Little Higgs at the LHC: Status and Prospects
|
|
- Reynard Hall
- 5 years ago
- Views:
Transcription
1 Little Higgs at the LHC: Status and Prospects Marco Tonini DESY Theory Group (Hamburg) based on: Reuter/MT, JHEP 1302, 077 (2013) Reuter/MT/de Vries, hep-ph/ Reuter/MT/de Vries, DESY (in prep.) SUSY August 2013
2 Motivation How to constrain a generic model in HEP? direct searches for resonances electroweak precision tests flavour constraints nowadays: Higgs sector Higgs sector is the key to understand EW-scale physics (and beyond?) 2 / 17
3 Two paradigms for EWSB hierarchy problem as guideline to answer the following question: what is the dynamical origin of EWSB? weakly coupled answer Ñ Supersymmetry strongly coupled answer Ñ Composite Higgs, Little Higgs... 3 / 17
4 Strongly coupled answer Original idea: pions of low-energy QCD E QCD - quarks as d.o.f. - perturbative th. for E>Λ low-energy QCD - pions: pngb of SSB (new d.o.f.) - eff. theory valid up to E<Λ Λ 1 GeV: SSB of QCD-flavour symmetry SU(2)xSU(2) SU(2) L QCD = 1 4 Ga µνg µν a + qi/dq q=u,d L 2 = f 2 4 tr µ Σ 2, Σ =exp i π 0 π + f π π 0 Composite/Little Higgs Ansatz Higgs as pngb of a new (approximate) global symmetry which is spontaneously broken at a scale Λ 4πf 4 / 17
5 Strongly coupled answer Original idea: pions of low-energy QCD E QCD - quarks as d.o.f. - perturbative th. for E>Λ low-energy QCD - pions: pngb of SSB (new d.o.f.) - eff. theory valid up to E<Λ Λ 1 GeV: SSB of QCD-flavour symmetry SU(2)xSU(2) SU(2) L QCD = 1 4 Ga µνg µν a + qi/dq q=u,d L 2 = f 2 4 tr µ Σ 2, Σ =exp i π 0 π + f π π 0 Composite/Little Higgs Ansatz Higgs as pngb of a new (approximate) global symmetry which is spontaneously broken at a scale Λ 4πf 5 / 17
6 Summary The Little Higgs paradigm: it is an effective theory valid up to the cut-off Λ: no UV-completion of the strongly coupled regime E ą Λ Higgs as a pngb of a global SSB at Λ 4πf (like pions!) new fermionic/vector states with masses f besides SM-ones EWSB is triggered naturally (Collective Symmetry Breaking), i.e. v Op100 GeVq for f 1 TeV with only log-sensitivity to Λ 6 / 17
7 Outline of the work purpose: constraining the parameter space of the three most popular Little Higgs models Simplest Little Higgs (SLH) [Schmaltz, 2004] Littlest Higgs (L 2 H) [Arkani-Hamed et al., 2002] Littlest Higgs with T parity (LHT) [Low et al., 2003] scrutinizing the available public data from the 7-8 TeV LHC runs Electroweak Precision Tests (EWPT) Higgs Searches Direct Searches for BSM states 7 / 17
8 EWPT & Higgs: Data used Precision constraints of the EW sector: M H M W W M Z Z 0 had 0 Rlep 0,l A FB A l (LEP) A l (SLD) 2 lept sin eff (Q ) FB 0,c A FB 0,b A FB A c A b 0 Rc 0 Rb m c m b m t (5) 2 had (M ) Z G fitter SM May Higgs results expressed in terms of µ i ř p ɛp i ř σp p ɛp i σsm p BR ph Ñ X ix iq BR ph Ñ X ix iq SM ñ best fit for each decay of the Higgs W,Z H bb H s (*) H WW l l s s H s s (*) H ZZ 4l s s Combined s s -1 = 7 TeV: Ldt = 4.6 fb -1 = 8 TeV: Ldt = 13 fb -1 = 7 TeV: Ldt = 4.6 fb -1 = 8 TeV: Ldt = 20.7 fb -1 = 7 TeV: Ldt = 4.8 fb -1 = 8 TeV: Ldt = 20.7 fb -1 = 7 TeV: Ldt = 4.6 fb -1 = 8 TeV: Ldt = 20.7 fb -1 = 7 TeV: Ldt = fb -1 = 8 TeV: Ldt = fb [ATLAS-CONF ] ATLAS Preliminary s s s -1 = 7 TeV: Ldt = 4.7 fb -1 = 8 TeV: Ldt = 13 fb µ = 1.30 ± 0.20 m H = GeV (O - O meas ) / fit meas [GFitter Collaboration] Signal strength (µ) up to 25 fb 1 at 7 ` 8 TeV! 8 / 17
