Discovery potential for SUGRA/SUSY at CMS
|
|
- Nathaniel Ross
- 5 years ago
- Views:
Transcription
1 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 Moortgat, Salavat Abdullin, Daniel Denegri April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 1
2 Contents SUSY in a nutshell LHC and CMS. Getting the right events: SUSY triggers in CMS: - Low luminosity - High luminosity Inclusive SUSY studies (msugra) SUSY Higgs SUSY Spectroscopy: - Point B, 10 fb -1 - Point B, 300 fb -1 - Point G, 300 fb -1 Conclusion April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 2
3 Why SUSY? Try to fix some problems in the Standard Model: - hierarchy (Weak-GUT-Planck) - naturalness (need fine tuning to keep scalar masses small) - no gravity Get some positive side effects: - unification of couplings - SUSY is there basically in all extensions of the SM which include gravity April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 3
4 SUSY in a nutshell A symmetry which relates fermions and bosons would solve the naturalness problem: SUSY Bosons Fermions: same number of deg. of freedom in each supermultiplet Fermions Sfermions (squarks, selectrons ) Bosons -inos (gluinos, higgsinos, gauginos ) CLEARLY, SUSY is broken! sparticles should have the same mass as their partners we do not see them. April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 4
5 SUSY in a nutshell Minimal SUSY extension of the SM is MSSM - 2 Higgs doublets. >100 parameters (too many) - introduce constrained MSSM. Parameters: m 1/2 : common gaugino mass at GUT scale m 0 : common scalar mass at GUT scale m A : pseudoscalar Higgs mass tanβ : ratio of vev of the two Higgs doublets µ : Higgs mixing parameter A t,b,τ : stop, sbottom, stau mixing parameters April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 5
6 SUSY in a nutshell Add more assumptions (SUSY breaking communicated by gravitation) minimal supergravity (msugra). only 5 parameters: m 1/2, m 0, tanβ, sign(µ (µ), A 0 One more variable in the game: R-parity: P R = (-1) 3(B-L)+2s P R = +1 for standard particles P R = -1 for sparticles If R-parity conserved the lightest sparticle is stable (LSP, a good candidate for dark matter) and sparticles are always produced in even numbers. April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 6
7 The LHC machine. pp collisions at 14 TeV center of mass energy scheduled to start in April 2007 luminosity cm -2 s -1 (initially 2x10 33 cm -2 s -1 ) 20 interactions per beam crossing at 40 MHz rate σ(pp) 70 mb H 4µ event plus 20 min. bias: quite crowded April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 7
8 The CMS detector General purpose detector: main aims: Higgs, SUSY or other New Physics in the TeV range for SUSY, need - good jet and missing E T resolution - hermetic calorimeters - efficient b-tagging and τ identification - precise lepton and jet energy scales April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 8
9 Typical SUSY event squark-gluino production Signature: - many high P T jets - missing E T - (leptons) April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 9
10 SUSY triggers April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 10
11 SUSY triggers Problem: select interesting events with the highest efficiency at an affordable rate. Studies performed at Low luminosity = cm -2 s -1 High luminosity = cm -2 s -1 at 3+3 msugra benchmark points. look also at R-parity violation All results obtained with GEANT + full reconstruction software. CMS Data Acquisition & High Level Trigger Technical Design Report just published (CERN/LHCC ) April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 11
12 Low luminosity trigger Just above Tevatron II reach Along M squark 400 GeV curve April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 12
13 Low luminosity trigger Consider jets and missing E T ; combine 2 selections: msugra 1 jet > 180 GeV 4 jets, E T >113 GeV miss point: > 123 GeV E T R-viol. Signal efficiency w.r.t. L1 (%) R 5R 6R (11) (14) (16) (28) (30) 9 26 (20) High Level Trigger efficiency Background (6.8) rate (Hz) Trigger efficiency still very good in R-violating case April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 13
14 High luminosity trigger Explore higher mass scale ( 2 TeV), R-parity viol. as well Low luminosity points April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 14
