Abstract

Results of a search for new phenomena in events with an energetic photon and large missing transverse momentum with the ATLAS experiment at the Large Hadron Collider are reported. The data were collected in proton--proton collisions at a centre-of-mass energy of 13 TeV and correspond to an integrated luminosity of 3.2 $\rm fb^{-1}$. The observed data are in agreement with the Standard Model expectations. Exclusion limits are presented in models of new phenomena including pair production of dark matter candidates or large extra spatial dimensions. In a simplified model of dark matter and an axial-vector mediator, the search excludes mediator masses of up to 710 GeV for dark matter candidate masses up to 150 GeV. In an effective theory of dark matter production, values of the suppression scale $M_*$ up to 570 GeV are excluded and the effect of truncation for various coupling values is reported. For the ADD large extra spatial dimension model the search places more stringent limits than earlier searches in the same event topology, excluding $M_{\rm D}$ up to about 2.3 (2.8) TeV for two (six) additional spatial dimensions; the limits are reduced by 20--40% depending on the number of additional spatial dimensions when applying a truncation procedure.

Highlights

  • Background estimationThe SM background to the γ + ETmiss final state is dominated by the Z(→ νν)γ process, where the photon is due to initial-state radiation

  • This paper focuses on simplified models assuming Dirac fermion DM candidates produced via an s-channel mediator with axial-vector interactions [12,13,14]

  • Systematic uncertainties from three different sources are added in quadrature: the difference between misidentification factors measured in data in two different windows around the Z mass (5 GeV and 10 GeV), the difference when measured in Z(→ ee) Monte Carlo (MC) events with the same method as used in data compared to using generator-level information, and the difference when measured in Z(→ ee) and W (→ eν) MC events using generator-level information

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Summary

The ATLAS detector

The ATLAS detector [18] is a multi-purpose particle physics apparatus with a forwardbackward symmetric cylindrical geometry and near 4π coverage in solid angle. The inner tracking detector (ID) covers the pseudorapidity range |η| < 2.5, and consists of a silicon. The inner tracking detector (ID) covers the pseudorapidity range |η| < 2.5, and consists of a silicon. The ID is surrounded by a thin superconducting solenoid providing a 2 T magnetic field. A high-granularity lead/liquid-argon sampling electromagnetic calorimeter covers the region |η| < 3.2 and is segmented longitudinally in shower depth. The second layer collects most of the energy deposited in the calorimeter in electromagnetic showers initiated by electrons or photons. Very high energy showers can leave significant energy deposits in the third layer, which can be used to correct for energy leakage beyond the EM calorimeter. The muon spectrometer (MS) surrounds the calorimeters It consists of three large air-core superconducting toroidal magnet systems, precision tracking chambers providing accurate muon tracking out to |η| = 2.7, and fast detectors for triggering in the region |η| < 2.4. A two-level trigger system is used to select events for offline analysis [20]

Monte Carlo simulation samples
Event reconstruction
Event selection
Background estimation
Zγ and W γ backgrounds
Fake photons from misidentified electrons
Fake photons from misidentified jets
Beam-induced background
Final background estimation
Results
Systematic uncertainties
Interpretation of results
10 Conclusion
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