9 Little evidence Where do Little Higgs corrections to SM quantities come from? new Higgs decay channels, e.g. invisible decay h Ñ A H A H in LHT modified Higgs couplings with SM fermions and vector bosons # e.g. 2 m2 W v yw h W `W, 1 SM y W 1 ` O `v 2 {f 2 LH new Higgs interactions with heavy resonances e.g. m T v yt h T T m T f, y T O `v 2 {f 2 modified neutral- and charged-currents g ÿ SM e.g. fγ µ pgl ` δg LqP L ` pgr SM ` δg RqP R f Z µ c W f 9 / 17
10 EWPT & Higgs: Results parameters: f SSB scale, R ratio of Yukawa couplings in top sector f Á 694 GeV at 95% CL ñ lower bounds on heavy partners, e.g. m W 1 Á 453 GeV m T Á 984 GeV minimum required fine tuning: 5% results mainly driven by EWPT (ev. see backup) 10 / 17
11 Direct Searches: Data used ATLAS and CMS published results of many SUSY & Exotica searches for BSM states, using up to 20 fb 1 data of 8 TeV LHC runs final state topology ATLAS CMS monojet + {E T CONF PAS EXO CONF jets + {E T PAS SUS CONF lepton(s) + jets + {E T CONF CONF CONF mostly interesting for BSM theorists: 95% CL upper bounds on the visible cross section of a generic BSM signal over the SM background σ vis σ BSM prod BR loooomoooon th. pred. ɛ A lomon cuts efficiency 11 / 17
12 Direct Searches: Recasting Analysis our work: ñ recasting of available analyses assuming a Little Higgs signal 1 generate samples of LH signal events matching the final state topologies, and evaluate relative cross-sections evaluate ɛ A of the event samples applying the selection cuts of the different analyses if σvis LH ą σ 95% : parameter space point is excluded at 95% CL vis 1 only for the Littlest Higgs model with T parity 12 / 17
13 An example example: monojet + {E T final state topology possible LHT signal: p p Ñ Q H QH Ñ pqa H q p qa H q! " #$%&'(# +#,# * " #,# +# )# )# * " # +#! " #$%&'(# ATLAS-CONF selection cuts: σ LHT vis σ 95% vis ñ n j ď 2 w/ p T ą 30 GeV p T pj 1q ą 120 GeV, ηpj 1q ă 2.0 n L 0 w/ p T peq ą 20 GeV, p T pµq ą 7 GeV {E T ą 120 GeV φp {E T, j 2q ą 0.5 pf 400 GeV, κ 0.5q 21.5 pb 2.8 pb exclusion at 95% CL!! O 13 / 17
14 An example example: monojet + {E T final state topology possible LHT signal: p p Ñ Q H QH Ñ pqa H q p qa H q! " #$%&'(# +#,# * " #,# +# )# )# * " # +#! " #$%&'(# ATLAS-CONF selection cuts: σ LHT vis σ 95% vis ñ n j ď 2 w/ p T ą 30 GeV p T pj 1q ą 120 GeV, ηpj 1q ă 2.0 n L 0 w/ p T peq ą 20 GeV, p T pµq ą 7 GeV {E T ą 120 GeV φp {E T, j 2q ą 0.5 pf 400 GeV, κ 0.5q 21.5 pb 2.8 pb exclusion at 95% CL!! O 14 / 17
15 An example example: monojet + {E T final state topology possible LHT signal: p p Ñ Q H QH Ñ pqa H q p qa H q! " #$%&'(# +#,# * " #,# +# )# )# * " # +#! " #$%&'(# ATLAS-CONF selection cuts: σ LHT vis σ 95% vis ñ n j ď 2 w/ p T ą 30 GeV p T pj 1q ą 120 GeV, ηpj 1q ă 2.0 n L 0 w/ p T peq ą 20 GeV, p T pµq ą 7 GeV {E T ą 120 GeV φp {E T, j 2q ą 0.5 pf 400 GeV, κ 0.5q 21.5 pb 2.8 pb exclusion at 95% CL!! O 15 / 17
16 Direct Searches: Results parameters: f SSB scale, κ mirror fermions coupling (assumed to be flavour blind) f Á 638 GeV at 95% CL (Higgs & EWPT: f Á 694 GeV) mirror fermions mass Á 1 TeV hadronic final states searches still the most sensitive ones four-fermion operator bounds necessary to constrain f possible optimization with the assumption of LHT signal instead of SUSY signal ñ backup slide 16 / 17