15 R-parity violating event Expect less missing E T : still some remains (lots of b, W/Z, τ, neutrinos) Additional jets April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 15
16 N jet and missing E T R-parity conserved E jet > 50 GeV T R-parity violated April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 16
17 High luminosity trigger results Very simple cuts do the job... miss msugra E > 239 GeV 4 jets, E T T >185 GeV point: R-viol. Signal efficiency w.r.t. L1 (%) R 8R 9R (18) (28) (28) (75) (78) (52) High Level Trigger efficiency Background (1.5) rate (Hz) Efficiency quite high, also in the R-parity violating case. April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 17
18 Inclusive SUSY searches April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 18
19 Inclusive SUSY searches Need to reduce the number of parameters msugra Final states investigated: E T E T E T E T E T E T miss miss miss miss miss miss + jets + jets + no leptons + jets + 1 lepton + jets + 2 OS leptons + jets + 2 SS leptons + jets + 3 leptons Strategy: look for signal (ISAJET) excess over SM (PYTHIA) background in the chosen final states detector response: fast simulation (CMSJET) explore reach in the (m 0, m 1/2 ) msugra plane Try a few tanβ values DISCOVERY defined as N signal (N signal + N bgd ) 1/2 5 April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 19
20 CMS reach on msugra mass plane 100 fb -1 ; A 0 = 0 tanβ = 2, µ > fb -1 ; A 0 = 0 tanβ = 35, µ < 0 April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 20
21 CMS reach on msugra mass plane A 0 =0, tanβ=35, µ>0 Final integ. luminosity One year at high lumi One year at low lumi One month at low lumi Final reach for squark and gluino mass: TeV valid in the bulk of the parameters space; possible exceptions depend on mass hierarchy little dependence on sign(µ) missing E T signature gives the best reach April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 21
22 , reach in the MSSM: q% %g Similar study on other (non msugra) sets of parameters: April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 22
23 SUSY Higgs April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 23
24 MSSM Higgs Discovery reach for MSSM Higgs bosons: Look for the heavy Higgs in low/intermediate tanβ region, where only h can be discovered through SM decays. Two strategies: 1. Chargino and neutralino decays of A, H, H m 2. h,a,h bb in SUSY cascades April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 24
25 Neutralino and chargino decays A, H χ~ 0 2 χ~ 0 2 4l m If neutralinos are light enough: H m χ~ 0 ~ m 2,3 χ 1,2 3l m + X Main backgrounds: ttx and SUSY cascades mainly produced via gb th m try to reconstruct associated top Main backgrounds: SUSY+ZZ April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 25
26 Higgs in SUSY cascades Several scenarios analysed; choose (a good) one... Look for bb decays of neutral Higgs: N jets > 5 E T hardest jet > 300 GeV miss E T > 150 GeV miss M eff = Σ E T + E T > 1200 GeV 2 b-tagged jets April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 26
27 Mass reach of h bb in cascades 2 msugra scenarios: - April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 27
28 SUSY spectroscopy April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 28
29 Post-LEP benchmark points More points in msugra space, chosen to perform full sparticle reconstruction Cosmologically interesting region CMS Studied B and G in detail April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 29
30 Sparticles spectrum (GeV) Point B with 10 fb -1 Start with gluino-sbottom decay chain; expect: 2 SFOS isolated leptons 2 b-jets missing E T April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 30
31 Step 1: dilepton mass 2-body decay: edge in M ll B 10 fb -1 April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 31
32 Step 2: fit the edge B Subtract OFOS lepton pairs: reduce background Generated value: M max ll = GeV April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 32
33 Step 3: sbottom reconstruction B 0 Assume M( χ~ 1) known For evts in the edge: 65 GeV < M < 81 GeV ll combine with most energetic b-jet Fit result: ~ ~ Generated: M(b L )=496 GeV; M(b R )=524 GeV April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 33
