Photons, Missing Energy and the Quest for Supersymmetry at the LHC
|
|
- Joshua Mitchell
- 5 years ago
- Views:
Transcription
1 Photons, Missing Energy and the Quest for Supersymmetry at the LHC Ulla Gebbert Thesis Defense
2 Motivation pp pp LHC: first pp-collisions in November 2009! Soon after: highest-energy particle accelerator on earth Susy Since March 2010: s = 7 TeV, L dt = ~5 fb-1 SM Higgs Boson Higgs 7 Searches for new physics 2
3 Outline 0. Introduction Standard Model Supersymmetry - and Photons? CMS Detector 1. Measuring the Missing Transverse Energy Reconstruction Corrections Large ET 2. Search for Supersymmetry in Events with Photons, Jets and ET Event Selection SM Backgrounds Results & Interpretation 3. Summary and Outlook 3
4 The Standard Model (SM) SM particles u c t g d s b γ νe νµ ντ W e µ τ Z γ Electromagnetic Force: Electric charge: q, e, µ, τ, W± ± H g - Strong Force: Colour: quarks & gluons quarks leptons Fermions Spin 1/2 Basic constituents of matter W±,Z0 - Weak Force: Weak isospin: left-handed fermions, W±,Z0 SU(2)L U(1)Y SU(3)C Bosons Spin 1 Spin 0 Mediators of forces Higgs: Accommodate massive gauge fields (MW/Z GeV) No experimental evidence hints at ~125 GeV? mh GeV (LEP), mh 127 GeV mh 600 GeV (CMS) 4
5 The Standard Model and beyond? Dark Matter? Unification of Forces? Origin unsolved within Standard Model Grand Unified Theories (GUTs) G SU(3) SU(2) U(1) SM SM? More fundamental theory? SUSY? Gravity? Naturalness of the SM? Number of free parameters? Number of generations? Masses of particles?... 5
6 The Standard Model and beyond? Dark Matter? Unification of Forces? Grand Unified Theories (GUTs) G SU(3) SU(2) U(1) SM Origin unsolved within Standard Model Lightest SUSY particle? SM? More fundamental Theory? SUSY SUSY? Gravity? SUSY? Naturalness of the SM? Number of free parameters? Number of generations? Masses of particles?
7 Supersymmetry Minimal Supersymmetric Standard Model (MSSM) u c t g d s b γ νe νµ ντ W± e µ τ Z quarks leptons Fermions ~ u ~ c ~t h0 H0 ~ d ~ s ~ b H± A 0 ν~e ν~µ ν~τ χ~10 ~ χ20 ~ χ30 ~ χ40 ~ e ~ µ ~τ ~ χ1± ~ χ2± Extension Bosons ~ g squarks sleptons Bosons Fermions Each SM particle linked to a supersymmetric particle (boson fermion) 7
8 Supersymmetry Minimal Supersymmetric Standard Model (MSSM) u c t g d s b γ νe νµ ντ W± e µ τ Z ~ u ~ c ~t h0 H0 ~ d ~ s ~ b H± A 0 ν~e ν~µ ν~τ χ~10 ~ χ20 ~ χ30 ~ χ40 ~ e ~ µ ~τ ~ χ1± ~ χ2± quarks leptons Fermions ~ g squarks sleptons Bosons Bosons Mass Eigenstates Fermions Each SM particle linked to a supersymmetric particle (Boson Fermion) 8
9 Supersymmetry Minimal Supersymmetric Standard Model (MSSM) u c t d s b νe νµ ντ e µ τ g 1 W W2 W3 B0 Hu0,Hd0, Hd,Hu+ quarks leptons Fermions ~ u ~ c ~t ~ d ~ s ~ b ν~e ν~µ ν~τ ~ e ~ µ ~τ ~ g Gauge Eigenstates ~ ~ B0,W0, ~ W± ~ ~ Hu+,Hd~ ~ Hu0,Hd0 squarks sleptons Bosons Bosons Mass Eigenstates Fermions Each SM particle linked to a supersymmetric particle (boson fermion) 9
10 Supersymmetry Minimal Supersymmetric Standard Model (MSSM) u c t g d s b γ νe νµ ντ W± e µ τ Z ~ u ~ c ~t h0 H0 ~ d ~ s ~ b H± A 0 ν~e ν~µ ν~τ χ~10 ~ χ20 ~ χ30 ~ χ40 ~ e ~ µ ~τ ~ χ1± ~ χ2± quarks leptons ~ g Gauge Eigenstates squarks sleptons Fermions Bosons PR=+1 Bosons Mass Eigenstates Fermions PR=-1 Each SM particle linked to a supersymmetric particle (boson fermion) Conservation of lepton/baryon number: R-Parity PR=(-1)3(B-L)+2S Pair production of SUSY particles at a collider Stable, lightest supersymmetric particle (LSP) Same colour, electrical charge, isospin and mass broken symmetry? 10
11 SUSY Breaking SUSY breaking in 'hidden' sector Different models exist, e.g: msugra: 'minimal supergravity' SM Gravity SUSY breaking 'hidden' sector GMSB: 'gauge mediated SUSY breaking' SM Messenger fields SU(3)C SU(2)L U(1)Y SUSY breaking 'hidden' sector Model independent framework: 'General Gauge Mediation' (GGM) Universal prediction: Gravitino LSP P. Meade, N. Seiberg, D. Shih, arxiv: v3 Lightest MSSM particle: NLSP 11
12 GGM Phenomenology at the LHC Typical production (LHC): squarks & gluinos R-parity conserved: two LSP's per event Neutralino NLSP mixture of Bino, Wino and Higgsino Y. Kats, et. al arxiv:
13 GGM Phenomenology at the LHC Typical production (LHC): squarks & gluinos R-parity conserved: two LSP's per event Neutralino NLSP mixture of Bino, Wino and Higgsino Final states with photons: γγ + ET +X J. Ruderman, D.Shih ArXiv: v1 Bino-like NLSP 13
14 GGM Phenomenology at the LHC Typical production (LHC): squarks & gluinos R-parity conserved: two LSP's per event Neutralino NLSP mixture of Bino, Wino and Higgsino Final states with photons: γγ + ET +X and γ + ET +X Wino-like NLSP J. Ruderman, D.Shih ArXiv: v1 14
15 GGM Phenomenology at the LHC Typical production (LHC): squarks & gluinos R-parity conserved: two LSP's per event Neutralino NLSP mixture of Bino, Wino and Higgsino Final states with photons: γγ + ET +X and γ + ET +X Wino-like NLSP J. Ruderman, D.Shih ArXiv: v1 15
16 GGM Phenomenology at the LHC Typical production (LHC): squarks & gluinos Wino-like NLSP R-parity conserved:two LSP's per event Neutralino NLSP mixture of Bino, Wino and Higgsino Final states with photons: γγ + ET and γ + ET (+jets/b-jets/leptons) Variety of other final states (without γ, non-prompt NLSP decay,...) Bino-like NLSP 16
17 GGM Phenomenology at the LHC Typical production (LHC): squarks & gluinos Wino-like NLSP R-parity conserved:two LSP's per event Neutralino NLSP mixture of Bino, Wino and Higgsino Final states with photons: γγ + ET and γ + ET (+jets/b-jets/leptons) Variety of other final states (without γ, non-prompt NLSP decay,...) Bino-like NLSP 17
