Pheno family reunion, 4/2008
|
|
- Allison Singleton
- 5 years ago
- Views:
Transcription
1 Stuff SFitter: Combining Stuff University of Edinburgh Pheno family reunion, 4/2008
2 Stuff Outline Phenomenology in the Underlying parameters ed SFitter
3 Stuff Phenomenology in the All hopes on the LHC find light Higgs? find new physics stabilizing Higgs mass? see dark matter candidate? early data: playing a fun game understood data: test TeV-scale models Particle theory in the test huge number of hypotheses [given too much time for model builders] forget about model independent analyses [tough LHC environment] link to other observations [DM+Tevatron propaganda uncovered: Hooper, TP, Vallinotto] reconstuct TeV-scale Lagrangian Role of LHC beyond inclusive searches [that was Tevatron] millions of new strongly interacting particles (1) try to survive QCD (2) aim at underlying theory χ 2o χ 1+ ν ν t 1t 1 χ 2o q χ 2o g Prospino2 (T Plehn) σ tot [pb]: pp g g, q q, t 1t 1, χ 2 o χ 1+, ν ν, χ 2o g, χ 2o q q q g g S = 14 TeV NLO LO m [GeV]
4 Stuff Underlying parameters From kinematics to weak scale parameters parameters: weak-scale Lagrangian [Fittino; SFitter: Lafaye, TP, Rauch, Zerwas] measurements: kinematic endpoints, branching ratios, rates [Prospino2] B decays, (g 2) µ, dark matter, e-w precision data... errors: general correlation, statistics & systematics & theory [flat theory errors!] problem in grid/fit: no local/global maximum problem in physics: secondary maxima
5 Stuff Underlying parameters From kinematics to weak scale parameters parameters: weak-scale Lagrangian [Fittino; SFitter: Lafaye, TP, Rauch, Zerwas] measurements: kinematic endpoints, branching ratios, rates [Prospino2] B decays, (g 2) µ, dark matter, e-w precision data... errors: general correlation, statistics & systematics & theory [flat theory errors!] problem in grid/fit: no local/global maximum problem in physics: secondary maxima Probability maps of new physics [Baltz,...; Roszkowski,...; Allanach,...; SFitter] undisputed: exclusive likelihood map p(d m) over m [hard part] general problem: remove directions Bayesian: p(m d) p(d m) p(m) with theory bias p(m) How does dark matter annihilate/couple? frequentist: best fitting point max m p(d m) Which is the most likely parameter point? [Allanach, Cranmer, Lester, Weber] m 0 (TeV) M 1/2 (TeV) L/L(max)
6 Stuff Underlying parameters From kinematics to weak scale parameters parameters: weak-scale Lagrangian [Fittino; SFitter: Lafaye, TP, Rauch, Zerwas] measurements: kinematic endpoints, branching ratios, rates [Prospino2] B decays, (g 2) µ, dark matter, e-w precision data... errors: general correlation, statistics & systematics & theory [flat theory errors!] problem in grid/fit: no local/global maximum problem in physics: secondary maxima Toy model: MSUGRA map from LHC [LHC endpoints with free y t ] weighted Markov chains [similar to: Ferrenberg & Swendsen] N P bin(p 0) = P Ni=1 1/p SFitter output #1: fully exclusive likelihood map SFitter output #2: ranked list of local maxima correlations and seconday maxima mean need for more measurements m t A χ 2 m 0 m 1/2 tan β A 0 µ m t 0.3e
7 Stuff Underlying parameters MSSM map in [SFitter+friends] from 6 to 19 parameter dimensions [killing grids, Minuit, laptop style fits...] SFitter outputs still the same, best points degenerate LHC edges: sign(µ) unknown [Allanach...] µ e+08 1e M 1 LHC edges: tan β from m h believe based and poor [even in msugra] tan(β) m 0 LHC rates: tan β from heavy Higgs tough [Kinnunen, Lehti, Moortgat, Nikitenko, Spira] flavor physics finally of BSM use? [Polesello in Cern flavor-lhc report] 1e
8 Stuff ed SFitter physics in the traditional flavor observables: BR(B s µµ) tan 6 β [SFitter + Jäger, Spannowsky] (g 2) µ tan β [SFitter + Alexander, Kreiss] serious physics: errors the key