34 Step 4: gluino reconstruction B ~ Combine b to the closest b-jet b-tag parameter Generated value: M( g~ ) = GeV April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 34
35 Non-b squark reconstruction ~ Now look at : u~, d, ~ c, s~ Look for non-b jets; expect more combinatorial background B April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 35
36 Non-b squark reconstruction Repeat same procedure as for sbottom: 1,2. dilepton inv. mass: SM B 3. Using evts. in the edge, form squark invariant mass. Apply b-veto: no jets in event with σ>3 Fit result: Generated: April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 36
37 Gluino reconstruction 4. Combine reconst. squark to nearest jet. B Fit result: Apply upper cut on the 2nd jet energy to reduce combinatorics due to jets coming from squarks. Generated value: M( g~ ) = GeV 10 fb -1 April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 37
38 Gluino-sbottom at 300 fb -1 Analysis repeated, with cuts reoptimised, to get resolutions below the 10 % level: B sbottom gluino April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 38
39 Point G with 300 fb -1 Heavier sparticles (M ~ g 900 GeV, M ~ b 750 GeV M q ~ 800 GeV ) lower SUSY cross section (6 pb) ~ Higher tanβ : larger χ 0 τ + τ ~ χ branching ratio, lower l + l - signal 300 fb -1 SM Need high statistics to reconstruct invariant mass peaks. miss E T > 250 GeV April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 39
40 Gluino-squark reconstruction squark gluino G Fit result ~ M(d L )=M(s ~ L )=778.0 GeV generated M(g)=860.8 ~ GeV M(u ~ L )=M(c ~ L )=773.9 GeV April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 40
41 miss Conclusion SUSY (jets+e T ) triggers in CMS: first GEANT + full reconstruction study. Good efficiency both at low and high lumi (mass), even with R-parity violation. Inclusive CMS SUSY reach, quite indep. of the choice of parms.: TeV for ~ q and g ~ (300 fb -1 ). MSSM heavy Higgs bosons decaying in charginos and neutralinos: extend the reach in the low tanβ part of the tanβ-m A plane. Full analysis of msugra points B and G show good resolution (below 10%) on M~ b, M q ~, M g ~, already with 10 fb -1 at p.b (300 fb -1 at p.g). April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 41
42 CMS reach on msugra mass plane Systematic studies Signal +/- 30% Background +100% / -50% April 14, 2003 Stefano Villa Discovery potential for SUGRA/SUSY at CMS 42
Supersymmetry at the LHC: Searches, Discovery Windows, and Expected Signatures
Supersymmetry at the LHC: Searches, Discovery Windows, and Expected Signatures Darin Acosta representing ATLAS & Outline Introduction to SUSY, LHC, and the Detectors Non-Higgs sparticle searches: Trigger
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 informationS.Abdullin ITEP. July 8, 2003 S.Abdullin (UMD) LHC SUSY Potential 1
S.Abdullin ITEP July 8, 2003 S.Abdullin (UMD) LHC SUSY Potential 1 Outline LHC and the Detectors SUSY : MSSM, msugra SUSY signatures Triggering on SUSY Inclusive SUSY searches SUSY spectroscopy Summary
More informationarxiv:hep-ex/ v1 30 Sep 1997
CMS CR 997/0 SEARCHES FOR SUSY AT LHC arxiv:hep-ex/970903v 30 Sep 997 For the CMS Collaboration Avtandyl Kharchilava Institute of Physics, Georgian Academy of Sciences, Tbilisi ABSTRACT One of the main
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 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 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 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 informationCosmology at the LHC
Cosmology at the LHC R. Arnowitt*, A. Aurisano*^, B. Dutta*, T. Kamon*, N. Kolev**, P. Simeon*^^, D. Toback*, P. Wagner*^ *Department of Physics, Texas A&M University **Department of Physics, Regina University
More informationLHC Capability for Dark Matter
LHC Capability for Dark atter 5// Bhaskar Dutta Texas A& University Discovery Time We are about to enter into an era of major discovery Dark atter: we need new particles to explain the content of the universe
More informationA Simulated Study Of The Potential For The Discovery of the Supersymmetric Sbottom Squark at the ATLAS Experiment
A Simulated Study Of The Potential For The Discovery of the Supersymmetric Sbottom Squark at the ATLAS Experiment By Rishiraj Pravahan University of Texas at Arlington Outline Why do we need Supersymmetry?
