Search for W′ bosons decaying to a top and a bottom quark in leptonic final states in proton-proton collisions at √𝑠 = 13 TeV
A search for W′ bosons decaying to a top and a bottom quark in final states including an electron or a muon is performed with the CMS detector at the LHC. The analyzed data correspond to an integrated luminosity of 138 fb−1 of proton-proton collisions at a center-of-mass energy of 13 TeV. Good agree...
Main Authors: | , , , , , , , , , , , , , , , , |
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Other Authors: | |
Format: | Article |
Language: | English |
Published: |
Springer Science and Business Media LLC
2024
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Online Access: | https://hdl.handle.net/1721.1/155002 |
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author | Hayrapetyan, A. Tumasyan, A. Adam, W. Andrejkovic, J. W. Bergauer, T. Chatterjee, S. Damanakis, K. Dragicevic, M. Escalante Del Valle, A. Hussain, P. S. Jeitler, M. Krammer, N. Liko, D. Mikulec, I. Schieck, J. Schöfbeck, R. Schwarz, D. |
author2 | Massachusetts Institute of Technology. Department of Physics |
author_facet | Massachusetts Institute of Technology. Department of Physics Hayrapetyan, A. Tumasyan, A. Adam, W. Andrejkovic, J. W. Bergauer, T. Chatterjee, S. Damanakis, K. Dragicevic, M. Escalante Del Valle, A. Hussain, P. S. Jeitler, M. Krammer, N. Liko, D. Mikulec, I. Schieck, J. Schöfbeck, R. Schwarz, D. |
author_sort | Hayrapetyan, A. |
collection | MIT |
description | A search for W′ bosons decaying to a top and a bottom quark in final states including an electron or a muon is performed with the CMS detector at the LHC. The analyzed data correspond to an integrated luminosity of 138 fb−1 of proton-proton collisions at a center-of-mass energy of 13 TeV. Good agreement with the standard model expectation is observed and no evidence for the existence of the W′ boson is found over the mass range examined. The largest observed deviation from the standard model expectation is found for a W′ boson mass (
m
W
′
$$ {m}_{{\textrm{W}}^{\prime }} $$
) hypothesis of 3.8 TeV with a relative decay width of 1%, with a local (global) significance of 2.6 (2.0) standard deviations. Upper limits on the production cross sections of W′ bosons decaying to a top and a bottom quark are set. Left- and right-handed W′ bosons with
m
W
′
$$ {m}_{{\textrm{W}}^{\prime }} $$
below 3.9 and 4.3 TeV, respectively, are excluded at the 95% confidence level, under the assumption that the new particle has a narrow decay width. Limits are also set for relative decay widths up to 30%. |
first_indexed | 2024-09-23T13:29:21Z |
format | Article |
id | mit-1721.1/155002 |
institution | Massachusetts Institute of Technology |
language | English |
last_indexed | 2025-02-19T04:22:46Z |
publishDate | 2024 |
publisher | Springer Science and Business Media LLC |
record_format | dspace |
spelling | mit-1721.1/1550022025-02-04T02:25:12Z Search for W′ bosons decaying to a top and a bottom quark in leptonic final states in proton-proton collisions at √𝑠 = 13 TeV Hayrapetyan, A. Tumasyan, A. Adam, W. Andrejkovic, J. W. Bergauer, T. Chatterjee, S. Damanakis, K. Dragicevic, M. Escalante Del Valle, A. Hussain, P. S. Jeitler, M. Krammer, N. Liko, D. Mikulec, I. Schieck, J. Schöfbeck, R. Schwarz, D. Massachusetts Institute of Technology. Department of Physics A search for W′ bosons decaying to a top and a bottom quark in final states including an electron or a muon is performed with the CMS detector at the LHC. The analyzed data correspond to an integrated luminosity of 138 fb−1 of proton-proton collisions at a center-of-mass energy of 13 TeV. Good agreement with the standard model expectation is observed and no evidence for the existence of the W′ boson is found over the mass range examined. The largest observed deviation from the standard model expectation is found for a W′ boson mass ( m W ′ $$ {m}_{{\textrm{W}}^{\prime }} $$ ) hypothesis of 3.8 TeV with a relative decay width of 1%, with a local (global) significance of 2.6 (2.0) standard deviations. Upper limits on the production cross sections of W′ bosons decaying to a top and a bottom quark are set. Left- and right-handed W′ bosons with m W ′ $$ {m}_{{\textrm{W}}^{\prime }} $$ below 3.9 and 4.3 TeV, respectively, are excluded at the 95% confidence level, under the assumption that the new particle has a narrow decay width. Limits are also set for relative decay widths up to 30%. 2024-05-20T16:06:51Z 2024-05-20T16:06:51Z 2024-05-06 2024-05-19T03:13:11Z Article http://purl.org/eprint/type/JournalArticle 1029-8479 https://hdl.handle.net/1721.1/155002 The CMS collaboration., Hayrapetyan, A., Tumasyan, A. et al. Search for W′ bosons decaying to a top and a bottom quark in leptonic final states in proton-proton collisions at 𝑠√ = 13 TeV. J. High Energ. Phys. 2024, 46 (2024). PUBLISHER_CC en 10.1007/jhep05(2024)046 Journal of High Energy Physics Creative Commons Attribution https://creativecommons.org/licenses/by/4.0/ The Author(s) application/pdf Springer Science and Business Media LLC Springer Berlin Heidelberg |
spellingShingle | Hayrapetyan, A. Tumasyan, A. Adam, W. Andrejkovic, J. W. Bergauer, T. Chatterjee, S. Damanakis, K. Dragicevic, M. Escalante Del Valle, A. Hussain, P. S. Jeitler, M. Krammer, N. Liko, D. Mikulec, I. Schieck, J. Schöfbeck, R. Schwarz, D. Search for W′ bosons decaying to a top and a bottom quark in leptonic final states in proton-proton collisions at √𝑠 = 13 TeV |
title | Search for W′ bosons decaying to a top and a bottom quark in leptonic final states in proton-proton collisions at √𝑠 = 13 TeV |
title_full | Search for W′ bosons decaying to a top and a bottom quark in leptonic final states in proton-proton collisions at √𝑠 = 13 TeV |
title_fullStr | Search for W′ bosons decaying to a top and a bottom quark in leptonic final states in proton-proton collisions at √𝑠 = 13 TeV |
title_full_unstemmed | Search for W′ bosons decaying to a top and a bottom quark in leptonic final states in proton-proton collisions at √𝑠 = 13 TeV |
title_short | Search for W′ bosons decaying to a top and a bottom quark in leptonic final states in proton-proton collisions at √𝑠 = 13 TeV |
title_sort | search for w bosons decaying to a top and a bottom quark in leptonic final states in proton proton collisions at √𝑠 13 tev |
url | https://hdl.handle.net/1721.1/155002 |
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