17 Conclusions Little Higgs are a viable alternative to weakly coupled solutions like SUSY, where fine tuning is a guideline to understand the naturalness of a model Little Higgs models without T parity are already forced into the TeV range by Electroweak Precision Data for models with T parity, sub-tev life is still possible: in LHT f Á 650 GeV at 95% CL Electroweak Precision Data still represent the most severe constraints, but Higgs- and Direct Searches are getting quickly competitive (especially for T parity models) a comprehensive method to constrain the LHT model has been explored, as well as an optimization proposal for SUSY and Exotica searches to increase the exclusion potential increasing luminosity will improve the visible cross section upper bounds and reduce the uncertainties of the Higgs results 17 / 17
18 Thank you for your attention!
19 Optimization Proposal: monojet + {E T 19 / 17
20 Higgs Searches vs. EWPT the shape of the combined result is driven by the EWPT constraints (much smaller uncertainties) Higgs Searches: for f Á 600 GeV invisible decay h Ñ A H A H open and dominant Higgs Searches: subdominant dependence on R w.r.t. f is a well-known result in the context of the Higgs Low-Energy Theorem 20 / 17
21 L 2 H results parameters: f SSB scale, c mixing angle in gauge sector f Á 3.6 TeV at 95% CL ñ lower bounds on heavy partners, e.g. m W 1 Á 2.4 TeV m T Á 5.1 TeV minimum required fine tuning: 0.1% results driven by EWPT 21 / 17
22 SLH results parameters: f SSB scale, t β ratio of vevs of scalar fields φ 1,2 f Á 3.3 TeV at 95% CL ñ lower bounds on heavy partners, e.g. m W 1 Á 1.5 TeV m T Á 3.2 TeV minimum required fine tuning: 0.5% results driven by EWPT 22 / 17
23 Partial Decay Widths in LH 1-loop decays Γph Ñ ggq LH α2 sm 3 h 32π 3 v 2 ˇˇˇ ÿ f,col 1 ˇˇˇ2 2 F 1 px f q y f 2 Γph Ñ γγq LH α2 m 2 ÿ h 4 ˇˇˇ 256π 3 v 2 2 F 1 px f q y f ` ÿ F 2 1px vq y v ` ÿ F 0px sq y sˇˇˇ2 f,ch v,ch s,ch where x i 4m2 i ; F m ipx iq are loop functions; y 2 i the modified Yuk. couplings h ñ tree-level decays narrow-width approximation: σ ggh LH Γph Ñ σggh ggqlh SM Γph Ñ ggq SM Γph Ñ V V q LH Γph Ñ V V q SM ˆ ghv V g SM Γph Ñ f fq LH Γph Ñ f fq SM ˆ ghff g SM hff hv V 2 2 where g hv V m2 V v y V and g hff m f y v f 23 / 17
24 LHT typical Mass Spectrum 24 / 17
25 LHT typical Branching Ratios Particle Decay BR k 1.0 BR k 0.4 u H A H W H d 61% 0% Z H u 30% 0% A H u 9% 100% W ` H stable A H W 100% 2% u H d 0% 44% d H u 0% 27% l H ν 0% 13.5% ν H l 0% 13.5% Z H A H H 100% 2% d H d 0% 40% u H u 0% 30% 0% 14% ν H ν 0% 14% l H l 25 / 17
26 LHT 8 TeV Production Cross Sections (1) 26 / 17
27 LHT 8 TeV Production Cross Sections (2) 27 / 17
28 LHT 8 TeV Production Cross Sections (3) 28 / 17
arxiv: v1 [hep-ph] 18 Jul 2013
DESY 13-114 Little Higgs Model Limits from LHC Input for Snowmass 2013 arxiv:1307.5010v1 [hep-ph] 18 Jul 2013 Jürgen Reuter 1a, Marco Tonini 2a, Maikel de Vries 3a a DESY Theory Group, D 22603 Hamburg,
More informationNatural Electroweak Symmetry Breaking in NMSSM and Higgs at 100 GeV
Natural Electroweak Symmetry Breaking in NMSSM and Higgs at 100 GeV Radovan Dermíšek Institute for Advanced Study, Princeton R.D. and J. F. Gunion, hep-ph/0502105 R.D. and J. F. Gunion, hep-ph/0510322
More informationarxiv: v2 [hep-ph] 20 Feb 2014
Prepared for submission to JHEP DESY 13-123 Littlest Higgs with T-parity: Status and Prospects arxiv:1310.2918v2 [hep-ph] 20 Feb 2014 Jürgen Reuter, Marco Tonini, Maikel de Vries DESY Theory Group Notkestr.