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 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 informationP. Sphicas/SSI2001. Standard Model Higgs
Standard Model Higgs SM Higgs (I) Production mechanisms & cross section Studying EWSB at the LHC 2 Decays & discovery channels Higgs couples to m f 2 SM Higgs (II) Heaviest available fermion (b quark)
More informationSUSY Models, Dark Matter and the LHC. Bhaskar Dutta Texas A&M University
SUSY odels, Dark atter and the LHC Bhaskar Dutta Texas A& University 11/7/11 Bethe Forum 11 1 Discovery Time We are about to enter into an era of major discovery Dark atter: we need new particles to explain
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 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 informationHiggs Signals and Implications for MSSM
Higgs Signals and Implications for MSSM Shaaban Khalil Center for Theoretical Physics Zewail City of Science and Technology SM Higgs at the LHC In the SM there is a single neutral Higgs boson, a weak isospin
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 informationMeasuring Relic Density at the LHC
easuring Relic Density at the LHC Bhaskar Dutta Collaborators R. Arnowitt, A. Gurrola, T. Kamon, A. Krislock, D. Toback Texas A& University 7 th July 8 easuring Relic Density at the LHC OUTLINE Dark atter
More informationLHC and Dark Matter 07/23/10. Bhaskar Dutta Texas A&M University
LHC and Dark atter 7/3/ Bhaskar Dutta Texas A& University Discovery Time We are about to enter into an era of major discovery Dark atter: we need new particles to explain the content of the universe Standard
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 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 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 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 informationDetermination of Non-Universal Supergravity Models at the LHC
Determination of Non-Universal Supergravity Models at the LHC B. Dutta 1, T. Kamon 1, 2, 3, N. Kolev 4, *, A. Krislock 1, Y. Oh 3 1 Texas A&M U., 2 Fermilab, 3 Kyungpook National U., 4 U. of Regina * kolev20n@uregina.ca
More informationProbing SUSY Dark Matter at the LHC
Probing SUSY Dark Matter at the LHC Kechen Wang Mitchell Institute for Fundamental Physics and Astronomy Texas A&M University Preliminary Examination, Feb, 24 OUTLINE Supersymmetry dark matter (DM) Relic
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 THE NEUTRAL HIGGS BOSONS OF THE MSSM
SEARCHES FOR THE NEUTRAL HIGGS BOSONS OF THE MSSM USING LEP DATA Elizabeth Locci SPP/DAPNIA Saclay Representing LEP Collaborations 1 Outline LEP performance Theoretical framework Search for neutral Higgs
More informationSearch for supersymmetry with disappearing tracks and high energy loss at the CMS detector
Search for supersymmetry with disappearing tracks and high energy loss at the CMS detector Teresa Lenz in Collaboration with Loic Quertenmont, Christian Sander, Peter Schleper, Lukas Vanelderen International
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 informationSupersymmetry Without Prejudice at the LHC
Supersymmetry Without Prejudice at the LHC Conley, Gainer, JLH, Le, Rizzo arxiv:1005.asap J. Hewett, 10 09 Supersymmetry With or Without Prejudice? The Minimal Supersymmetric Standard Model has ~120 parameters
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 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 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 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 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 informationSUSY Searches at CMS in the Fully Hadronic Channel
SUSY Searches at CMS in the Fully Hadronic Channel Project B2 - Supersymmetry at the Large Hadron Collider Christian Autermann, Sergei Bobrovskyi, Ulla Gebbert, Kolja Kaschube, Friederike Nowak, Benedikt
More informationSearches at LEP. Ivo van Vulpen CERN. On behalf of the LEP collaborations. Moriond Electroweak 2004
Searches at LEP Moriond Electroweak 2004 Ivo van Vulpen CERN On behalf of the LEP collaborations LEP and the LEP data LEP: e + e - collider at s m Z (LEP1) and s = 130-209 GeV (LEP2) Most results (95%
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 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 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 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 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 informationSzuperszimmetria keresése az LHC-nál
Horváth Dezső: Szuperszimmetria keresése Debrecen, 2011.06.16 1. fólia p. 1/37 Szuperszimmetria keresése az LHC-nál ATOMKI-szeminárium, Debrecen, 2011.06.16 Horváth Dezső MTA KFKI RMKI, Budapest és MTA
More informationSearch for Supersymmetry at LHC
Horváth Dezső: SUSY Search at LHC PBAR-11, Matsue, 2011.11.29 p. 1/40 Search for Supersymmetry at LHC PBAR-11, Matsue, 2011.11.29 Dezső Horváth KFKI Research Institute for Particle and Nuclear Physics,
More informationSearch for R-parity violating Supersymmetry. III Phys. Inst. A, RWTH Aachen
R-parity violating Supersymmetry III Phys. Inst. A, RWTH Aachen Introduction to R-parity violating SUSY Three DØ searches via non-zero LLE (short and long lived LSP) and LQD couplings Perspectives for
More informationProbing the Connection Between Supersymmetry and Dark Matter
Probing the Connection Between Supersymmetry and Dark Matter Bhaskar Dutta Texas A&M University Physics Colloquium, OSU, March 30, 2006 March 30, 2006 Probing the Connection Between SUSY and Dark Matter
More informationDark Matter Experiments and Searches
Dark Matter Experiments and Searches R.J.Cashmore Principal Brasenose College,Oxford and Dept of Physics,Oxford R.Cashmore Dark Matter 3 1 Dark Matter at LHC R.Cashmore Dark Matter 3 2 Satellite view of
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 informationSUSY searches with ATLAS What did we learn with few fb -1?