18 CMS Detector Length:14.6m, 21.6 m, t 3.8 T solenoid enclosing calorimetry Tracker: good resolution & reconstruction efficiency H bb, SUSY with b/τ Electromagnetic calorimeter: excellent resolution (e,γ) H γγ, Z' ee, GGM Muon system: wide acceptance & charge measurement H ZZ µ+µ µ+µ,z' µ+µ Hadronic calorimeter Jets & ET: good hermetic coverage & resolution needed ET: needed for many SUSY & BSM searches technically challenging reconstruction 18
19 Outline 0. Introduction Standard Model Supersymmetry - and Photons? CMS Detector 1. Measuring the Missing Transverse Energy Reconstruction Corrections Large ET 2. Search for Supersymmetry in Events with Photons, Jets and ET Event Selection SM Backgrounds Results & Interpretation 3. Summary and Outlook 19
20 ET Reconstruction CMS 3 different algorithms commissioned hadronic calorimeter electromagnetic calorimeter Calo ET: Use only calorimetric energy deposits 20
21 ET Reconstruction CMS 3 different algorithms commissioned hadronic calorimeter electromagnetic calorimeter Calo ET: Use only calorimetric energy deposits tracker TC ET: Inclusion of the measured track momenta Correction of calorimeter only measurement 21
22 ET Reconstruction CMS 3 different algorithms commissioned hadronic calorimeter electromagnetic calorimeter Calo ET: Use only calorimetric energy deposits muon chambers tracker TC ET: Inclusion of the measured track momenta Correction of calorimeter only measurement PF ET: Use calibrated particles ( particle flow ) 22
23 Correction of the Measurement Non linear response HCAL Jet Energy Corrections (JEC) corrections needed Unclustered energy deposits in calorimeter below pt thresholds for other physics objects Derive correction from Z ee events: Use balance between Z boson momentum and recoil from: JINST 6 (2011) P11002 Type-I: Type-II: Correct ET for the difference between jets before/after JEC Correct ET for the difference between unclustered deposits before/after correction 23
24 Derivation of Type II Corrections Z ee if: no jets above JEC threshold 24
25 Derivation of Type II Corrections Measure <R> in dependence of qt: Calo ET 25
26 Derivation of Type II Corrections Measure <R> in dependence of qt: Calo ET 26
27 Derivation of Type II Corrections Measure <R> in dependence of qt: Calo ET Correction applicable to different event topologies! 27
28 Derivation of Type II Corrections Resulting correction: Z, rel= Calo ET Z p T U meas, Z pt Data-driven derivation Small (36/pb) dataset functional form from simulation Data/simulation agree within uncertainties PF ET: Similar results, smaller correction 28
29 Validation in Di jet Events Good performance in Z ee events test in other event topology (di jet) Di-jet Dominated by unclustered energy 29
30 ET scale in Di jet Events Calo ET published in: JINST 6 (2011) P09001 Type II reduces negative offset large effect for Calo ET: scale within 2 GeV down to lowest pt PF ET published in: JINST 6 (2011) P09001 Smaller, but similar effect for PF ET: already well adjusted (<2 GeV) Scale well adjusted after type II corrections for both ET algorithms 30
31 ET Resolution in Multi jet Events Calo ET Type-I Calo ET Type-II TC ET PF ET includes tracking information from: JINST 6 (2011) P09001 //AN Type-II correction improves Calo ET resolution Resolution improved clearly by inclusion of tracking information 31
32 SUSY: ET Tails sensitive to instrumental mismeasurement Anomalous calorimeter signals Non collision particles Non instrumented/non functioning detector regions... Additional contributions to tail of ET distribution crucial for analyses requiring high ET, e.g. SUSY searches from: JINST 6 (2011) P
33 Outline 0. Introduction Standard Model Supersymmetry - and Photons? CMS Detector 1. Measuring the Missing Transverse Energy Reconstruction Corrections Large ET 2. Search for Supersymmetry in Events with Photons, Jets and ET Event Selection SM Backgrounds Results & Interpretation 3. Summary and Outlook 33
34 Event Selection Final states with only one, jets + MET MET 366 GeV Jets (>=2) + MET + Photon Photon 96 GeV Lumi [fb 1] Trigger Photons Jets Photon-HT >=1, pt>80 GeV 2*,HT*>450 > 100 GeV 4.3 GeV pt > 30 GeV γ pt>70 GeV η <1.44 HT>400 GeV ET >=2 jets η <2.6 *scalar pt sum of jets (calorimeter jets, pt>40 GeV, η <3.0, cleaned from e,µ & leading γ) *particle flow jets, anti kt (R=0.5), cleaned from e,µ & leading γ 34
35 SM Background: γ/qcd Main background: γ/qcd Multi-jet: jet photon Photon-jet No intrinsic ET But: jet resolution, non-gaussian tails,... Data driven estimate: 1)Select γjet control sample γjet: similar to γ, looser isolation Orthogonal selection C Photon p T = Fake Photon Photon 35
36 SM Background: γ/qcd Main background: γ/qcd Multi-jet: jet photon Photon-jet No intrinsic ET But: jet resolution, non-gaussian tails,... Data driven estimate: 1)Select γjet control sample 2)Derive event weight w-1: Control region (ET<100 GeV) C Photon p T = 2 jets Fake Photon Photon >=3 jets 36
37 SM Background: γ/qcd Main background QCD: Multi-jet: jet photon Photon-jet No intrinsic ET But: jet resolution, non-gaussian tails,... Data driven estimate: 1)Select γjet control sample 2)Derive event weight w-1: Control region (ET<100 GeV) C Photon p T = Fake Photon Photon 3)Reweight γjet control sample Estimate for background Systematic uncertainties: Extrapolation from low to high ET < 5% Statistical uncertainty of w-1 Closure Test 37