More informationBSM Higgs Searches at ATLAS
BSM Higgs Searches at ATLAS Martin zur Nedden Humboldt-Universität zu Berlin for the ATLAS Collaboration SUSY Conference 2014 Manchester July 20 th July 25 th, 2014 Introduction Discovery of a scalar Boson
More informationLight generations partners at the LHC
Light generations partners at the LHC Giuliano Panico CERN IPNL Lyon 21 March 2014 based on C. Delaunay, T. Flacke, J. Gonzales, S. Lee, G. P. and G. Perez 1311.2072 [hep-ph] Introduction Introduction
More informationSinglet Assisted Electroweak Phase Transitions and Precision Higgs Studies
Singlet Assisted Electroweak Phase Transitions and Precision Higgs Studies Peter Winslow Based on: PRD 91, 035018 (2015) (arxiv:1407.5342) S. Profumo, M. Ramsey-Musolf, C. Wainwright, P. Winslow arxiv:1510.xxxx
More informationProperties of the Higgs Boson, and its interpretation in Supersymmetry
Properties of the Higgs Boson, and its interpretation in Supersymmetry U. Ellwanger, LPT Orsay The quartic Higgs self coupling and Supersymmetry The Next-to-Minimal Supersymmetric Standard Model Higgs
More informationSearch for Higgs in H WW lνlν
Search for Higgs in H WW lνlν John Alison University of Pennsylvania on behalf of the ATLAS Collaboration Higgs Physics Standard Model Remarkably Accurate Description Data. One Remaining Piece: Higgs Boson.
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 informationOblique corrections from Light Composite Higgs
Oblique corrections from Light Composite Higgs Slava Rychkov (ENS Paris & CERN) with Axel Orgogozo 1111.3534 & work in progress EWPT in Standard Model M H 0.0 M W -1.2 % W 0.2 M Z 0.2 % Z 0.1 0! had 0
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 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 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 informationLittle Higgs Models Theory & Phenomenology
Little Higgs Models Theory Phenomenology Wolfgang Kilian (Karlsruhe) Karlsruhe January 2003 How to make a light Higgs (without SUSY) Minimal models The Littlest Higgs and the Minimal Moose Phenomenology
More informationComposite Higgs and Flavor
Composite Higgs and Flavor Xiaohong Wu East China University of Science and Technology Seminar @ ICTS, Jun. 6, 2013 125GeV SM-like Higgs Discovered p 0 5 3-3 -5-7 -9 1 3 Combined observed γγ observed llll
More informationDouble Higgs production via gluon fusion (gg hh) in composite models
Double Higgs production via gluon fusion (gg hh) in composite models Ennio Salvioni CERN and University of Padova based on work in collaboration with C.Grojean (CERN), M.Gillioz (Zürich), R.Gröber and
More informationHiggs Property Measurement with ATLAS
Higgs Property Measurement with ATLAS Haijun Yang (on behalf of the ATLAS) Shanghai Jiao Tong University Hadron Collider Physics Symposium HCP 2012, Kyoto University, Japan November 12-16, 2012 Observation
More informationHiggs boson(s) in the NMSSM
Higgs boson(s) in the NMSSM U. Ellwanger, LPT Orsay Supersymmetry had a bad press recently: No signs for squarks/gluino/charginos/neutralinos... at the LHC Conflict (?) between naturalness and the Higgs
More informationLittle Higgs Models Status and Concepts
1/32 J. R. Reuter Little Higgs Models Heräus Seminar "Understanding the LHC", Bad Honnef, 14.02.2017 Little Higgs Models Status and Concepts Jürgen Reuter DESY JRR/Shim, in preparation; JRR/Tonini/de Vries,
More informationHiggs and Precision Electroweak Data
Higgs and Precision Electroweak Data Brian Batell University of Chicago work in progress with Stefania Gori and Lian-Tao Wang MCTP Spring Symposium on Higgs Boson Physics April 16-20, 2012 Higgs Signal
More informationATLAS+CMS Higgs run 1 Combinations