SUSY searches with ATLAS What did we learn with few fb -? Iacopo Vivarelli Universität Freiburg I. Vivarelli - Marseille - 09 Feb 0 Wednesday, February 8, 0 Is the Standard Model enough? The Standard Model
More informationSearches for Natural SUSY with RPV. Andrey Katz. C. Brust, AK, R. Sundrum, Z. Han, AK, M. Son, B. Tweedie, 1210.XXXX. Harvard University
Searches for C. Brust, AK, R. Sundrum, 126.2353 Z. Han, AK, M. Son, B. Tweedie, 121.XXXX Harvard University Frontiers Beyond the Standard Model III, Minneapolis, October 13, 212 (Harvard) October, 13 1
More informationDetection of SUSY Signals in Stau-Neutralino
Detection of SUSY Signals in Stau-Neutralino Coannhilation at the LHC - Finger Print of CDM - R. Arnowitt, 1) A. Aurisano, 1)* B. Dutta, 1) T. Kamon, 1) V. Khotilovich, 1)* N. Kolev, ) P. Simeon, 1)**
More informationPhysics at the LHC: from Standard Model to new discoveries
Physics at the LHC: from Standard Model to new discoveries Kirill Melnikov University of Hawaii May 2006 Sendai, June 2006 Physics at the LHC: from Standard Model to new discoveries p. 1/22 Outline Standard
More informationTesting msugra and Extensions at the LHC
Testing msugra and Extensions at the LHC Bhaskar Dutta and Teruki Kamon Texas A& University BS 9, Northeastern University, Boston nd June 9 Discovery Time We are about to enter into an era of major discovery
More informationNatural SUSY and the LHC
Natural SUSY and the LHC Clifford Cheung University of California, Berkeley Lawrence Berkeley National Lab N = 4 SYM @ 35 yrs I will address two questions in this talk. What is the LHC telling us about
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 informationSearch for Supersymmetry with the CMS - Detector
Search for Supersymmetry with the CMS - Detector Aachen 3a SUSY Group: Markus Merschmeyer, Arnd Meyer, Prof. Thomas Hebbeker, Holger Pieta, Daniel Teyssier 29. August 2007 Supersymmetry SUSY at CMS Computing,
More informationSupersymmetry at the LHC
Supersymmetry at the LHC Howard Baer Florida State University SUSY at LHC SUSY signatures SM backgrounds GEANT figure msugra : ~ g m 0 = 1000 GeV, m 1/2 = 500 GeV, A 0 = 0, ~ ul ~ t1 t - W + b ( jet4,
More informationSplit SUSY and the LHC
Split SUSY and the LHC Pietro Slavich LAPTH Annecy IFAE 2006, Pavia, April 19-21 Why Split Supersymmetry SUSY with light (scalar and fermionic) superpartners provides a technical solution to the electroweak
More informationSUPERSYMETRY FOR ASTROPHYSICISTS
Dark Matter: From the Cosmos to the Laboratory SUPERSYMETRY FOR ASTROPHYSICISTS Jonathan Feng University of California, Irvine 29 Jul 1 Aug 2007 SLAC Summer Institute 30 Jul 1 Aug 07 Feng 1 Graphic: N.