38 SM Background: e γ (EWK) Minor background: e γ (EWK) tt+jets e γ, W+jets intrinsic ET from ν's Data driven estimate 1)Select γe (electron) control sample γe: same as γ, but require track 2)Z ee (ratio ee/eγ): derive fake rate γ pt > 80 GeV: C Photon p T = 3) Reweight γe control sample Estimate for background Fake Photon Photon Fit for γ>80 GeV taken from: AN (γγ) 38
39 Results: Observation & Expectation Signal region: 6 bins with ET > 100 GeV Data driven estimation for QCD & EWK Simulation for FSR/ISR No excess over the SM expectation observed 39
40 Interpretation Limit calculation: Use 6 bins with ET>100 GeV CLs, frequentist approach based on RooStats Systematic uncertainties (signal): Experimental: Photon efficiency in data/mc: 4% Jet energy scale 2% Luminosity 4.5% PDF uncert. on the acceptance ~ % Theoretical: PDF uncert. on cross section (10-70%) Renormalisation scale (10-30%) Three different GGM scenarios studied: Bino-like NLSP Wino-like NLSP 40
41 Interpretation Bino, ~ q vs. ~ g Typical acceptance: ET>100 GeV ~ 75% ET>350 GeV ~ 12% mgluino>msquark: more (high pt) jets Acceptance drops: Mass Neutralino Mass Gluino/Squark 41
42 Interpretation Bino, ~ q vs. ~ g Typical acceptance: ET>100 GeV ~ 75% ET>350 GeV ~ 12% Observed cross section limit, 95% CL ~0.01 pb Exclude: Mgluino < 960 GeV Msquark < 1040 GeV 42
43 ~ ~ Interpretation Bino, χ10 vs. g Typical acceptance: ET>100 GeV ~ 60-80% ET>350 GeV ~ 10-15% Observed cross section limit, 95% CL ~ pb Exclude: Mgluino < GeV, if Mχ < 800 GeV 43
44 ~ ~ Interpretation Bino, χ10 vs. g Typical acceptance: ET>100 GeV ~ 60-80% ET>350 GeV ~ 10-15% Observed cross section limit, 95% CL ~ pb Exclude: Mgluino < GeV, if Mχ < 800 GeV CMS γγ (4.7/fb) ATLAS γγ (1/fb) 44
45 ~ vs. g ~ Interpretation Wino, q Typical acceptance: ET>100 GeV ~ 8% ET>350 GeV ~ 1% Observed cross section limit, 95% CL ~0.1 pb Exclude: Mgluino < 730 GeV Msquark < 780 GeV 45
46 ~ vs. g ~ Interpretation Wino, q Typical acceptance: ET>100 GeV ~ 8% ET>350 GeV ~ 1% Observed cross section limit, 95% CL ~0.1 pb Exclude: Mgluino < 730 GeV Msquark < 780 GeV Most stringent limit on wino-like neutralino to date CMS γ+l (36/pb) ~ 450 GeV γγ : no published limits, much lower acceptances ( 6-10) 46
47 Results: γ + jets + ET Extend previous CMS GMSB SUSY searches: single photon, jets & ET Data driven estimates for main backgrounds (QCD,EWK) Further background (ISR/FSR TTBar, V+Jets) from simulation No excess in data observed Limits calculated for wino- and bino-like neutralino 4.3/fb results made public in PAS-SUS Luminosity 4.3 fb-1 +/- 4.5% Acceptance times efficiency Upper Limit cross section Msquark > Mgluino > Bino-like: ~ 80 % ~ 0.01 pb-1 ~ 960 GeV ~ 1040 GeV Similar (slightly lower) sensitivity than CMS γγ (SUS ) presented at Moriond 2012 paper in preparation Wino-like: ~8 % ~0.1 pb-1 ~780 GeV ~730 GeV Most stringent limit to date 47
48 Outline 0. Introduction Standard Model Supersymmetry - and Photons? CMS Detector 1. Measuring the Missing Transverse Energy Reconstruction Corrections Large ET 2. Search for Supersymmetry in Events with Photons, Jets and ET Event Selection SM Backgrounds Results & Interpretation 3. Summary and Outlook 48
49 Summary (1/2) ET: key ingredient to many SUSY & other BSM searches (not only GMSB) High ET : sensitive to misreconstruction non linear response of the calorimeter scale can be adjusted with type I/II corrections Inclusion of tracking: significantly lower resolution CMS has 3 different, well tested ET algorithms commissioned JINST 6 (2011) P09001 Several complementary measurements show excellent performance of ET Eur. Phys. J. C72 (2012) Measuring the Missing Transverse Energy JINST 6 (2011) P
50 Summary (2/2) Final states with photons expected in GGM SUSY scenarios Variety of possible final states including γ + ET + jets Branching ratios to photon & W,Z,H depend on neutralino mixture CMS has performed several analyses covering many of the possible final states Final states with photons: JHEP 1106 (2011), 36/pb γ + E + lepton T γ + ET + >=2 jets γγ + ET + >=1 jet presented here SUS , /fb Most stringent limits on GGM gluino/squark production to date Msquark Mgluino Bino-like: > ~ 1000 GeV > ~ 1100 GeV 1. Measuring the Missing Transverse Energy Wino-like: ~800 GeV ~700 GeV 50
51 Outlook (1/4) LHC results: challenging large parts of the SUSY parameter space msugra parameter space: CMS-PAS-SUS Measuring the Missing Transverse Energy ATLAS-CONF
52 Outlook (2/4) LHC results: challenging SUSY reach further! 1) Optimize analyses e.g. γ+jets+et (wino-like): High masses: EWK production less stringent jet selection? leptons? More exotic, less inclusive: additional b-jets (higgsino-like NLSP)? 1. Measuring the Missing Transverse Energy 52
53 Outlook (3/4) LHC results: challenging SUSY reach further! 1) Optimize analyses e.g. γ+jets+et (wino-like): High masses: EWK production less stringent jet selection? leptons? More exotic, less inclusive: additional b-jets (higgsino-like NLSP)? Taken from: L. Hill, LBNL SUSY Workshop ) New searches EWK production Low ET 3rd generation, e.g. stop Intermediate (via gluino): mg< 800 GeV Direct production: no LHC result ~ mstop < GeV 1. Measuring the Missing Transverse Energy Reinterpretation of LHC results Taken from: M. Papucci, et. al. arxiv: v1 53
54 Outlook LHC 2012 (4/4) Higher beam energies (8 TeV), higher luminosity +400 % +30% Taken from: Chamonix '12 Summary, CERN Find or exclude (SM?) Higgs SUSY? Other BSM? Measuring the Missing Transverse Energy 54
