Journal article 1011 views
Mesons in large-N QCD
Gunnar Bali,
Francis Bursa,
Luca Castagnini,
Sara Collins,
Luigi Debbio,
Biagio Lucini ,
Marco Panero
Journal of High Energy Physics, Volume: 2013, Issue: 6
Swansea University Author: Biagio Lucini
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DOI (Published version): 10.1007/JHEP06(2013)071
Abstract
We present the results of a systematic, first-principles study of the spectrum and decay constants of mesons for different numbers of color charges N, via lattice computations. We restrict our attention to states in the non-zero isospin sector, evaluating the masses associated with the ground-state...
Published in: | Journal of High Energy Physics |
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ISSN: | 1029-8479 |
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2013
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URI: | https://cronfa.swan.ac.uk/Record/cronfa15285 |
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2013-11-01T14:10:35.1792140 v2 15285 2013-07-29 Mesons in large-N QCD 7e6fcfe060e07a351090e2a8aba363cf 0000-0001-8974-8266 Biagio Lucini Biagio Lucini true false 2013-07-29 SMA We present the results of a systematic, first-principles study of the spectrum and decay constants of mesons for different numbers of color charges N, via lattice computations. We restrict our attention to states in the non-zero isospin sector, evaluating the masses associated with the ground-state and first excitation in the pseudoscalar, vector, scalar, and axial vector channels. Our results are based on a new set of simulations of four dimensional SU(N) Yang-Mills theories with the number of colors ranging from N = 2 to N =17;the spectra and the decay constants are computed in the quenched approximation (which becomes exact in the ’t Hooft limit) using Wilson fermions. After discussing the extrapolations to the chiral and large-N limits, we present a comparison of our results to some of the numerical computations and analytical predictions available in the literature — including, in particular, those from holographic computations. Journal Article Journal of High Energy Physics 2013 6 1029-8479 Lattice QCD, AdS-CFT Correspondence, 1/N Expansion 31 12 2013 2013-12-31 10.1007/JHEP06(2013)071 COLLEGE NANME Mathematics COLLEGE CODE SMA Swansea University 2013-11-01T14:10:35.1792140 2013-07-29T10:34:05.2544519 Faculty of Science and Engineering School of Biosciences, Geography and Physics - Physics Gunnar Bali 1 Francis Bursa 2 Luca Castagnini 3 Sara Collins 4 Luigi Debbio 5 Biagio Lucini 0000-0001-8974-8266 6 Marco Panero 7 |
title |
Mesons in large-N QCD |
spellingShingle |
Mesons in large-N QCD Biagio Lucini |
title_short |
Mesons in large-N QCD |
title_full |
Mesons in large-N QCD |
title_fullStr |
Mesons in large-N QCD |
title_full_unstemmed |
Mesons in large-N QCD |
title_sort |
Mesons in large-N QCD |
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7e6fcfe060e07a351090e2a8aba363cf |
author_id_fullname_str_mv |
7e6fcfe060e07a351090e2a8aba363cf_***_Biagio Lucini |
author |
Biagio Lucini |
author2 |
Gunnar Bali Francis Bursa Luca Castagnini Sara Collins Luigi Debbio Biagio Lucini Marco Panero |
format |
Journal article |
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Journal of High Energy Physics |
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2013 |
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2013 |
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Swansea University |
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1029-8479 |
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10.1007/JHEP06(2013)071 |
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Faculty of Science and Engineering |
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description |
We present the results of a systematic, first-principles study of the spectrum and decay constants of mesons for different numbers of color charges N, via lattice computations. We restrict our attention to states in the non-zero isospin sector, evaluating the masses associated with the ground-state and first excitation in the pseudoscalar, vector, scalar, and axial vector channels. Our results are based on a new set of simulations of four dimensional SU(N) Yang-Mills theories with the number of colors ranging from N = 2 to N =17;the spectra and the decay constants are computed in the quenched approximation (which becomes exact in the ’t Hooft limit) using Wilson fermions. After discussing the extrapolations to the chiral and large-N limits, we present a comparison of our results to some of the numerical computations and analytical predictions available in the literature — including, in particular, those from holographic computations. |
published_date |
2013-12-31T03:17:24Z |
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1763750387309871104 |
score |
11.036706 |