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This presentation provides an introduction to Supersymmetry (SUSY) models and discusses various signatures and techniques for measuring masses at the Large Hadron Collider (LHC). It also explores R-parity conserving and violating scenarios, long-lived charged sparticles, and the challenges in finding conclusive evidence for SUSY.
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Overview of SUSY phenomenology at the LHC Are R. Raklev CERN / University of Bergen TexPoint fonts used in EMF. Read the TexPoint manual before you delete this box.: AAAAAAAA
Content • SUSY models • (mSUGRA?) Signatures • Measuring masses • R-parity conserving vs. R-parity violating • Long lived charged sparticles • Finding that it’s SUSY • Lack of conclusions Overview of SUSY phenomenology
Warning Label • Not an experiment talk • No motivation slide • Not complete (not even close) • Also, apologies for any stupid jokes... Overview of SUSY phenomenology
SUSY models SUSY MSSM GMSB mSUGRA NMSSM Split SUSY AMSB Will keep to the MSSM subset of all SUSY models Overview of SUSY phenomenology
(mSUGRA) Signatures [Drawing by C. Lester] Overview of SUSY phenomenology
(mSUGRA) Signatures We expect (or perhaps hope for?): • Missing energy – from ”missing” LSP • Hard jets – from gluino/squark production • Leptons – from gaugino decays Overview of SUSY phenomenology
(mSUGRA) Signatures We expect (or perhaps hope for?): • Missing energy – from ”missing” LSP • Hard jets – from gluino/squark production • Leptons – from gaugino decays However: • The LSP might decay (R-parity violation) • We can have a metastable NLSP (GMSB, GDM etc.) • Squarks and sleptons may be too heavy to be produced(Split SUSY) • The whole SUSY spectrum might be quite degenerate(Mixed modular anomaly mediation, MMAM) [Choi et al 2005] Overview of SUSY phenomenology
(mSUGRA) Signatures Cross sections for gluino / squark production very probably several orders of magnitude below SM background [CMS collaboration] Overview of SUSY phenomenology
with lepton veto • One lepton channel • Two opposite sign (OS) leptons • Two same sign (SS) leptons (mSUGRA) Signatures CMS 5 reach for R-parity conserving mSUGRA in various inclusive channels: [CMS collaboration] Overview of SUSY phenomenology
Effective mass Effective mass, an effective discriminant between SUSY and SM background. Open circles are SUSY events, hatched histogram total SM background. [ATLAS TDR, 1999] Overview of SUSY phenomenology
Effective mass [ATLAS TDR, 1999] Overview of SUSY phenomenology
Effective mass [ATLAS TDR, 1999] [Asai, TeV4LHC workshop, 2005] Overview of SUSY phenomenology
Effective mass Progress towards a better understanding of SM multi-jet backgrounds Attempt to use PS and ME matching to estimate multi-jet backgrounds. Results from Tevatron very important! [Asai and Sasaki, hep-ph/0608322] Overview of SUSY phenomenology
Measuring masses • With escaping neutalinos we must study the kinematics of the detectable decay products of decay chains to measure masses • Let’s take the following decay chain as an example Overview of SUSY phenomenology
Measuring masses • The distribution of the invariant mass of the two leptons can be shown to have a kinematic edge (endpoint) at Overview of SUSY phenomenology
Kinematic edges SPS1a [Gjelsten, Miller, Osland, hep-ph/0410303] Overview of SUSY phenomenology
Kinematic edges SPS1a SPS1a SPS1a [Gjelsten, Miller, Osland, hep-ph/0410303] Overview of SUSY phenomenology
Kinematic edges Drawbacks: • We must manage to identify the correct jets and/or leptons • Fitting endpoints is a tricky buisness: Multiple solutions, feet • Very good at mass differences, very bad at absolute mass SPS1a Overview of SUSY phenomenology
Kinematic edges Drawbacks: • We must manage to identify the correct jets and/or leptons • Fitting endpoints is a tricky buisness: Multiple solutions, feet • Very good at mass differences, very bad at absolute mass • What did we measure? Identification of decay chain • Does not use all information Improvements: • Use complete distribution, not only endpoint [Miller, Osland, ARR, hep-ph/0510356] Overview of SUSY phenomenology
Other techniques Three unknown momenta components Mass relation method: Only four constraints, but next event has only three more unknowns! Four unknown masses [Kawagoe, Polesello, Nojiri, hep-ph/0402295] Overview of SUSY phenomenology
To R-parity or not to R-parity RPC RPV RPV [Drawings by C. Lester] Overview of SUSY phenomenology
To R-parity or not to R-parity SM SUSY Overview of SUSY phenomenology
RPV • Lepton number violating couplings: • Baryon number violating couplings: • Strong bound on most couplings, • Will imitate RPC if • No missing energy? Not neccessarily true for lepton number violation. Overview of SUSY phenomenology
Long live the Sparticles! A number of models exist that can have long lived charged sparticles: In principle no transverse momentum imbalance, but sometimes slow sparticles! Overview of SUSY phenomenology
Long live the Sparticles! Many interesting experimental signatures: • Slow, muon-like particles. If we can measure Time-of-Flight: • High ionization • Late decays & trapped particles • Charge flipping (R-hadrons) [Ellis, ARR, Øye, hep-ph/0607261] Overview of SUSY phenomenology
Long live the Sparticles! Many interesting experimental signatures: • Slow, muon-like particles • High ionization • Late decays & trapped particles • Charge flipping (R-hadrons) Overview of SUSY phenomenology
Finding SUSY vs. finding it’s SUSY Assuming that we find a 5 deviation from the SM in some channel, or even measure the masses of some particles, how do we know if it’s SUSY? For example, can we determine spin in our decay chains? [A. Barr, hep-ph/0405052] Overview of SUSY phenomenology
What I haven’t said • NMSSM and other non-minimal models • LFV (through slepton mixing) • Gaugino mixing matrices (estimating DM density) • SUSY higgs sector (see Filip Moortgat’s talk) • Pluss many other things I’ve forgotten about • Including also not saying anything about most of the around 12,000 papers on SPIRES with ”SUSY” or ”supersymmetry” in the title! Overview of SUSY phenomenology
[With apologies to D. Kazakov for stealing his joke from ICHEP’06] Overview of SUSY phenomenology
Backup slide Green areas in mSUGRA plane shows the existence of the usefull decay chain: Overview of SUSY phenomenology
Backup slide Early stage 5 reach contours for missing energy channel. [Tovey, 2002] Overview of SUSY phenomenology
Backup slide [Kawagoe, Nojiri, hep-ph/0606104] Overview of SUSY phenomenology
Backup slide [Kran, Hansen, Nevski, hep-ph/0511014] Overview of SUSY phenomenology