55 Backup 55
56 Analysis: γ+jets+met 56
57 Trigger efficiencies 57
58 Systematic uncertainties 58
59 >=3 jets 59
60 60
61 Sample Limit Calculation pb obs. upper limit Total number of signal events 61
62 Contributions from individual bins 62
63 Signal Contamination 63
64 Theor. Uncert. on cross section 64
65 GGM model parameter 65
66 Higgsino-like NLSP higgsino-like NLSP 66
67 SM Background: ISR/FSR Further background: ISR/FSR tt+jets initial/final state radiation of γ, W/Z+jets intrinsic E from ν's T Use MC simulation to estimate contribution Madgraph + Pythia no events with electrons on generator level (estimated already by fe->y) Assign conservative systematic uncertainty: 100% C Photon p T = Fake Photon Photon 67
68 SM Background: QCD 68
69 SM Background: e γ (EWK) Closure Test 69
70 Number of jet dependency 70
71 Theoretical uncertainties 71
72 2 vs 3 jet selection 72
73 Eventdisplays MET tail Punch-through? Masked ECAL? 73
74 Photon/Electron ID Object definitions very similar to di-photon, but No additional IsoVL cuts applied (needed due to trigger requirements for di-photon Higher upper cut on fake-photon isolation to ensure statistics PU correction derived with same methods, but for the slightly different photon Id Details: Photon ID (isolation cone 0.3):!hasPixelSeed() R9()<1 CombinedIsolation*<6 GeV σiηiη<0.011 H/E<0.05 Combined isolation = ecaliso() *rho + hcaliso() *rho +trackiso() < 6 GeV Fake Photon ID (jet FO) (isolation cone 0.3) Same as photon, but: CombinedIsolation> 6 σiηiη>0.011 CombinedIsolation* < min(30,0.3*pt) *CombinedIsolation=ecalIso**+hcalIso**+trackIso **PU correction for ecal/hcal iso applied: EcalIso=ecalIso() *rho(eta<2.5) HcalIso=hcalIso() *rho(eta<2.5) Electron ID: like photon but with pixel seed 74
75 Analysis: MET 75
76 Pf Corrections 76
77 Data driven results: all data points 77
78 Performance in Z ee 78
79 Performance in Z ee 79
80 Systematic uncertainties Quark-gluon- composition:1.5-6 % UT vs U: ~4 GeV negligible effect on scale compared to other uncert. 80
81 Minimum Bias 81
82 Punchthrough & masked ECAL Mask ECAL cells in simulation (only the ones masked in the real detector) 82
83 Z ee event selection pt>20 GeV 60 GeV< Minv<120 GeV 83
84 Higgs searches 84
85 Higgs 85
86 Higgs 86
87 SUSY & Higgs 87
88 CMS 88
89 UED CMS-PAS-SUS
90 Long lived NLSP CMS-PAS-EXO
91 JES From: JINST 6 (2011) P
92 CMS material thickness 92
93 CMS detector photons EB edge η =1.479 leptons ME edge η =2.1 jets HF edge η =2.6 beam line Interaction point 93
94 Event reconstruction 94
95 ATLAS Exotica Summary 95
96 ATLAS Summary 96
CMS Searches for New Physics
CMS Searches for New Physics Christian Autermann, for the CMS collaboration I. Phys. Inst. RWTH Aachen University, Germany QCD14 2 Overview Searches for New Physics at CMS Inclusive search for Supersymmetry
More informationEarly SUSY Searches in Events with Leptons with the ATLAS-Detector
Early SUSY Searches in Events with Leptons with the ATLAS-Detector Timo Müller Johannes Gutenberg-Universität Mainz 2010-29-09 EMG Annual Retreat 2010 Timo Müller (Universität Mainz) Early SUSY Searches
More informationStudy of supersymmetric tau final states with Atlas at LHC: discovery prospects and endpoint determination
Study of supersymmetric tau final states with Atlas at LHC: discovery prospects and endpoint determination University of Bonn Outlook: supersymmetry: overview and signal LHC and ATLAS invariant mass distribution
More informationSUSY Phenomenology & Experimental searches
SUSY Phenomenology & Experimental searches Alex Tapper Slides available at: http://www.hep.ph.ic.ac.uk/tapper/lecture.html Reminder Supersymmetry is a theory which postulates a new symmetry between fermions
More informationHadronic Search for SUSY with MT2 variable
Hadronic Search for SUSY with MT2 variable Esmaeel Eskandari on behalf of the CMS Collaboration School of Particles & Accelerators, Institute for Research in Fundamental Sciences (IPM) The 2nd IPM Meeting
More informationThe search for missing energy events at the LHC and implications for dark matter search (ATLAS and CMS)
The search for missing energy events at the LHC and implications for dark matter search (ATLAS and CMS) Valery P. Andreev UCLA representing the CMS collaboration th UCLA Symposium on Sources and Detection
More informationSeaches fo log-lived paticles with displaced signatues at the LHC. Daniela Salvatore (INFN Cosenza) on behalf of the ATLAS and CMS Collaborations
Seaches fo log-lived paticles with displaced signatues at the LHC Daniela Salvatore (INFN Cosenza) on behalf of the ATLAS and CMS Collaborations Outline A review of the most recent results from ATLAS &
More informationSearches for SUSY & Exotics with ATLAS
Searches for SUSY & Exotics with ATLAS Evelyn Thomson University of Pennsylvania May 17 2017 BLV 2017 Cleveland, Ohio 1 Outline Introduction Supersymmetry searches Gluinos Scalar top Electroweakinos Exotic
More informationSearches for exotica at LHCb
Searches for exotica at LHCb Lorenzo Sestini Università di Padova e INFN LHCb Implications Workshop, Geneve-Cern, 3-11-2015 Searches for exotics LHCb can be complementary to ATLAS and CMS in the search
More informationStop NLSPs. David Shih Rutgers University. Based on: Kats & DS ( ) Kats, Meade, Reece & DS ( )
Stop NLSPs David Shih Rutgers University Based on: Kats & DS (06.0030) Kats, Meade, Reece & DS (0.6444) This year, the LHC has performed extremely well. ATLAS and CMS have collected over 5/fb of data each!!