9 Stuff ed SFitter physics in the traditional flavor observables: BR(B s µµ) tan 6 β [SFitter + Jäger, Spannowsky] (g 2) µ tan β [SFitter + Alexander, Kreiss] serious physics: errors the key BR(B s µµ) combined with stop chargino sector [Hisano, Kawagoe, Nojiri] 7% error on f Bs by 2015 crucial [Della Morte, Del Debbio] perturbative effects secondary no theory error BR/BR = 15% true best error best error tan β M A M M M µ M t,r
10 Stuff ed SFitter physics in the traditional flavor observables: BR(B s µµ) tan 6 β [SFitter + Jäger, Spannowsky] (g 2) µ tan β [SFitter + Alexander, Kreiss] serious physics: errors the key BR(B s µµ) combined with stop chargino sector [Hisano, Kawagoe, Nojiri] 7% error on f Bs by 2015 crucial [Della Morte, Del Debbio] perturbative effects secondary no theory error BR/BR = 15% true best error best error tan β M A M M M µ M t,r (g 2) µ combined with slepton neutralino sector [review: Stöckinger] already current precision promising LHC LHC (g 2) SPS1a tan β 10.0± ± M ± ± M ± ± M ± ± µ 350.5± ± M µ,r 135.0± ± M q,r 507.3± ± technical fitting/scanning issues solved and implemented in SFitter work to be done, community focus not helpful?
11 Stuff Physics in the understand e-w symmetry breaking confirm new physics [dark matter] complete Standard Model Fundamental theory SUSY breaking? unification, GUT? scale-invariant sum rules? [Cohen, Schmalz] renormalization group bottom up [SFitter + Kneur] LHC sensitive to UV models 1/M i M 1 M 2 M log(q) Technical status 20D parameter spaces under control [including statistics and errors] give us time to apply methods collaborations and suggestions welcome
12 Stuff
Tilman Plehn. Mainz 2/2009
Once we have all Heidelberg Mainz 2/29 Outline Effective Standard Model from cascades Interlude: and jets Interlude: spins from jets Underlying parameters TeV-scale MSSM: Effective Standard Model Data
More informationLHC More than just Discoveries. Tilman Plehn. SUSY parameters. Markov chains. SUSY maps. MPI für Physik & University of Edinburgh.
LHC More than MPI für Physik & University of Edinburgh Budapest, 6/27 Outline Weak Boson Fusion and Supersymmetry Supersymmetric parameter space SUSY parameter maps Weak Boson Fusion and Supersymmetry
More informationFun physics at the LHC
Fun physics at the LHC Edinburgh Cambridge /2008 Outline Effective Standard Model Underlying parameters Annoying TeV-scale MSSM: Large extra dimensions Effective KK theory completion Fixed-point completion
More informationMSSM Parameter Reconstruction at the LHC
MSSM Parameter Reconstruction at the LHC Michael Rauch Rémi Lafaye, Tilman Plehn, Dirk Zerwas Michael Rauch SFitter: MSSM Parameter Reconstruction at the LHC SUSY-GDR 7 p. 1 What SFitter does Set of measurements
More informationReconstructing the Supersymmetric Lagrangian
Reconstructing the Supersymmetric Lagrangian Michael Rauch (in collaboration with Rémi Lafaye, Tilman Plehn, Dirk Zerwas) arxiv:79.3985 [hep-ph] https://trac.lal.in2p3.fr/sfitter Michael Rauch SFitter:
More informationReconstructing Supersymmetry in the LHC era
Reconstructing Supersymmetry in the LHC era Michael Rauch ( in collaboration with Rémi Lafaye, Tilman Plehn, Dirk Zerwas) Michael Rauch SFitter: Reconstructing Supersymmetry in the LHC era Durham, Nov
More informationReconstructing the Supersymmetric Lagrangian
Reconstructing the Supersymmetric Lagrangian Michael Rauch ( in collaboration with Rémi Lafaye, Tilman Plehn, Dirk Zerwas) arxiv:79.3985 [hep-ph] Michael Rauch SFitter: Reconstructing the Supersymmetric
More informationMeasuring Supersymmetry
Measuring Supersymmetry Michael Rauch ( in collaboration with Rémi Lafaye, Tilman Plehn, Dirk Zerwas) arxiv:79.3985 [hep-ph] Michael Rauch SFitter: Measuring Supersymmetry Edinburgh, Dec 7 p. Outline Supersymmetry
More informationReconstructing the supersymmetric Lagrangian
Reconstructing the supersymmetric Lagrangian Michael Rauch ( in collaboration with Rémi Lafaye, Tilman Plehn, Dirk Zerwas) Michael Rauch SFitter: Reconstructing the supersymmetric Lagrangian Glasgow, Feb