More informationLecture 03. The Standard Model of Particle Physics. Part III Extensions of the Standard Model
Lecture 03 The Standard Model of Particle Physics Part III Extensions of the Standard Model Where the SM Works Excellent description of 3 of the 4 fundamental forces Explains nuclear structure, quark confinement,
More informationSUSY searches at the LHC * and Dark Matter
SUSY searches at the LHC * and Dark Matter Elisabetta Barberio ATL-PHYS-SLIDE-2009-025 26 February 2009 School of Physics The University of Melbourne/Australia Dark 2009: Seventh International Heidelberg
More informationRecent searches for new particles using 13 TeV data with ATLAS at the LHC
Recent searches for new particles using 13 TeV data with ATLAS at the LHC Vivek Jain (on behalf of the ATLAS Collaboration) State University of New York, Albany MIAMI2015 Dec 19, 2015 Beyond the Standard
More informationSearch for Pair Production of Stop Quarks Mimicking Top Event Signatures
CDF/PUB/TOP/PUBLIC/9343 Search for Pair Production of Stop Quarks Mimicking Top Event Signatures The CDF Collaboration URL http://www-cdf.fnal.gov May 29, 2008 Abstract We present the search for the pair-produced
More informationDiscovery potential of toppartners in a realistic composite Higgs model with early LHC data
Discovery potential of toppartners in a realistic composite Higgs model with early LHC data Günther Dissertori, Elisabetta Furlan, Filip Moortgat, JHEP09(20)019 Kick-off Meeting Of The LHCPhenoNet Initial
More informationYukawa and Gauge-Yukawa Unification
Miami 2010, Florida Bartol Research Institute Department Physics and Astronomy University of Delaware, USA in collaboration with Ilia Gogoladze, Rizwan Khalid, Shabbar Raza, Adeel Ajaib, Tong Li and Kai
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 informationCMS 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 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 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 informationDetecting Higgs Bosons within Supersymmetric Models
Detecting Higgs Bosons within Supersymmetric Models Yili Wang University of Oklahoma C. Kao and Y. Wang, Phys. Lett. B 635, 3 (26) 1 Outlook of the Talk MSSM has two Higgs doulets. After symmetry reaking,
More informationMeasuring supersymmetry at the large hadron collider
PRAMANA cfl Indian Academy of Sciences Vol. 60, No. 2 journal of February 2003 physics pp. 239 247 Measuring supersymmetry at the large hadron collider BCALLANACH TH Division, CERN, Geneva 23, CH 1211,
More informationProbing Supersymmetric Connection with Dark Matter
From サイエンス 82 Probing Supersymmetric Connection with Dark Matter Taken from Science, 1982 Teruki Kamon Department of Physics Texas A&M University November 3, 2005 Physics Colloquium, Texas Tech University
More informationSearches for Physics Beyond the Standard Model at the Tevatron
FERMILAB-CONF-10-704-E-PPD Proceedings of the XXX. Physics in Collision Searches for Physics Beyond the Standard Model at the Tevatron Chris Hays 1 for the CDF and D0 Collaborations (1) Oxford University,
More informationKaluza-Klein Theories - basic idea. Fig. from B. Greene, 00
Kaluza-Klein Theories - basic idea Fig. from B. Greene, 00 Kaluza-Klein Theories - basic idea mued mass spectrum Figure 3.2: (Taken from [46]). The full spectrum of the UED model at the first KK level,
More informationSUSY Phenomenology & Experimental searches
SUSY Phenomenology & Experimental searches Slides available at: Alex Tapper http://www.hep.ph.ic.ac.uk/~tapper/lecture.html Objectives - Know what Supersymmetry (SUSY) is - Understand qualitatively the
More informationSUSY and Exotics. UK HEP Forum"From the Tevatron to the LHC, Cosener s House, May /05/2009 Steve King, UK HEP Forum '09, Abingdon 1
SUSY and Exotics Standard Model and the Origin of Mass Puzzles of Standard Model and Cosmology Bottom-up and top-down motivation Extra dimensions Supersymmetry - MSSM -NMSSM -E 6 SSM and its exotics UK
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 informationNeutralino spin measurement with ATLAS detector at LHC
Neutralino spin measurement with ATLAS detector at LHC M. Biglietti 1,2, I. Borjanovic 3, G. Carlino 2, F. Conventi 1,2, E. Gorini 3,4, A. Migliaccio 1,2, E. Musto 1,2, M. Primavera 3, S. Spagnolo 3,4,
More informationContributions by M. Peskin, E. Baltz, B. Sadoulet, T. Wizansky
Contributions by M. Peskin, E. Baltz, B. Sadoulet, T. Wizansky Dark Matter established as major component of the Universe: CMB determination of its relic density further confirmed by SNs and galaxy clusters;
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 informationEmerging the 7 TeV LHC & the LC
Emerging BSM @ the 7 TeV LHC & the LC T.G. Rizzo 03/16/11 THE QUESTIONS: How is electroweak symmetry broken? How is the hierarchy stabilized? What is the origin of flavor? Are there more than 4 dimensions?
