Search for supersymmetry using Higgs boson to diphoton decays at sqrt{s} = 13 TeV

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Fernandez Bedoya,C Hajdú ,C Işik ,C K Mackay,C Madrid,C Martin Perez,C Martínez Rivero ,C Mora Herrera,C Neu,C Oropeza Barrera,C P A Roland ,C Peña ,C S Moon,C Scharf,C Schwanenberger,C Tuvé ,C Uribe Estrada,C Vander Velde,C Vellidis ,C Wissing,C Ávila ,Chia‐Ming Kuo ,Christopher T Hill ,Claudia-Elisabeth Wulz ,Cong Peng ,D A Sanz Becerra,D Blöch ,D De Jesus Damião ,D Del Re,D Di Croce,D Doḿınguez Damiani ,D E Marley ,D Ferenček ,D Horváth ,D K Mishra,D Kotliński ,D Matos Figueiredo,D R Mendis,D Soldi,D Sunar Cerci,D Ćutts ,Deepak Kumar Sahoo ,E A De Wolf,E Ayala,E Belchior Batista Das Chagas,E Carrera Jarrin,E Clément ,E De La Cruz-Burelo,E Di Marco,E Eskandari Tadavani,E Gurpinar Guler ,E J Tonelli Manganote,E M Da Costa,E Palencia Cortezon,E Popova,E Pérez ,Eric Wayne Vaandering ,F Canelli ,F De Guio,F Dölek ,F García ,F Gasparini,F M Stober,F Mohamad Idris,F Nessi‐Tedaldi ,F Pauß ,F Rezaei Hosseinabadi,F Siklér ,F Simonetto,F Torres Da Silva De Araujo,F Vazquez Valencia,F 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doi:10.1007/jhep11(2019)109

Abstract

A search for supersymmetry (SUSY) is presented where at least one Higgs boson is produced and decays to two photons in the decay chains of pair-produced SUSY particles. Two analysis strategies are pursued: one focused on strong SUSY production and the other focused on electroweak SUSY production. The presence of charged leptons, additional Higgs boson candidates, and various kinematic variables are used to categorize events into search regions that are sensitive to different SUSY scenarios. The results are based on data from proton-proton collisions at the Large Hadron Collider at a center-of-mass energy of 13 TeV collected by the CMS experiment, corresponding to an integrated luminosity of 77.5 fb−1. No statistically significant excess of events is observed relative to the standard model expectations. We exclude bottom squark pair production for bottom squark masses below 530 GeV and a lightest neutralino mass of 1 GeV; wino-like chargino-neutralino production in gauge-mediated SUSY breaking (GMSB) for chargino and neutralino masses below 235 GeV with a gravitino mass of 1 GeV; and higgsino-like chargino-neutralino production in GMSB, where the neutralino decays exclusively to a Higgs boson and a gravitino for neutralino masses below 290 GeV.

Highlights

A search for supersymmetry (SUSY) is presented where at least one Higgs boson is produced and decays to two photons in the decay chains of pair-produced SUSY particles
The results are based on data from proton-proton collisions at the Large Hadron Collider at a center-of-mass energy of 13 TeV collected by the CMS experiment, corresponding to an integrated luminosity of 77.5 fb−1
The production cross section for squark pair production is computed at next-to-leading order (NLO) plus next-to-leading logarithmic (NLL) accuracy in quantum chromodynamics (QCD) [25,26,27,28,29,30] under the assumption that all SUSY particles other than those in the relevant diagram are too heavy to participate in the interaction

Summary

The CMS detector

The central feature of the CMS detector is a superconducting solenoid of 6 m internal diameter, providing a magnetic field of 3.8 T. Within the solenoid volume are a silicon pixel and strip tracker, a lead tungstate crystal electromagnetic calorimeter (ECAL), and a brass and scintillator hadron calorimeter, each composed of a barrel and two endcap sections. Forward calorimeters extend the pseudorapidity (η) coverage provided by the barrel and endcap detectors. Muons are measured in gas-ionization detectors embedded in the steel flux-return yoke outside the solenoid. The first level of the CMS trigger system [12], composed of custom hardware processors, uses information from the calorimeters and muon detectors to select the most interesting events in a fixed time interval of less than 4 μs. The high-level trigger processor farm further decreases the event rate from around 100 kHz to less than 1 kHz before data storage. A more detailed description of the CMS detector, together with a definition of the coordinate system used and the relevant kinematic variables, can be found in ref. [13]

Event simulation

Event reconstruction and selection

Analysis strategy

Backgrounds

Systematic uncertainties

Results and interpretation

Summary

A Additional simplified model interpretations

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Journal: Journal of High Energy Physics	Publication Date: Nov 1, 2019
Citations: 39	License type: open-access

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