More informationTilman Plehn. Dresden, 4/2009
New Physics at the Universität Heidelberg Dresden, 4/2009 Outline The Large Hadron Collider: starting Summer 20XX The Large Hadron Collider: starting Summer 20XX Einstein: beam energy to particle mass
More informationKarlsruhe, 12/2006. New Methods for New Physics. Tilman Plehn. Supersymmetry. LHC Signals. Masses. Spins. Parameters. Some ideas
New Methods MPI für Physik & University of Edinburgh Karlsruhe, 12/26 Outline TeV scale supersymmetry Supersymmetric signatures at LHC New physics mass measurements New physics spin measurements Supersymmetric
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 informationSUPERSYMMETRY AT THE LHC
SUPERSYMMETRY AT THE LHC Tilman Plehn MPI München and University of Edinburgh A few MSSM conventions SUSY-Higgs at the LHC SUSY at the Tevatron SUSY searches at the LHC SUSY measurements at the LHC (and
More informationSeminar IKTP, TU Dresden January 07, 2010
1 Predicting and understanding supersymmetry Peter Wienemann University of Bonn Work in collaboration with: Philip Bechtle (DESY), Klaus Desch and Mathias Uhlenbrock (U Bonn) Seminar IKTP, TU Dresden January
More informationGlobal (SUSY) Fits in 2012 (Frequentist Approach)
Global (SUSY) Fits in 2012 (Frequentist Approach) Oliver Buchmueller Imperial College London darkattack2012 1 Confronting a theory with data Recipe: Combine measurements Compare with predictions Constrain
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 informationSupersymmetry at the LHC
at the LHC Heidelberg PSI, 10/2010 Standard Model effective theory Building a fundamental theory Fermi 1934: theory of weak interactions [n pe νe] (2 2) transition amplitude A G F E 2 probability/ unitarity
More informationModel Fitting in Particle Physics
Fits to Model Fitting in Particle Physics Matthew Dolan 1 1 DAMTP University of Cambridge High Throughput Computing in Science, 2008 Outline Fits to 1 2 3 Outline Fits to 1 2 3 Model Fits to Model of particle
More informationHigh tanβ Grid Search
October 21, 2011 About me About me Started my 4 year PhD in january 2011 at the university of Bergen under the DAMARA project About me About me Started my 4 year PhD in january 2011 at the university of
More informationMagnetic moment (g 2) µ and new physics
Dresden Lepton Moments, July 2010 Introduction A 3σ deviation for a exp µ a SM µ has been established! Currently: a exp µ a SM µ = (255 ± 63 ± 49) 10 11 Expected with new Fermilab exp. (and th. progress):
More informationExploring new physics at the LHC
Goethe-Universität Frankfurt, January 12th 2011 Exploring new physics at the LHC Michael Krämer (RWTH Aachen) 1 / 46 Goethe-Universität Frankfurt, January 12th 2011 Exploring new physics at the LHC Michael
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 informationIdentifying the NMSSM by combined LHC-ILC analyses
Identifying the NMSSM by combined LHC-ILC analyses Stefan Hesselbach High Energy Physics, Uppsala University based on G. Moortgat-Pick, S. Hesselbach, F. Franke, H. Fraas, JHEP 06 (2005) 048 [hep-ph/0502036]
More informationSUSY-particle production at Hadron Colliders
NRW Phänomenoloie-Treffen, Januar 2006 SUSY-particle production at Hadron Colliders Michael Krämer (RWTH Aachen) Basics of SUSY particle production at hadron colliders The calculation of SUSY-QCD corrections
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 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 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 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 informationGood News for LHC Analyses
Good News for LHC Analyses Not a proper unbiased theory overview Universität Heidelberg Higgs Workshop, Seattle, /29 Outline SFitter at LHC Weak boson fusion and supersymmetry A new channel to detect H
More informationJet Substructure. Adam Davison. University College London
