Search for new physics in mono-jet final states in pp collisions : at sqrt(s)=13 TeV with the ATLAS Experiment at the LHC / Giuliano Gustavino.

4.5.2 Indirect Detection4.5.3 Run-1 Mono-Jet Results; 4.6 Effective Field Theory; 4.7 Simplified Models; 4.7.1 Vector and Axial-Vector Mediators; 4.7.2 Scalar and Pseudo-scalar Mediators; References; 5 Experimental Facilities; 5.1 The Large Hadron Collider; 5.1.1 Accelerator Complex; 5.1.2 LHC Performance; 5.2 The ATLAS Detector; 5.2.1 Coordinate System; 5.2.2 Magnets; 5.2.3 Tracking System; 5.2.4 Calorimeter System; 5.2.5 Muon Spectrometers; 5.2.6 Trigger System; References; 6 Physics Objects; 6.1 Electrons; 6.2 Photons; 6.3 Muons; 6.4 Jets; 6.5 Overlap Removal

6.6 Missing Transverse MomentumReferences; 7 The Mono-jet Analysis; 7.1 Data and MC Samples; 7.1.1 2015 Data Sample; 7.1.2 MC Simulations; 7.2 Event Selection; 7.3 Trigger; 7.4 Background Estimation; 7.4.1 Electroweak Background; 7.4.2 Diboson and Top Backgrounds; 7.4.3 Multi-jet Background; 7.4.4 Non-collision Background; 7.5 Fit Strategy; 7.6 Systematic Uncertainties; 7.6.1 Background Systematics; 7.6.2 Signal Systematics; 7.7 Background-Only Fit; 7.7.1 Impact of Systematic Uncertainties; 7.8 Validation of the Background Estimation Technique; 7.9 Results and Interpretations

Appendix A Signal Cross-SectionsAppendix B Signal Region Results; Appendix C Signal Expected Yields in the Signal Region; Appendix D Signal Limits; Curriculum Vitae