ATLAS+CMS Higgs run 1 Combinations Paolo Francavilla, on behalf of the ATLAS and CMS collaborations 7th Higgs Hunting 2016 August 31 - September 2, LPNHE Paris, France 1 Outline Higgs boson mass measurement
More informationarxiv: v1 [hep-ex] 5 Sep 2014
Proceedings of the Second Annual LHCP CMS CR-2014/199 September 8, 2014 Future prospects of Higgs Physics at CMS arxiv:1409.1711v1 [hep-ex] 5 Sep 2014 Miguel Vidal On behalf of the CMS Experiment, Centre
More informationRecent Developments in Little Higgs Searches. at LHC
SUSY 06, Newport Beach 1 Recent Developments in Little Higgs Searches at LHC presented by: F. Ledroit on behalf of the ATLAS collaboration Outline 2 The model Heavy gauge boson searches Leptonic decays
More informationMirror World and Improved Naturalness
Mirror World and Improved Naturalness Thomas Grégoire Boston University Based on hep-ph/0509242 R. Barbieri, T.G., L. Hall Mirror Worlds Motivations Originally introduced to restore parity Dark Matter
More informationHiggs Searches and Properties Measurement with ATLAS. Haijun Yang (on behalf of the ATLAS) Shanghai Jiao Tong University
Higgs Searches and Properties Measurement with ATLAS Haijun Yang (on behalf of the ATLAS) Shanghai Jiao Tong University LHEP, Hainan, China, January 11-14, 2013 Outline Introduction of SM Higgs Searches
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 informationAbdelhak DJOUADI ( LPT Orsay)
Physics at the LHC bdelhak DJOUDI ( LPT Orsay) Standard Physics at the LHC 1 The Standard Model QCD at the LHC 3 Tests of the SM at the LHC The SM Higgs at the LHC SUSY and SUSY Higgs at the LHC Physics
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 informationGeneral Composite Higgs Models
General Composite Higgs Models Marco Serone, SISSA, Trieste In collaboration with David Marzocca and Jing Shu, based on 1205.0770 1 The Higgs hunt at the LHC is quickly coming to an end A SM Higgs is ruled
More informationMeasurements of the Higgs Boson at the LHC and Tevatron
Measurements of the Higgs Boson at the LHC and Tevatron Somnath Choudhury (for the ATLAS, CMS, DØ and CDF collaborations) 44 th International Symposium on Multiparticle Dynamics 8 12 September 2014, Bologna
More informationHidden two-higgs doublet model
Hidden two-higgs doublet model C, Uppsala and Lund University SUSY10, Bonn, 2010-08-26 1 Two Higgs doublet models () 2 3 4 Phenomenological consequences 5 Two Higgs doublet models () Work together with
More informationReview of Higgs results at LHC (ATLAS and CMS results)
Review of Higgs results at LHC (ATLAS and CMS results) Università degli Studi di Genova and INFN, Genova, Italy E-mail: andrea.favareto@ge.infn.it The status of Higgs sector studies at the Large Hadron
More informationTeoria e fenomenologia dei modelli di Higgs composto. Roberto Contino - CERN
Teoria e fenomenologia dei modelli di Higgs composto Roberto Contino - CERN Part I: Quick review of the Composite Higgs Composite Higgs models [Georgi & Kaplan, `80s] EWSB sector H G G _ _ Aµ (G SM ) ψ
More informationBuried Higgs Csaba Csáki (Cornell) with Brando Bellazzini (Cornell) Adam Falkowski (Rutgers) Andi Weiler (CERN)
Buried Higgs Csaba Csáki (Cornell) with Brando Bellazzini (Cornell) Adam Falkowski (Rutgers) Andi Weiler (CERN) Rutgers University, December 8, 2009 Preview Found a SUSY model, where: Weird higgs decays
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 informationLHC Higgs Signatures from Extended Electroweak Guage Symmetry
LHC Higgs Signatures from Extended Electroweak Guage Symmetry Tomohiro Abe Tsinghua U. based on JHEP 1301 (013) 08 In collabollations with Ning Chen, Hong-Jian He Tsinghua U. HPNP013, February 15th 1.
