CMS-PAS-FTR-21-003 | ||
Prospects for HH measurements in the WW$\gamma\gamma$ and $\tau\tau\gamma\gamma$ final states in proton-proton collisions at $\sqrt{s}=$ 14 TeV at the High Luminosity-LHC | ||
CMS Collaboration | ||
March 2022 | ||
Abstract: Prospects for nonresonant Higgs boson pair production measurements in the WW$\gamma\gamma$ and $\tau\tau\gamma\gamma$ final states in proton-proton collisions at a centre-of-mass energy of 14 TeV with the upgraded Phase-2 CMS detector at the High-Luminosity LHC (HL-LHC) are presented. The study is performed using generated events that passed DELPHES fast simulation of the CMS detector with an average of 200 proton-proton interactions per bunch crossing and an integrated luminosity of 3000 fb$^{-1}$. | ||
Links: CDS record (PDF) ; CADI line (restricted) ; |
Figures | |
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Figure 1:
Feynman diagrams for leading order Higgs boson pair production via gluon fusion. |
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Figure 1-a:
Feynman diagrams for leading order Higgs boson pair production via gluon fusion. |
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Figure 1-b:
Feynman diagrams for leading order Higgs boson pair production via gluon fusion. |
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Figure 2:
DNN output scores in the one lepton (left) and one tau (right) final states. |
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Figure 2-a:
DNN output scores in the one lepton (left) and one tau (right) final states. |
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Figure 2-b:
DNN output scores in the one lepton (left) and one tau (right) final states. |
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Figure 3:
$m_{\gamma \gamma}$ distributions in the WW$\gamma \gamma$, 1L (left) and ${\tau \tau \gamma \gamma}$, 1$\tau $ (right) final states. |
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Figure 3-a:
$m_{\gamma \gamma}$ distributions in the WW$\gamma \gamma$, 1L (left) and ${\tau \tau \gamma \gamma}$, 1$\tau $ (right) final states. |
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Figure 3-b:
$m_{\gamma \gamma}$ distributions in the WW$\gamma \gamma$, 1L (left) and ${\tau \tau \gamma \gamma}$, 1$\tau $ (right) final states. |
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Figure 4:
$m_{\gamma \gamma}$ distributions in the WW$\gamma \gamma$, 1L (top left), 2L (top right) and {\tau \tau \gamma \gamma}, 2$\tau $s (bottom) final states. |
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Figure 4-a:
$m_{\gamma \gamma}$ distributions in the WW$\gamma \gamma$, 1L (top left), 2L (top right) and {\tau \tau \gamma \gamma}, 2$\tau $s (bottom) final states. |
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Figure 4-b:
$m_{\gamma \gamma}$ distributions in the WW$\gamma \gamma$, 1L (top left), 2L (top right) and {\tau \tau \gamma \gamma}, 2$\tau $s (bottom) final states. |
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Figure 4-c:
$m_{\gamma \gamma}$ distributions in the WW$\gamma \gamma$, 1L (top left), 2L (top right) and {\tau \tau \gamma \gamma}, 2$\tau $s (bottom) final states. |
Tables | |
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Table 1:
One Lepton final state DNN score categories. |
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Table 2:
Selection criteria of the Two Lepton Channel. |
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Table 3:
Experimental uncertainties considered in this study. |
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Table 4:
Theoretical uncertainties considered on the ggHH signal and single Higgs processes. |
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Table 5:
Expected HL-LHC significances ($\sigma $) results of the WW$\gamma \gamma $ and ${\tau \tau \gamma \gamma}$ processes with their combination. |
Summary |