Jet Substructure Adam Davison University College London 1 Outline Jets at the LHC Machine and ATLAS detector What is a jet? Jet substructure What is it? What can it do for us? Some ATLAS/Higgs bias here
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 informationPhysics at e + e - Linear Colliders. 4. Supersymmetric particles. M. E. Peskin March, 2002
Physics at e + e - Linear Colliders 4. Supersymmetric particles M. E. Peskin March, 2002 In this final lecture, I would like to discuss supersymmetry at the LC. Supersymmetry is not a part of the Standard
More informationSUSY and Exotica. Talk outline. Ben Allanach (University of Cambridge)
SUSY and Exotica by Ben Allanach (University of Cambridge) Talk outline SUSY Fits Impact of LHC data SUSY Tactics Exotica and A FB (t t) Please ask questions while I m talking SUSY and Exotica B.C. Allanach
More informationSearch for Resonant Slepton Production with DØ
Overview Search for Resonant Slepton Production with DØ Christian Autermann, III. Phys. Inst. A, RWTH Aachen Event Topology Data Selection and Efficiencies Control Plots Selection Optimization Preliminary
More informationSlepton, Charginos and Neutralinos at the LHC
Slepton, Charginos and Neutralinos at the LHC Shufang Su U. of Arizona, UC Irvine S. Su In collaboration with J. Eckel, W. Shepherd, arxiv:.xxxx; T. Han, S. Padhi, arxiv:.xxxx; Outline Limitation of current
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 informationDark Matter Implications for SUSY
Dark Matter Implications for SUSY Sven Heinemeyer, IFCA (CSIC, Santander) Madrid, /. Introduction and motivation. The main idea 3. Some results 4. Future plans Sven Heinemeyer, First MultiDark workshop,
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 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 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 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 informationLHC+LC Synergy: SUSY as a case study
LHC+LC Synergy: SUSY as a case study εργον συν work together Outline: Why LHC/LC studies? Why SUSY as case study? 5 Examples of Synergy Conclusions Klaus Desch University of Hamburg ALCPG meeting - SLAC
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 informationBeenakker, Hopker, Spira, Zerwas, hep-ph/
m g = GeV N - -!(q q ) [ pb] #m q = + GeV m g = GeV #m q = +3 GeV - 5 5 3 35 4!(q q ") [ pb] - - evatron 5 5 35 35 4 5 5 3 35 5 3 35 q 4 m g [GeV] (a)!(g g ) [ pb] N m N q = GeV #m g = +8 GeV - - N!(g
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 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 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 informationSearch for Resonant Slepton Production with the DØ-Experiment
Overview Search for Resonant Slepton Production with the DØ-Experiment Christian Autermann, III. Phys. Inst. A R-parity violating Supersymmetry Resonant Slepton Production and Neutralino Decay Data selection
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 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 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 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 informationThe study of the properties of the extended Higgs boson sector within hmssm model
The study of the properties of the extended Higgs boson sector within hmssm model T.V. Obikhod, E.A. Petrenko Institute for Nuclear Research, National Academy of Science of Ukraine 47, prosp. Nauki, Kiev,
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 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 informationSUSY Candidates. Talk outline. Ben Allanach (University of Cambridge) SUSY dark matter: generalities Neutralino Gravitino Sneutrino Axino
SUSY Candidates by Ben Allanach (University of Cambridge) Talk outline SUSY dark matter: generalities Neutralino Gravitino Sneutrino Axino SUSY Candidates Please ask questions while I m talking B.C. Allanach