More informationSearch for SUSY at CMS in lepton or photon final states. PANIC 2011 K. Theofilatos (on behalf of CMS)
Search for SUSY at CMS in lepton or photon final states CMS in one slide Optimal design for reconstructing leptons & photons Compact & precisely aligned detector with B=3.8 T Calorimeters operating inside
More informationHiggs Searches at CMS
Higgs Searches at CMS Ashok Kumar Department of Physics and Astrophysics University of Delhi 110007 Delhi, India 1 Introduction A search for the Higgs boson in the Standard Model (SM) and the Beyond Standard
More informationUpgrade of ATLAS and CMS for High Luminosity LHC: Detector performance and Physics potential
IL NUOVO CIMENTO 4 C (27) 8 DOI.393/ncc/i27-78-7 Colloquia: IFAE 26 Upgrade of ATLAS and CMS for High Luminosity LHC: Detector performance and Physics potential M. Testa LNF-INFN - Frascati (RM), Italy
More informationSearches for Supersymmetry at ATLAS
Searches for Supersymmetry at ATLAS Renaud Brunelière Uni. Freiburg On behalf of the ATLAS Collaboration pp b b X candidate 2 b-tagged jets pt 52 GeV and 96 GeV E T 205 GeV, M CT (bb) 20 GeV Searches for
More informationSUSY at Accelerators (other than the LHC)
SUSY at Accelerators (other than the LHC) Beate Heinemann, University of Liverpool Introduction Final LEP Results First Tevatron Run 2 Results Summary and Outlook IDM 2004, Edinburgh, September 2004 Why
More information14th Lomonosov Conference on Elementary Particle Physics Moscow, 24 August 2009
M. Biglietti University of Rome Sapienza & INFN On behalf of the ATLAS Collaboration 1 14th Lomonosov Conference on Elementary Particle Physics Moscow, 24 August 2009 Theoretically favored candidates for
More informationDiscovery Physics at the Large Hadron Collider
+ / 2 GeV N evt 4 10 3 10 2 10 CMS 2010 Preliminary s=7 TeV -1 L dt = 35 pb R > 0.15 R > 0.20 R > 0.25 R > 0.30 R > 0.35 R > 0.40 R > 0.45 R > 0.50 10 1 100 150 200 250 300 350 400 [GeV] M R Discovery
More informationarxiv: v1 [hep-ph] 29 Dec 2017 SUSY (ATLAS) André Sopczak on behalf of the ATLAS Collaboration
arxiv:1712.10165v1 [hep-ph] 29 Dec 2017 SUSY (ATLAS) André Sopczak on behalf of the ATLAS Collaboration Institute of Experimental and Applied Physics, Czech Technical University in Prague, Czech Republic
More informationTaller de Altas Energías Michael Holzbock September 7, LMU Munich
Search for top squark pair production in final states with two τ leptons, jets, and missing transverse momentum in s = TeV pp-collisions with the ATLAS detector Taller de Altas Energías 6 Michael Holzbock
More informationInclusive searches in ATLAS: How can we discover SUSY in 2009
Inclusive searches in ATLAS: How can we discover SUSY in 2009 George Redlinger Brookhaven National Laboratory (for the ATLAS Collaboration) University of Michigan LHC Dark Matter Workshop 6-10 Jan 2009
More informationOutline: Introduction Search for new Physics Model driven Signature based General searches. Search for new Physics at CDF
PE SU Outline: Introduction Search for new Physics Model driven Signature based General searches R Search for new Physics at CDF SUperSYmmetry Standard Model is theoretically incomplete SUSY: spin-based
More informationSearch for squarks and gluinos with the ATLAS detector. Jeanette Lorenz (LMU München)
Search for squarks and gluinos with the ATLAS detector Jeanette Lorenz (LMU München) Research Area B Science Day, Supersymmetry Symmetry between fermions and bosons Only possible extension of Poincare
More informationSUSY at Accelerators (other than the LHC)
SUSY at Accelerators (other than the LHC) Beate Heinemann, University of Liverpool Introduction Final LEP Results First Tevatron Run 2 Results Summary and Outlook IDM 2004, Edinburgh, September 2004 Why
More informationSearches for SUSY in Final States with Photons
SUSY4: The nd International Conference on Supersymmetry and Unification of Fundamental Interactions" -6 July 4, Manchester, England" Searches for SUSY in Final States with Photons On Behalf of the CMS
More informationCollider Physics Analysis Procedures
Collider Physics Analysis Procedures Alex Tapper Slides available at: http://www.hep.ph.ic.ac.uk/~tapper/lecture.html Aim Overview of analysis techniques at CMS Contrast with Tevatron (see DØ lecture)
More informationPreparations for SUSY searches at the LHC
Preparations for SUSY searches at the LHC Alex Tapper UK HEP Forum: LHC First Results and Outlook, September 20-21 20. Outline Search strategy Examples with 70 nb -1 Hadronic searches Leptonic searches
More informationBeyond the SM: SUSY. Marina Cobal University of Udine
Beyond the SM: SUSY Marina Cobal University of Udine Why the SM is not enough The gauge hierarchy problem Characteristic energy of the SM: M W ~100 GeV Characteristic energy scale of gravity: M P ~ 10
More informationSUSY & Non SM Higgs Searches
SUSY & Non SM Higgs Searches Mario Martínez-Pérez (IFAE-Barcelona) Outline SUSY Squark/Gluino Searches Search for Chargino/Neutralino GMSB Scenario Non SM Higgs Searches Bs->μμ vs MSSM SUSY @ the LHC Final
More informationSearch for Supersymmetry at CMS in all-hadronic final states
Search for Supersymmetry at CMS in all-hadronic final states The 9th Particles and Nuclei International Conference, MIT Matthias Schröder (Universität Hamburg) on behalf of the CMS Collaboration 5 July
More informationCMS Searches for SUSY in Final States with Taus. Alfredo Gurrola (Vanderbilt) on behalf of the CMS Collaboration
CMS Searches for SUSY in Final States with Taus Alfredo Gurrola (Vanderbilt) on behalf of the CMS Collaboration Why SUSY with Taus? 2 Theoretical motivation ( Naturalness ) SUSY can cancel top loop corrections
More informationPreparations for SUSY searches at the LHC
Preparations for SUSY searches at the LHC Alex Tapper UK HEP Forum: LHC First Results and Outlook, September 20-21 20. Outline Search strategy Examples with 70 nb Hadronic searches Leptonic searches (single
More informationFirst physics with the ATLAS and CMS experiments. Niels van Eldik on behalf of the ATLAS and CMS collaborations
First physics with the ATLAS and CMS experiments Niels van Eldik on behalf of the ATLAS and CMS collaborations Content Status of the LHC and the ATLAS and CMS experiments Event production rates First physics