More informationDmitri Sidorov Oklahoma State University On behalf of the ATLAS Collaboration DIS2014, 04/28/2014
Dmitri Sidorov Oklahoma State University On behalf of the ATLAS Collaboration DIS4, 4/8/4 Introduc)on We discovered a Standard Model (SM) like Higgs boson at mh=5 GeV. This is not the end of the story.
More informationExotic scalars. Stefania Gori. Second MCTP Spring Symposium on Higgs Boson Physics. The University of Chicago & Argonne National Laboratory
Exotic Exotic scalars scalars and and the the Higgs Higgs to to gamma gamma -- gamma gamma rate rate Stefania Gori The University of Chicago & Argonne National Laboratory Second MCTP Spring Symposium on
More informationPotential Discoveries at the Large Hadron Collider. Chris Quigg
Potential Discoveries at the Large Hadron Collider Chris Quigg Fermilab quigg@fnal.gov XXIII Taiwan Spring School Tainan 31 March - 3 April 2010 Electroweak theory successes Theoretical Physics Department,
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 informationComposite Higgs Overview
Composite Higgs Overview Tony Gherghetta Fundamental Composite Dynamics, IBS CTPU, Daejeon, Korea, December 6, 2017 1 IBS Daejeon - 6 December 2017 Composite Higgs New strong force with coupling, g s g
More informationHiggs Coupling Measurements!
Status, prospects, and interplay with searches for physics BSM Seminar University of California - Irvine April 23rd, 2014 Introduction Fantastic progress since discovery July 2012 Observation in three
More informationEffective Theory for Electroweak Doublet Dark Matter
Effective Theory for Electroweak Doublet Dark Matter University of Ioannina, Greece 3/9/2016 In collaboration with Athanasios Dedes and Vassilis Spanos ArXiv:1607.05040 [submitted to PhysRevD] Why dark
More informationtth searches at ATLAS and CMS Thomas CALVET for the ATLAS and CMS collaborations Stony Brook University Apr 11 th, 2018
tth searches at ATLAS and CMS Thomas CALVET for the ATLAS and CMS collaborations Stony Brook University SM@LHC2018 Apr 11 th, 2018 Cross-section (pb) The Higgs Top Sector Higgs boson discovery in 2012
More informationSearch for physics beyond the Standard Model at LEP 2
Search for physics beyond the Standard Model at LEP 2 Theodora D. Papadopoulou NTU Athens DESY Seminar 28/10/03 1 Outline Introduction about LEP Alternatives to the Higgs mechanism Technicolor Contact
More information8.882 LHC Physics. Higgs Physics and Other Essentials. [Lecture 22, April 29, 2009] Experimental Methods and Measurements
8.882 LHC Physics Experimental Methods and Measurements Higgs Physics and Other Essentials [Lecture 22, April 29, 2009] Organization Next week lectures: Monday 2pm and Tuesday 9:30am (which room?) Project
More informationHiggs: Interpretation and Implications. Marco Farina April 19, 2013
Higgs: Interpretation and Implications Marco Farina April 19, 2013 Discovery! ATLAS coll. ATLAS-CONF-2013-034. CMS coll. CMS-PAS-HIG-13-002 Data Giardino et al. 1303.3570 Giardino et al. 1303.3570 Higgs
More informationGolden SUSY, Boiling Plasma, and Big Colliders. M. Perelstein, Cornell University IPMU LHC Workshop talk, 12/18/07
Golden SUSY, Boiling Plasma, and Big Colliders M. Perelstein, Cornell University IPMU LHC Workshop talk, 12/18/07 Outline Part I: Supersymmetric Golden Region and its Collider Signature (with Christian
More informationThe first year of the LHC and Theory. G.G.Ross, Krakow, December 09
The first year of the LHC and Theory G.G.Ross, Krakow, December 09 The LHC a discovery machine The gauge sector : new gauge bosons? The maber sector : new quarks and leptons? The scalar sector : the hierarchy