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 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 informationSupersymmetry at the ILC
Supersymmetry at the ILC Abdelhak DJOUADI (LPT Paris Sud). Introduction 2. High precision measurements 3. Determination of the SUSY lagrangian 4. Connection to cosmology 5. Conclusion For more details,
More informationPrecision Calculations for Collider Physics
SFB Arbeitstreffen März 2005 Precision Calculations for Collider Physics Michael Krämer (RWTH Aachen) Radiative corrections to Higgs and gauge boson production Combining NLO calculations with parton showers
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 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 informationStau Pair Production At The ILC Tohoku University Senior Presentation Tran Vuong Tung
e + Z*/γ τ + e - τ Stau Pair Production At The ILC Tohoku University Senior Presentation Tran Vuong Tung 1 Outline Introduction of the International Linear Collider (ILC) Introduction of (g μ -2) in the
More informationProbing SUSY Contributions to Muon g-2 at LHC and ILC
Probing SUSY Contributions to Muon g-2 at LHC and ILC Motoi Endo (Tokyo) Based on papers in collaborations with ME, Hamaguchi, Iwamoto, Yoshinaga ME, Hamaguchi, Kitahara, Yoshinaga ME, Hamaguchi, Iwamoto,
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 informationAbdelhak DJOUADI (LPT Orsay/Next Southampton)
SUSY@ILC Abdelhak DJOUADI (LPT Orsay/Next Southampton) 1. Probing SUSY 2. Precision SUSY measurements at the ILC 3. Determining the SUSY Lagrangian 4. Summary From the physics chapter of the ILC Reference
More informationBeyond the MSSM (BMSSM)
Beyond the MSSM (BMSSM) Nathan Seiberg Strings 2007 SUSY 2012 Based on M. Dine, N.S., and S. Thomas, to appear Assume The LHC (or the Tevatron) will discover some of the particles in the MSSM. These include
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 informationIntroducing SModelS - with an application to light neutralino DM
Hi! Introducing SModelS - with an application to light neutralino DM Suchita Kulkarni (LPSC, Grenoble) based on: 1) work in progress with W. Waltenberger, U. Laa, A. Lessa, D. Proschofsky, S. Kraml 2)
More informationNon-Standard Higgs Decays
Non-Standard Higgs Decays David Kaplan Johns Hopkins University in collaboration with M McEvoy, K Rehermann, and M Schwartz Standard Higgs Decays Standard Higgs Decays 1 _ bb 140 GeV WW BR for SM Higgs
More informationHiggs couplings. Michael Rauch HDays 2012 INSTITUTE FOR THEORETICAL PHYSICS
Higgs couplings Michael Rauch HDays INSTITUTE FOR THEORETICAL PHYSICS KIT Universität des Landes Baden-Württemberg und nationales Forschungszentrum in der Helmholtz-Gemeinschaft www.kit.edu Higgs properties
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 informationFlavor Violation at the LHC. Bhaskar Dutta. Texas A&M University
Flavor Violation at the LHC Bhaskar Dutta Texas A&M University Sixth Workshop on Theory, Phenomenology and Experiments in Flavour Physics - FPCapri2016, June 13th, 2016 1 Outline 1. Colored, Non colored
More informationSearching for Supersymmetric Higgs Bosons at the LHC
Searching for Supersymmetric Higgs Bosons at the LHC Tilman Plehn CERN Light neutral Higgs: no-lose-theorem Charged Higgs: bottom induced processes Heavy neutral Higgs: decay to two light Higgses MSSM
More informationarxiv:hep-ex/ v1 15 Jun 2006
arxiv:hep-ex/6636v 5 Jun 6 SEARCHES FOR NEW PHYSICS IN LEPTON FINAL STATES CATALIN I. CIOBANU FOR THE CDF AND DØ COLLABORATIONS Department of Physics, University of Illinois at Urbana-Champaign, W. Green
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 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 scans and dark matter
SUSY scans and dark matter Pat Scott Oskar Klein Centre for Cosmoparticle Physics & Department of Physics, Stockholm University May 27 2010 Mostly based on: JCAP 1001:031 (2010; arxiv:0909.3300) JHEP 1004:057
More informationSUSY Parameter and Mass Determination at the LHC