A measurement of non-resonant Higgs boson pair production in the WW$\gamma\gamma$ and ${\tau\tau\gamma\gamma}$ final states was performed in simulated proton-proton collision events at a centre-of-mass energy of 14 TeV and integrated luminosity of 3000 fb$^{-1}$ at the HL-LHC. Combining all final state categories and including systematic uncertainties, an expected significance 0.22$\sigma$ for signal is measured. |
References | ||||
1 | ATLAS Collaboration | Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC | PLB 716 (2012) 1 | 1207.7214 |
2 | CMS Collaboration | Observation of a New Boson at a Mass of 125 GeV with the CMS Experiment at the LHC | PLB 716 (2012) 30 | CMS-HIG-12-028 1207.7235 |
3 | CMS Collaboration | Observation of a New Boson with Mass Near 125 GeV in $ pp $ Collisions at $ \sqrt{s} = $ 7 and 8 TeV | JHEP 06 (2013) 081 | CMS-HIG-12-036 1303.4571 |
4 | DELPHES 3 Collaboration | DELPHES 3, A modular framework for fast simulation of a generic collider experiment | JHEP 02 (2014) 057 | 1307.6346 |
5 | CMS Collaboration | The CMS Experiment at the CERN LHC | JINST 3 (2008) S08004 | CMS-00-001 |
6 | CMS Collaboration | Technical Proposal for the Phase-II Upgrade of the CMS Detector | CMS-PAS-TDR-15-002 | CMS-PAS-TDR-15-002 |
7 | CMS Collaboration | The Phase-2 Upgrade of the CMS Tracker | CMS-PAS-TDR-17-001 | CMS-PAS-TDR-17-001 |
8 | CMS Collaboration | The Phase-2 Upgrade of the CMS Barrel Calorimeters Technical Design Report | CMS-PAS-TDR-17-002 | CMS-PAS-TDR-17-002 |
9 | CMS Collaboration | The Phase-2 Upgrade of the CMS Endcap Calorimeter | CMS-PAS-TDR-17-007 | CMS-PAS-TDR-17-007 |
10 | CMS Collaboration | The Phase-2 Upgrade of the CMS Muon Detectors | CMS-PAS-TDR-17-003 | CMS-PAS-TDR-17-003 |
11 | CMS Collaboration | A MIP Timing Detector for the CMS Phase-2 Upgrade | CMS-PAS-TDR-19-002 | CMS-PAS-TDR-19-002 |
12 | CMS Collaboration | The Phase-2 Upgrade of the CMS Level-1 Trigger | CMS-PAS-TDR-20-001 | CMS-PAS-TDR-20-001 |
13 | CMS Collaboration | The Phase-2 Upgrade of the CMS Data Acquisition and High Level Trigger | CDS | |
14 | CMS Collaboration | Expected performance of the physics objects with the upgraded CMS detector at the HL-LHC | CDS | |
15 | P. Nason | A New method for combining NLO QCD with shower Monte Carlo algorithms | JHEP 11 (2004) 040 | hep-ph/0409146 |
16 | S. Frixione, P. Nason, and C. Oleari | Matching NLO QCD computations with Parton Shower simulations: the POWHEG method | JHEP 11 (2007) 070 | 0709.2092 |
17 | S. Alioli, P. Nason, C. Oleari, and E. Re | A general framework for implementing NLO calculations in shower Monte Carlo programs: the POWHEG BOX | JHEP 06 (2010) 043 | 1002.2581 |
18 | G. Heinrich et al. | Probing the trilinear Higgs boson coupling in di-Higgs production at NLO QCD including parton shower effects | JHEP 06 (2019) 066 | 1903.08137 |
19 | T. Sjostrand et al. | An Introduction to PYTHIA 8.2 | CPC 191 (2015) 159 | 1410.3012 |
20 | J. Alwall et al. | The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations | JHEP 07 (2014) 079 | 1405.0301 |
21 | P. Artoisenet, R. Frederix, O. Mattelaer, and R. Rietkerk | Automatic spin-entangled decays of heavy resonances in Monte Carlo simulations | JHEP 03 (2013) 015 | 1212.3460 |
22 | R. Frederix and S. Frixione | Merging meets matching in MC@NLO | JHEP 12 (2012) 061 | 1209.6215 |
23 | Sherpa Collaboration | Event Generation with Sherpa 2.2 | SciPost Phys. 7 (2019), no. 3, 034 | 1905.09127 |
24 | CMS Collaboration | Performance of the DeepJet b tagging algorithm using 41.9/fb of data from proton-proton collisions at 13TeV with Phase 1 CMS detector | CDS | |
25 | E. Bols et al. | Jet Flavour Classification Using DeepJet | JINST 15 (2020), no. 12, P12012 | 2008.10519 |
26 | A. Dainese et al. | Report on the Physics at the HL-LHC, and Perspectives for the HE-LHC | technical report, Geneva, Switzerland | |
27 | The ATLAS Collaboration, The CMS Collaboration, The LHC Higgs Combination Group Collaboration | Procedure for the LHC Higgs boson search combination in Summer 2011 | technical report, CERN, Geneva, Aug |
Compact Muon Solenoid LHC, CERN |