-01
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| Series: | Journal of High Energy Physics |
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| Online Access: | https://doi.org/10.1007/JHEP08(2021)151 |
| _version_ | 1818449980860399616 |
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| author | Vikas Yadav Gopal Yadav Aalok Misra |
| author_facet | Vikas Yadav Gopal Yadav Aalok Misra |
| author_sort | Vikas Yadav |
| collection | DOAJ |
| description | Abstract Obtaining the values of the coupling constants of the low energy effective theory corresponding to QCD, compatible with experimental data, even in the (vector) mesonic sector from (the M $$ \mathcal{M} $$ -theory uplift of) a UV-complete string theory dual, has thus far been missing in the literature. We take the first step in this direction by obtaining the values of the coupling constants of the O $$ \mathcal{O} $$ (p 4) χPT Lagrangian in the chiral limit involving the NGBs and ρ meson (and its flavor partners) from the M $$ \mathcal{M} $$ -theory/type IIA dual of large-N thermal QCD, inclusive of the O $$ \mathcal{O} $$ (R 4) corrections. We observe that ensuring compatibility with phenomenological/lattice results (the values) as given in [1], requires a relationship relating the O $$ \mathcal{O} $$ (R 4) corrections and large-N suppression. In other words, QCD demands that the higher derivative corrections and the large-N suppressed corrections in its M/string theory dual, are related. As a bonus, we explicitly show that the O $$ \mathcal{O} $$ (R 4) corrections in the UV to the M $$ \mathcal{M} $$ -theory uplift of the type IIB dual of large-N thermal QCD at low temperatures, can be consistently set to be vanishingly small. |
| first_indexed | 2024-12-14T20:44:02Z |
| format | Article |
| id | doaj.art-0ae6c2eca92445829cf00951f04fa08c |
| institution | Directory Open Access Journal |
| issn | 1029-8479 |
| language | English |
| last_indexed | 2024-12-14T20:44:02Z |
| publishDate | 2021-08-01 |
| publisher | SpringerOpen |
| record_format | Article |
| series | Journal of High Energy Physics |
| spelling | doaj.art-0ae6c2eca92445829cf00951f04fa08c2022-12-21T22:48:09ZengSpringerOpenJournal of High Energy Physics1029-84792021-08-012021815010.1007/JHEP08(2021)151(Phenomenology/Lattice-Compatible) SU(3) MχPT HD up to O $$ \mathcal{O} $$ (p4) and the O $$ \mathcal{O} $$ (R4)-Large-N ConnectionVikas Yadav0Gopal Yadav1Aalok Misra2Department of Physics, Indian Institute of Technology RoorkeeDepartment of Physics, Indian Institute of Technology RoorkeeDepartment of Physics, Indian Institute of Technology RoorkeeAbstract Obtaining the values of the coupling constants of the low energy effective theory corresponding to QCD, compatible with experimental data, even in the (vector) mesonic sector from (the M $$ \mathcal{M} $$ -theory uplift of) a UV-complete string theory dual, has thus far been missing in the literature. We take the first step in this direction by obtaining the values of the coupling constants of the O $$ \mathcal{O} $$ (p 4) χPT Lagrangian in the chiral limit involving the NGBs and ρ meson (and its flavor partners) from the M $$ \mathcal{M} $$ -theory/type IIA dual of large-N thermal QCD, inclusive of the O $$ \mathcal{O} $$ (R 4) corrections. We observe that ensuring compatibility with phenomenological/lattice results (the values) as given in [1], requires a relationship relating the O $$ \mathcal{O} $$ (R 4) corrections and large-N suppression. In other words, QCD demands that the higher derivative corrections and the large-N suppressed corrections in its M/string theory dual, are related. As a bonus, we explicitly show that the O $$ \mathcal{O} $$ (R 4) corrections in the UV to the M $$ \mathcal{M} $$ -theory uplift of the type IIB dual of large-N thermal QCD at low temperatures, can be consistently set to be vanishingly small.https://doi.org/10.1007/JHEP08(2021)151Chiral LagrangiansGauge-gravity correspondenceM-Theory |
| spellingShingle | Vikas Yadav Gopal Yadav Aalok Misra (Phenomenology/Lattice-Compatible) SU(3) MχPT HD up to O $$ \mathcal{O} $$ (p4) and the O $$ \mathcal{O} $$ (R4)-Large-N Connection Journal of High Energy Physics Chiral Lagrangians Gauge-gravity correspondence M-Theory |
| title | (Phenomenology/Lattice-Compatible) SU(3) MχPT HD up to O $$ \mathcal{O} $$ (p4) and the O $$ \mathcal{O} $$ (R4)-Large-N Connection |
| title_full | (Phenomenology/Lattice-Compatible) SU(3) MχPT HD up to O $$ \mathcal{O} $$ (p4) and the O $$ \mathcal{O} $$ (R4)-Large-N Connection |
| title_fullStr | (Phenomenology/Lattice-Compatible) SU(3) MχPT HD up to O $$ \mathcal{O} $$ (p4) and the O $$ \mathcal{O} $$ (R4)-Large-N Connection |
| title_full_unstemmed | (Phenomenology/Lattice-Compatible) SU(3) MχPT HD up to O $$ \mathcal{O} $$ (p4) and the O $$ \mathcal{O} $$ (R4)-Large-N Connection |
| title_short | (Phenomenology/Lattice-Compatible) SU(3) MχPT HD up to O $$ \mathcal{O} $$ (p4) and the O $$ \mathcal{O} $$ (R4)-Large-N Connection |
| title_sort | phenomenology lattice compatible su 3 mχpt hd up to o mathcal o p4 and the o mathcal o r4 large n connection |
| topic | Chiral Lagrangians Gauge-gravity correspondence M-Theory |
| url | https://doi.org/10.1007/JHEP08(2021)151 |
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