More informationCMS. Saeid Paktinat. On behalf of the CMS Collaborations. (IPM, Tehran)
SUSY @ CMS (IPM, Tehran) On behalf of the CMS Collaborations outline SUSY Common Signatures Some Examples Conclusion 2 Why SUperSYmmetry(1) SM describes a lot of experimental results very precisely, but
More informationSUSY searches at LHC and HL-LHC perspectives
SUSY searches at LHC and HL-LHC perspectives Maximilian Goblirsch-Kolb, on behalf of the ATLAS and CMS collaborations 26.10.2017, LCWS 2017, Strasbourg SUSY particle production in p-p collisions Two main
More informationEarly SUSY searches at the LHC
Early SUSY searches at the LHC Alex Tapper Searching for SUSY at the LHC and interplay with astroparticle physics Institute of Physics Workshop, 24 th March 20, Imperial College London Introduction Many
More informationICHEP 2008 Philadelphia
ICHEP 2008 Philadelphia LHC CERN Geneva 2008 Sascha Caron Standard SUSY at LHC 2 Almost all LHC sectors are cooled down (2 sectors at this moment at 20-30K) Start at s = 10 TeV in 2008 2008 Luminosity
More informationApproaching SUSY searches at CMS. Frédéric Ronga (ETH Zurich) LPHE seminar November 15, 2010
Approaching SUSY searches at CMS Frédéric Ronga (ETH Zurich) LPHE seminar November 15, 20 Outline SUSY: what and why? The Compact Muon Solenoid SUSY searches at CMS Prospects F. Ronga (ETH Zurich) LPHE
More informationRecent Results on New Phenomena and Higgs Searches at DZERO
Recent Results on New Phenomena and Higgs Searches at DZERO Neeti Parashar Louisiana Tech University Ruston, Louisiana U.S.A. 1 Outline Motivation for DØ Run II Detector at Fermilab The Fermilab Tevatron
More information7 Results 7.1 Results for the inclusive-mt2 analysis 7.2 Results for the MT2 Higgs analysis
Published for SISSA by Springer Received: February 15, 2015 Accepted: April 17, 2015 Published: May 15, 2015 Searches for supersymmetry using the MT2 variable in hadronic events produced in pp collisions
More informationSearch for long-lived particles at CMS
Search for long-lived particles at CMS Jie Chen Florida State University for the CMS Collaboration 03/19/12 Jie Chen @ SEARCH12 1 Outline Brief introduction to long-lived particle Neutral long-lived particles
More informationCarlos Sandoval Universidad Antonio Nariño On behalf of the ATLAS collaboration DIS Kobe, Japan
Carlos Sandoval Universidad Antonio Nariño On behalf of the ATLAS collaboration DIS 2018 - Kobe, Japan 1 Search for long-lived massive particles (LLP) in events with displaced vertices (DV): arxiv:1710.04901v1
More informationSUSY Search Strategies at Atlas and CMS
1 SUSY Search Strategies at Atlas and CMS (Universität Hamburg) for the Atlas and CMS Collaborations All-hadronic SUSY search Leptonic Inclusive SUSY search Reach in the msugra plane supported by: SUSY
More informationFirst V+jets results with CMS. Vitaliano Ciulli (Univ. & INFN Firenze) V+jets workshop, 8-10 Sep 2010, Durham
First V+jets results with CMS Vitaliano Ciulli (Univ. & INFN Firenze) V+jets workshop, 8- Sep 20, Durham Outline Jet and missing energy reconstruction W and Z selections and cross-section measurement First
More informationEarly SUSY searches at the LHC
on behalf of the ATLAS and CMS Collaborations Imperial College London E-mail: a.tapper@imperial.ac.uk Supersymmetry may give rise to striking events that could be discovered early in LHC running. Search
More informationLHC signals for SUSY discovery and measurements
06 March 2009 ATL-PHYS-SLIDE-2009-038 LHC signals for SUSY discovery and measurements Vasiliki A. Mitsou (for the ATLAS and CMS Collaborations) IFIC Valencia PROMETEO I: LHC physics and cosmology 2-6 March,
More informationATLAS-CONF October 15, 2010
ATLAS-CONF-2010-096 October 15, 2010 Data-driven background estimation for the H τ + τ τ h search at 7 TeV with the ATLAS detector Ian Howley 7 December 2010 1 Motivation One of the primary LHC physics
More informationSUSY Search at CMS. Jet+MET+0 lepton analysis Jet+MET+leptons analysis MET independent analysis Conclusions
SUSY Search at CMS Jet+MET+0 lepton analysis Jet+MET+leptons analysis MET independent analysis Conclusions Anwar A Bhatti The Rockefeller University On behalf of CMS Collaboration LHC Dark Matter Workshop
More informationEarly physics with Atlas at LHC
Early physics with Atlas at LHC Bellisario Esposito (INFN-Frascati) On behalf of the Atlas Collaboration Outline Atlas Experiment Physics goals Next LHC run conditions Physics processes observable with
More informationReview of ATLAS experimental results (II)
Review of ATLAS experimental results (II) Rachid Mazini Academia Sinica Taiwan CTEQ 2012 summer school Lima, Peru 30 July -8 August Rachid Mazini, Academia Sinica 1 Outline part II Higgs searches H, H
More informationSearch for top squark pair production and decay in four bodies, with two leptons in the final state, at the ATLAS Experiment with LHC Run2 data
Search for top squark pair production and decay in four bodies, with two leptons in the final state, at the ATLAS Experiment with LHC Run data Marilea Reale INFN Lecce and Università del Salento (IT) E-mail:
More informationSUSY Experimental Results from CMS and ATLAS
SUSY Experimental Results from CMS and ATLAS Kenichi Hatakeyama Baylor University Review of Discovery Physics Results from ICHEP Argonne National Laboratory July 17, 2012 Why SUSY Now? Three very compelling
More informationarxiv: v1 [hep-ex] 8 Nov 2010
Searches for Physics Beyond the Standard Model at CMS Sung-Won Lee, on behalf of the CMS Collaboration Texas Tech University, Lubbock, TX 799, USA Recent results on searches for physics beyond the Standard
More informationStatus of ATLAS+CMS SUSY searches
Status of ATLAS+CMS SUSY searches Renaud Brunelière Uni. Freiburg ~ ~ pp b b1 X candidate 2 b-tagged jets pt ~ 152 GeV and 96 GeV E miss T ~ 205 GeV, M CT (bb) ~ 201 GeV Status of ATLAS+CMS SUSY searches
More informationSearches for new physics at ATLAS
1 Searches for new physics at ATLAS Gökhan Ünel U.C. Irvine On behalf of the ATLAS collaboration ICPP 2011 Istanbul Outline 2 LHC has been giving us data at ever increasing pace. Lint =1 fb reached as
More informationSearching for Supersymmetry at the LHC David Stuart, University of California, Santa Barbara. CMS SUSY Search, D. Stuart, June 2011, Lisbon!
