2025-10-30 21:08 |
Combination of ATLAS and CMS searches for Higgs boson pair production at 13 TeV
/CMS Collaboration
This note presents a combination of searches for Higgs boson pair (HH) production performed by the ATLAS and CMS Collaborations using proton-proton collision data sets recorded at $\sqrt{s}$ = 13 TeV at the LHC Run 2, corresponding to integrated luminosities ranging between 126 and 140 $\mathrm{fb^{-1}}$. The upper limit at the 95\% confidence level on the total HH production cross section corresponds to 2.5 times the standard model (SM) prediction with an expected value of 1.7 (2.8) assuming the absence (presence) of the SM HH signal. [...]
CMS-PAS-HIG-25-014.-
Geneva : CERN, 2025
Figure_001: PDF; Figure_002-a: PDF; Figure_002-b: PDF; Figure_003: PDF; Figure_004: PDF; Figure_005: PDF; Figure_006: PDF; Figure_007: PDF; Figure_008: PDF; Figure_009: PDF; Figure_010: PDF; Figure_011: PDF; Figure_012: PDF; Figure_013: PDF; Figure_014: PDF; Figure_015: PDF; Figure_016: PDF; Figure_017: PDF; Figure_018: PDF; Figure_019-a: PDF; Figure_019-b: PDF; Figure_019-c: PDF; Figure_019-d: PDF; Figure_020-a: PDF; Figure_020-b: PDF; Figure_020-c: PDF; Figure_020-d: PDF; Fulltext in PDF: PDF; External link: Additional information for the analysis (restricted access)
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2025-10-29 10:44 |
Improved results on Higgs boson pair production in the 4b final state
/CMS Collaboration
Measurements of Higgs boson pair (HH) production in the four bottom quark final state are presented using a data set of proton-proton (pp) collisions at $\sqrt{s}=13.6~\mathrm{TeV}$ collected by the CMS experiment during 2022--2023 and corresponding to an integrated luminosity of $62~\mathrm{fb}^{-1}$. Events in which each Higgs boson decay is separately reconstructed as a pair of small-radius jets (resolved), as well as events in which each $\mathrm{H}\to\mathrm{b}\bar{\mathrm{b}}$ decay is reconstructed as a single large-radius jet (merged) are analyzed exclusively. [...]
CMS-PAS-HIG-24-010.-
Geneva : CERN, 2025
Figure_001-a: PDF; Figure_001-b: PDF; Figure_001-c: PDF; Figure_001-d: PDF; Figure_001-e: PDF; Figure_002-a: PDF; Figure_002-b: PDF; Figure_003-a: PDF; Figure_003-b: PDF; Figure_004-a: PDF; Figure_004-b: PDF; Figure_005-a: PDF; Figure_005-b: PDF; Figure_006-a: PDF; Figure_006-b: PDF; Figure_006-c: PDF; Figure_007-a: PDF; Figure_007-b: PDF; Figure_008-a: PDF; Figure_008-b: PDF; Figure_009: PDF; Figure_010-a: PDF; Figure_010-b: PDF; Figure_011-a: PDF; Figure_011-b: PDF; Figure_012-a: PDF; Figure_012-b: PDF; Figure_013-a: PDF; Figure_013-b: PDF; Figure_014: PDF; Figure_015-a: PDF; Figure_015-b: PDF; Figure_015-c: PDF; Figure_015-d: PDF; Figure_016-a: PDF; Figure_016-b: PDF; Figure_016-c: PDF; Figure_017-a: PDF; Figure_017-b: PDF; Figure_017-c: PDF; Figure_017-d: PDF; Figure_018: PDF; Figure_019-a: PDF; Figure_019-b: PDF; Figure_020-a: PDF; Figure_020-b: PDF; Figure_021-a: PDF; Figure_021-b: PDF; Figure_022-a: PDF; Figure_022-b: PDF; Figure_023: PDF; Figure_024-a: PDF; Figure_024-b: PDF; Figure_024-c: PDF; Figure_024-d: PDF; Figure_025-a: PDF; Figure_025-b: PDF; Figure_026-a: PDF; Figure_026-b: PDF; Figure_027-a: PDF; Figure_027-b: PDF; Figure_028-a: PDF; Figure_028-b: PDF; Fulltext in PDF: PDF; External link: Additional information for the analysis (restricted access)
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2025-10-27 14:09 |
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2025-10-24 17:49 |
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2025-10-22 11:27 |
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2025-10-21 09:42 |
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2025-10-20 11:09 |
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2025-10-07 18:11 |
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2025-10-06 18:35 |
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2025-10-02 15:46 |
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