SFB 676 Project B2 SUSY Parameter and Mass Determination at the LHC C. Sander, Hamburg University Cambridge Phenomenology Seminar C. Sander - Parameter Determination at the LHC 2 kstars Cambridge 25th
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 informationMadGolem: Automated NLO predictions for SUSY and beyond
David López-Val D. Gonçalves Netto (MPI, Munich), T. Plehn (Heidelberg U.), I. Wigmore (Edinburgh U.), K. Mawatari (Vrije U.) together with ITP - Universität Heidelberg SUSY 2013, Trieste (Italy) - August
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 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 informationNon-Minimal SUSY Computation of observables and fit to exp
Non-Minimal SUSY Computation of observables and fit to experimental data + Peter Athron, Alexander Voigt Dresden Fittino Workshop, 24th November 2010, DESY Outline 1 Introduction 2 Motivation 3 Outline
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 informationarxiv:hep-ph/ v1 11 Jan 2001
IFT/00-36 hep-ph/0101111 Phenomenology of the Chargino and Neutralino Systems arxiv:hep-ph/0101111v1 11 Jan 2001 J. Kalinowski Instytut Fizyki Teoretycznej, Uniwersytet arszawski Hoża 69, 00681 arsaw,
More informationThe Standard Model and Beyond
The Standard Model and Beyond Nobuchika Okada Department of Physics and Astronomy The University of Alabama 2011 BCVSPIN ADVANCED STUDY INSTITUTE IN PARTICLE PHYSICS AND COSMOLOGY Huê, Vietnam, 25-30,
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 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 informationMagnetic moment (g 2) µ and beyond the Standard Model physics
Magnetic moment (g 2) µ and beyond the Standard Model physics TU Dresden Lepton Moments Symposium, Cape Cod, July 2014 Discrepancy SM prediction too low by (28.7±8.0) 10 10 Note: discrepancy twice as large
More informationDetecting and Distinguishing Top Partners
Detecting and Distinguishing Top Partners Ayres Freitas and Devin Walker After the discovery of tt+e/ T events at a hadron collider it will be crucial to determine the properties of the new particles which
More informationBSM at the LHC. Dirk Zerwas LAL Orsay
BSM at the LHC Dirk Zerwas LAL Orsay Lecture I: LHC and the Detectors Standard Model Lecture II: The standard model Higgs boson The supersymmetric Higgs bosons Lecture III: Supersymmetry Exotics Supersymmetry
More informationA profile likelihood analysis of the CMSSM with Genetic Algorithms
A profile likelihood analysis of the CMSSM with Genetic Algorithms TeVPA 2009 / SLAC / July 13, 2009 Yashar Akrami Collaborators: Pat Scott, Joakim Edsjö, Jan Conrad and Lars Bergström Oskar Klein Center
More informationTop and Higgs Tagging and Where it Helps
Top and Higgs Tagging and Where it Helps Universität Heidelberg Mainz 2/2 Boosted particles at the LHC 994 boosted W 2 jets from heavy Higgs [Seymour] 994 boosted t 3 jets [Seymour] 22 boosted W 2 jets
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 informationComposite gluino at the LHC
Composite gluino at the LHC Thomas Grégoire University of Edinburgh work in progress with Ami Katz What will we see at the LHC? Natural theory of EWSB? Supersymmetry? Higgs as PGSB (LH, RS-like)? Extra-
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 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 informationExotic Dark Matter as Spin-off of Proton Stability. Kaustubh Agashe (University of Maryland)
Exotic Dark Matter as Spin-off of Proton Stability Kaustubh Agashe (University of Maryland) Outline and Summary Warped extra dimensions address Planckweak and flavor hierarchies: new (KK) particles at
More informationSupersymmetry at the LHC
Supersymmetry at the LHC Howard Baer Florida State University SUSY at LHC SUSY models GEANT figure sparticle production msugra : ~ g - W + b ( jet4, s ( jet5, ~+ ( jet3, W2 + b ~+ W1 + Z ~ Z1 + event generation
More information