Searching for Supersymmetry at the LHC David Stuart, University of California, Santa Barbara CMS SUSY Search, D. Stuart, June 2011, Lisbon! 1! Searching for Supersymmetry at the LHC David Stuart, University
More informationSearch for the Standard Model Higgs Boson in H WW lν lν with the ATLAS experiment
Search for the Standard Model Higgs Boson in H WW lν lν with the ATLAS experiment MCTP Symposium 2012, University of Michigan, Ann Arbor, US Outline SM Higgs Boson production and decay Analysis based on
More informationNew physics at the LHC
New physics at the LHC Giacomo Polesello INFN Sezione di Pavia Motivations for going beyond Standard Model Observations unexplained by SM Dark matter problem Matter-antimatter asymmetry problem Fine-tuning
More informationHiggs Boson in Lepton Decay Modes at the CMS Experiment
Higgs Boson in Lepton Decay Modes at the Experiment Somnath Choudhury 1 for the collaboration 1 DESY - Hamburg, Germany DOI: http://dx.doi.org/1.34/desy-proc-14-4/1 The results on the standard model Higgs
More informationLHC Results in Majid Hashemi IPM, Tehran Wednesday, 11 th May 2011
LHC Results in 2010-11 Majid Hashemi IPM, Tehran Wednesday, 11 th May 2011 1 LHC results after a year of successful data taking Majid Hashemi IPM, 18th May 2011 http://cms.web.cern.ch/cms/timeline/index.html
More informationHiggs and New Physics at ATLAS and CMS
Higgs and New Physics at ATLAS and CMS F. Malek, LPSC-Grenoble for the ATLAS and CMS Collaborations 56th International Winter Meeting on Nuclear Physics 22-26 January 2018, Bormio-Italy ATLAS and CMS experiments
More informationSEARCH FOR PHYSICS BEYOND STANDARD MODEL AT THE LHC. Daniele del Re Sapienza Università & INFN Sezione Roma
SEARCH FOR PHYSICS BEYOND STANDARD MODEL AT THE LHC Daniele del Re Sapienza Università & INFN Sezione Roma WHY BSM Several open issues implying Physics beyond Standard Model. Some examples: 1. Why only
More informationPhysics at the TeV Scale Discovery Prospects Using the ATLAS Detector at the LHC
Physics at the TeV Scale Discovery Prospects Using the ATLAS Detector at the LHC Peter Krieger Carleton University Physics Motivations Experimental Theoretical New particles searches Standard Model Higgs
More informationCMS Searches for SUSY in Hadronic Final States
CMS Searches for SUSY in Hadronic Final States Teruki Kamon on behalf of the CMS Collaboration Mitchell Institute for Fundamental Physics and Astronomy Texas A&M University JnHF 2018: Santa Fe Jets and
More informationPhysics at the Tevatron. Lecture IV
Physics at the Tevatron Lecture IV Beate Heinemann University of California, Berkeley Lawrence Berkeley National Laboratory CERN, Academic Training Lectures, November 2007 1 Outline Lecture I: The Tevatron,
More informationOverall CMS SUSY search strategy
GGI workshop Overall CMS SUSY search strategy Filip Moortgat (ETH Zurich) Florence, October 22, 2012 GGI workshop 2012 Filip Moortgat (ETH Zurich) 1 Outline Strategy for the first data Assume pair production
More informationSearch for Displaced Supersymmetry using the Compact Muon Solenoid Detector
Search for Displaced Supersymmetry using the Compact Muon Solenoid Detector L. Antonelli, F. Blekman, A. Hart, N. Heracleous, C. Hill, B. Liu, and Q. Python for the CMS Collaboration 1 Outline Motivation!
More informationMono-X, Associate Production, and Dijet searches at the LHC
Mono-X, Associate Production, and Dijet searches at the LHC Emily (Millie) McDonald, The University of Melbourne CAASTRO-CoEPP Joint Workshop Melbourne, Australia Jan. 30 - Feb. 1 2017 M. McDonald, University
More informationDark matter searches and prospects at the ATLAS experiment
Dark matter searches and prospects at the ATLAS experiment Wendy Taylor (York University) for the ATLAS Collaboration TeVPA 2017 Columbus, Ohio, USA August 7-11, 2017 Dark Matter at ATLAS Use 13 TeV proton-proton
More informationLong lived particle decay LHC. Simone Gennai on behalf of the ATLAS, CMS and LHCb Collaborations
Long lived particle decay searches @ LHC Simone Gennai on behalf of the ATLAS, CMS and LHCb Collaborations 1 Why searching for LLP? 2 Standard Model includes quite few LLP it is natural to assume they
More informationSearch for a heavy gauge boson W e
Search for a heavy gauge boson W e Cornell University LEPP Journal Club Seminar April 1, 2011 The LHC Machine 2 The beginning of the LHC era First collisions at 7 TeV confirmed on March 30, 2010 There
More informationTop Quark Physics at the LHC
Top Quark Physics at the LHC Ayana Arce HEP 0 Lectures #7 March 4, 203 Outline Introduction 2 Why are top quarks interesting? 3 Creating Top Quarks 4 Identifying Top Quarks 5 Some LHC results 6 Beyond
More informationSupersymmetry after LHC Run 1. Brian Petersen CERN
Supersymmetry after LHC Run 1 Brian Petersen CERN Outline Supersymmetry What and why? Searching for Supersymmetry at the LHC Brief intro to LHC and the ATLAS experiment and how we search for Supersymmetry
More informationSearch for long-lived particles at CMS. TeVPA Brian Francis for the CMS Collaboration
Search for long-lived particles at CMS TeVPA 7 Brian Francis for the CMS Collaboration Long-lived particles (LLP) at CMS Despite best efforts, no evidence yet of BSM physics at the LHC If it s not where
More informationSearch for exotic Higgs-boson decays in events with at least one photon, missing transverse momentum,
in events with at least one photon, missing transverse momentum, and two forward jets produced in s = 8 ev pp collisions with the ALAS detector on behalf of the ALAS Collaboration New York University E-mail:
More informationA search for heavy and long-lived staus in the LHCb detector at s = 7 and 8 TeV
A search for heavy and long-lived staus in the LHCb detector at s = 7 and 8 TeV Trần Minh Tâm minh-tam.tran@epfl.ch on behalf of the LHCb Collaboration LHCb-CONF-2014-001 EPFL, Laboratoire de Physique
More informationDiscovery potential for SUGRA/SUSY at CMS
Discovery potential for SUGRA/SUSY at CMS Stefano Villa, Université de Lausanne, April 14, 2003 (Based on talk given at SUGRA20, Boston, March 17-21, 2003) Many thanks to: Massimiliano Chiorboli, Filip
More informationSearches for Beyond SM Physics with ATLAS and CMS
Searches for Beyond SM Physics with ATLAS and CMS (University of Liverpool) on behalf of the ATLAS and CMS collaborations 1 Why beyond SM? In 2012 the Standard Model of Particle Physics (SM) particle content