More informationCMS Search for Supersymmetry at the LHC
CMS Search for Supersymmetry at the LHC [Credits] Images of Baryon Acoustic Bscillations with Cosmic Microwave Background by E.M. Huff, the SDSS-III team, and the South Pole Telescope team. Graphic by
More informationSupersymmetry Basics. J. Hewett SSI J. Hewett
Supersymmetry Basics J. Hewett SSI 2012 J. Hewett Basic SUSY References A Supersymmetry Primer, Steve Martin hep-ph/9709356 Theory and Phenomenology of Sparticles, Manual Drees, Rohini Godbole, Probir
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 informationThe Dark Matter Puzzle and a Supersymmetric Solution. Andrew Box UH Physics
The Dark Matter Puzzle and a Supersymmetric Solution Andrew Box UH Physics Outline What is the Dark Matter (DM) problem? How can we solve it? What is Supersymmetry (SUSY)? One possible SUSY solution How
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 informationPhenomenology of new neutral gauge bosons in an extended MSSM
Phenomenology of new neutral gauge bosons in an extended MSSM Gennaro Corcella 1, Simonetta Gentile 2 1. Laboratori Nazionali di Frascati, INFN 2. Università di oma, La Sapienza, INFN Outline Motivation
More informationChapter 4 Supersymmetry
Chapter 4 Supersymmetry Contents 4.1 Introduction... 68 4. Difficulties in the standard model... 68 4.3 Minimal Supersymmetric Standard Model... 69 4.3.1 SUSY... 69 4.3. Reasons to introduce SUSY... 69
More informationIntroduction to SUSY. Giacomo Polesello. INFN, Sezione di Pavia
. Introduction to SUSY Giacomo Polesello INFN, Sezione di Pavia Why physics beyond the Standard Model? Gravity is not yet incorporated in the Standard Model Hierarchy/Naturalness problem Standard Model
More informationTesting the Standard Model and Search for New Physics with CMS at LHC
Dezső Horváth: Search for New Physics with CMS FFK2017, Warsaw, Poland p. 1 Testing the Standard Model and Search for New Physics with CMS at LHC FFK-2017: International Conference on Precision Physics
More informationPhysics Beyond the. Texas A&M University. For the. Mini-Symposium May, 2009
Physics Beyond the Standard Model David Toback Texas A&M University For the David Toback, Texas CDF A&M and University DØ collaborations 1 Mini-Symposia on Searches Exciting New Search Results from the
More informationUniversal Extra Dimensions
Universal Extra Dimensions Add compact dimension(s) of radius R ~ ant crawling on tube Kaluza-Klein tower of partners to SM particles due to curled-up extra dimensions of radius R n = quantum number for
More informationSearches for New Phenomena with Lepton Final States at the Tevatron
Searches for New Phenomena with Lepton Final States at the Tevatron including charginos, neutralinos,, excited leptons and unexpected signatures Todd Adams Florida State University for the CDF and DØ Collaborations
More informationHiggs Physics. Yasuhiro Okada (KEK) November 26, 2004, at KEK
Higgs Physics Yasuhiro Okada (KEK) November 26, 2004, at KEK 1 Higgs mechanism One of two principles of the Standard Model. Gauge invariance and Higgs mechanism Origin of the weak scale. Why is the weak
More informationBEST: Bi-Event Subtraction Technique and Mass Reconstruction at the LHC
BEST: Bi-Event Subtraction Technique and Mass Reconstruction at the LHC Kuver Sinha Mitchell Institute for Fundamental Physics Texas A M University PHENO 2012 Supersymmetry at the LHC DM (or l+l-, τ+τ
More informationInterconnection between Particle Physics and Cosmology at the LHC
Interconnection between Particle Physics and Cosmology at the LHC Selections from the Cosmo Secret Cube Catalogue Transformer Cube Standard Model Cube PPC Cube Premiere Props Teruki Kamon Mitchell Institute
More informationDPG Sascha Caron (Freiburg)
DPG 2010 Sascha Caron (Freiburg) Outline 2 Reminder: Why is SUSY interesting? SUSY production at LHC LHC, ATLAS and CMS status What can we expect in the next 2 years? Summary SUSY Reminder 3 SUPERSYMMETRY
More informationTheoretical Developments Beyond the Standard Model
Theoretical Developments Beyond the Standard Model by Ben Allanach (DAMTP, Cambridge University) Talk outline Bestiary of some relevant models SUSY dark matter Spins and alternatives B.C. Allanach p.1/18
More information