Please use this identifier to cite or link to this item:
https://hdl.handle.net/20.500.11851/12690
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DC Field | Value | Language |
---|---|---|
dc.contributor.author | Aad, Georges | - |
dc.contributor.author | Abbott, Brad K. | - |
dc.contributor.author | Abbott, D. C. | - |
dc.contributor.author | Abeling, Kira | - |
dc.contributor.author | Abidi, Syed Hani | - |
dc.contributor.author | Aboulhorma, Asmaa | - |
dc.contributor.author | Abusleme Hoffman, A. C. | - |
dc.date.accessioned | 2025-09-10T17:26:50Z | - |
dc.date.available | 2025-09-10T17:26:50Z | - |
dc.date.issued | 2025 | - |
dc.identifier.issn | 1029-8479 | - |
dc.identifier.uri | https://doi.org/10.1007/JHEP05(2025)159 | - |
dc.identifier.uri | https://hdl.handle.net/20.500.11851/12690 | - |
dc.description.abstract | Correction to one figure and the corresponding numbers in the text are noted for the paper. A wrong cross-section was used for the theory prediction of t¯tA(→ t¯t), which was estimated to differ by around 1% with respect to the one of t¯tH(→ t¯t). It was found later that the production cross-section for t¯tA(→ t¯t) can be up to 60% higher than the one of t¯tH(→ t¯t) for tan β ∼ 1. This affects the theoretical prediction shown in figure 7, and the limits in the tan β vs mH/A plane shown in figure 8(a). The changes in the text are noted for sections 8 and 9. • In the scenario where the scalar H and pseudo-scalar A bosons have equal masses and both contribute to BSM t¯tt¯t production, values of tan β below 1.9 and 0.7 are excluded for mH/A between 400 GeV and 1000 GeV, respectively, at 95% CL instead of 1.6 and 0.6. • In the scenario where only the pseudo-scalar A boson contributes to BSM t¯tt¯t production, values of tan β below 1.5 and 0.5 are excluded for mA between 400 GeV and 1000 GeV, respectively, at 95% CL instead of 1.2 and 0.5. The original plot for this scenario is not included in the paper as it was nearly identical to the one where only the scalar H boson contributes to BSM t¯tt¯t production, and was therefore omitted. After correction, the updated limits in the tan β vs mA plane are shown in figure 8(c). © 2025 Elsevier B.V., All rights reserved. | en_US |
dc.language.iso | en | en_US |
dc.publisher | Springer Science and Business Media Deutschland GmbH | en_US |
dc.relation.ispartof | Journal of High Energy Physics | en_US |
dc.rights | info:eu-repo/semantics/closedAccess | en_US |
dc.title | Erratum to: Search for (Formula Presented.) Production in the Multilepton Final State in Proton–Proton Collisions at (Formula Presented.) = 13 TeV with the ATLAS Detector (Journal of High Energy Physics, (2023), 2023, 7, (203), 10.1007/jhep07(2023)203) | en_US |
dc.type | Erratum | en_US |
dc.department | TOBB University of Economics and Technology | en_US |
dc.identifier.volume | 2025 | en_US |
dc.identifier.issue | 5 | en_US |
dc.identifier.scopus | 2-s2.0-105014099440 | - |
dc.identifier.doi | 10.1007/JHEP05(2025)159 | - |
dc.authorscopusid | 26326745400 | - |
dc.authorscopusid | 35226946900 | - |
dc.authorscopusid | 57208306618 | - |
dc.authorscopusid | 57210132793 | - |
dc.authorscopusid | 56536227400 | - |
dc.authorscopusid | 57246251500 | - |
dc.authorscopusid | 57202556479 | - |
dc.relation.publicationcategory | Diğer | en_US |
dc.identifier.scopusquality | Q1 | - |
dc.identifier.wosquality | Q1 | - |
item.cerifentitytype | Publications | - |
item.languageiso639-1 | en | - |
item.grantfulltext | none | - |
item.openairetype | Erratum | - |
item.openairecristype | http://purl.org/coar/resource_type/c_18cf | - |
item.fulltext | No Fulltext | - |
Appears in Collections: | Scopus İndeksli Yayınlar Koleksiyonu / Scopus Indexed Publications Collection |
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