More informationSearches Beyond the Standard Model at the LHC. Yuri Gershtein
Searches Beyond the Standard Model at the LHC Yuri Gershtein There Must Be New Physics! Explain low mass of Higgs (hierarchy problem) Explain Dark Matter why shouldn t it be produced at colliders? Explain
More informationWhat the LHC Will Teach Us About Low Energy Supersymmetry
What the LHC Will Teach Us About Low Energy Supersymmetry Darin Acosta representing ATLAS & Outline Introduction to SUSY, LHC, and the Detectors Trigger strategies at start-up Inclusive squark/gluino searches
More informationThe HL-LHC physics program
2013/12/16 Workshop on Future High Energy Circular Collider 1 The HL-LHC physics program Takanori Kono (KEK/Ochanomizu University) for the ATLAS & CMS Collaborations Workshop on Future High Energy Circular
More informationProbing Dark Matter at the LHC Alex Tapper
Probing Dark Matter at the LHC Alex Tapper 1 Outline The LHC and ATLAS and CMS detectors Detector performance and Standard Model physics Status of Dark Matter searches at the LHC MET based searches Long-lived
More informationFrontiers in Theoretical and Applied Physics 2017, Sharjah UAE
A Search for Beyond the Standard Model Physics Using Final State with Light and Boosted Muon Pairs at CMS Experiment Frontiers in Theoretical and Applied Physics 2017, Sharjah UAE Alfredo Castaneda* On
More informationMaster Thesis Topics 2013/14 in Experimental Particle Physics
July 2, 23 Master Thesis Topics 23/4 in Experimental Particle Physics at LS Schaile At LS Schaile we offer a broad spectrum of master thesis topics in experimental elementary particle physics. Contacts:
More informationOn behalf of the ATLAS and CMS Collaborations
On behalf of the ATLAS and CMS Collaborations Reza Goldouzian Université libre de Bruxelles 1 Ø There are several models of physics beyond the standard model require new particles that couple to quarks
More informationInclusive SUSY Searches at CMS with Emphasis on Detector Systematics
Inclusive SUSY Searches at with Emphasis on Detector Systematics R. Cavanaugh (on behalf of ) University of Florida SUSY06 Detector Background Calibrations Inclusive Search Strategies Detector Systematics
More informationW/Z + jets and W/Z + heavy flavor production at the LHC
W/Z + jets and W/Z + heavy flavor production at the LHC A. Paramonov (ANL) on behalf of the ATLAS and CMS collaborations Moriond QCD 2012 Motivation for studies of jets produced with a W or Z boson Standard
More informationLHC State of the Art and News
LHC State of the Art and News ATL-GEN-SLIDE-2010-139 16 June 2010 Arno Straessner TU Dresden on behalf of the ATLAS Collaboration FSP 101 ATLAS Vulcano Workshop 2010 Frontier Objects in Astrophysics and
More informationLecture 4 - Beyond the Standard Model (SUSY)
Lecture 4 - Beyond the Standard Model (SUSY) Christopher S. Hill University of Bristol Warwick Flavour ++ Week April 11-15, 2008 Recall the Hierarchy Problem In order to avoid the significant finetuning
More informationStrategy for early SUSY searches at ATLAS
SUSY07 The 15th International Conference on Supersymmetry and the Unification of Fundamental Interactions Karlsruhe, Germany Strategy for early SUSY searches at ATLAS July 26, 2007 Shimpei Yamamoto (ICEPP,
More informationSearch for SUperSYmmetry SUSY
PART 3 Search for SUperSYmmetry SUSY SUPERSYMMETRY Symmetry between fermions (matter) and bosons (forces) for each particle p with spin s, there exists a SUSY partner p~ with spin s-1/2. q ~ g (s=1)
More informationSearch for supersymmetric phenomena at LHC with the CMS detector
Search for supersymmetric phenomena at LHC with the CMS detector Michele Pioppi Imperial College London 6 April 2011 Rutherford Appleton Laboratory Outline Why Supersymmetry @ LHC Why you should believe
More informationMeasurement of Jet Energy Scale and Resolution at ATLAS and CMS at s = 8 TeV
Measurement of Jet Energy Scale and Resolution at ATLAS and CMS at s = 8 TeV EDSBlois 2015 02.07.2015 Dominik Haitz on behalf of the ATLAS and CMS Collaborations INSTITUT FÜR EXPERIMENTELLE KERNPHYSIK
More informationLecture 18 - Beyond the Standard Model
Lecture 18 - Beyond the Standard Model Why is the Standard Model incomplete? Grand Unification Baryon and Lepton Number Violation More Higgs Bosons? Supersymmetry (SUSY) Experimental signatures for SUSY
More informationIdentification of the Higgs boson produced in association with top quark pairs in proton-proton
Identification of the Higgs boson produced in association with top quark pairs in proton-proton collision: an analysis of the final state containing three leptons with the ATLAS detector Valentina Vecchio,
More informationR-hadrons and Highly Ionising Particles: Searches and Prospects
R-hadrons and Highly Ionising Particles: Searches and Prospects David Milstead Stockholm University The need for new particles Why they could be heavy and stable How can we identify them in current and
More informationThe Compact Muon Solenoid Experiment. Conference Report. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland
Available on CMS information server CMS CR -207/27 The Compact Muon Solenoid Experiment Conference Report Mailing address: CMS CERN, CH2 GENEVA 23, Switzerland 05 May 207 (v3, May 207) Search for unconventional
More informationPoS(Kruger 2010)034. CMS searches for new physics. Mara Senghi Soares On behalf of the CMS Collaboration.
On behalf of the CMS Collaboration E-mail: mara.senghi@ciemat.es We discuss the first searches for new physics being carried out with the CMS detector, at the early stage of data taking. Prospects for
More informationarxiv:hep-ph/ v1 17 Apr 2000
SEARCH FOR NEW PHYSICS WITH ATLAS AT THE LHC arxiv:hep-ph/0004161v1 17 Apr 2000 V.A. MITSOU CERN, EP Division, CH-1211 Geneva 23, Switzerland and University of Athens, Physics Department, Nuclear and Particle
More informationExotics Searches for New Physics with the ATLAS Detector
Exotics Searches for New Physics with the ATLAS Detector Jalal Abdallah IFAE Barcelona on behalf of ATLAS Collaboration 19th Particles & Nuclei International Conference 24-29 July 2011 Outline New results
More informationQCD Jets at the LHC. Leonard Apanasevich University of Illinois at Chicago. on behalf of the ATLAS and CMS collaborations
QCD Jets at the LHC Leonard Apanasevich University of Illinois at Chicago on behalf of the ATLAS and CMS collaborations Outline Physics at the LHC Jet Reconstruction and Performance Clustering Algorithms
More information