More informationTwin Higgs Theories. Z. Chacko, University of Arizona. H.S Goh & R. Harnik; Y. Nomura, M. Papucci & G. Perez
Twin Higgs Theories Z. Chacko, University of Arizona H.S Goh & R. Harnik; Y. Nomura, M. Papucci & G. Perez Precision electroweak data are in excellent agreement with the Standard Model with a Higgs mass
More informationSearch for Higgs Bosons at LEP. Haijun Yang University of Michigan, Ann Arbor
Search for Higgs Bosons at LEP Haijun Yang University of Michigan, Ann Arbor L3 On behalf of the L3 Collaboration American Physical Society Meeting(APS03), Philadelphia April 5-8, 2003 OUTLINE Introduction
More informationEW phase transition in a hierarchical 2HDM
EW phase transition in a hierarchical 2HDM G. Dorsch, S. Huber, K. Mimasu, J. M. No ACFI workshop, UMass Amherst Phys. Rev. Lett. 113 (2014) 211802 [arxiv:1405.5537] September 18th, 2015 1 Introduction
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 informationProbing Two Higgs Doublet Models with LHC and EDMs
Probing Two Higgs Doublet Models with LHC and EDMs Satoru Inoue, w/ M. Ramsey-Musolf and Y. Zhang (Caltech) ACFI LHC Lunch, March 13, 2014 Outline 1 Motivation for 2HDM w/ CPV 2 Introduction to 2HDM 3
More informationFlavor, Minimality and Naturalness in Composite Higgs Models
eth zurich Flavor, Minimality and Naturalness in Composite Higgs Models Adrián Carmona Bermúdez Institute for Theoretical Physics, ETH Zurich In collaboration with F. Goertz A naturally light Higgs without
More informationCristiano Alpigiani Shanghai Jiao Tong University Shanghai, 18 May 2017
Searches for dark matter in ATLAS Shanghai Jiao Tong University Shanghai, 18 May 2017 Dark Matter and Particle Physics Astrophysical evidence for the existence of dark matter! First observed by Fritz Zwicky
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 informationWhy Higgs Boson Searches?
Why Higgs Boson Searches? Not just a search for a new particle... The missing piece in a spectacularly successful theory construct: the Standard Model of the fundamental interactions A massive experimental
More informationBeyond the Standard Model
Beyond the Standard Model The Standard Model Problems with the Standard Model New Physics Supersymmetry Extended Electroweak Symmetry Grand Unification References: 2008 TASI lectures: arxiv:0901.0241 [hep-ph]
More informationSearch for BSM Higgs bosons in fermion decay modes with ATLAS
Search for BSM Higgs bosons in fermion decay modes with ATLAS A. Straessner on behalf the ATLAS Collaboration FSP 103 ATLAS CC BY-SA 3.0 LHCP 2017 Shanghai May 15-20, 2017 LHCHXSWG-2015-002 arxiv:1302.7033
More informationConstraining New Models with Precision Electroweak Data
Constraining New Models with Precision Electroweak Data Tadas Krupovnickas, BNL in collaboration with Mu-Chun Chen and Sally Dawson LoopFest IV, Snowmass, 005 EW Sector of the Standard Model 3 parameters
More informationDecoupling and Alignment in Light of the Higgs Data. Howard E. Haber Pi Day, 2014 Bay Area ParCcle Physics Seminar San Francisco State Univ.
Decoupling and Alignment in Light of the Higgs Data Howard E. Haber Pi Day, 2014 Bay Area ParCcle Physics Seminar San Francisco State Univ. Outline I. IntroducCon Ø Snapshot of the LHC Higgs data Ø SuggesCons
More informationGauge-Higgs Unification on Flat Space Revised
Outline Gauge-Higgs Unification on Flat Space Revised Giuliano Panico ISAS-SISSA Trieste, Italy The 14th International Conference on Supersymmetry and the Unification of Fundamental Interactions Irvine,
More informationSearch for Fermionic Higgs Boson Decays in pp Collisions at ATLAS and CMS
Higgs boson searches in fermionic final state at LHC Search for Fermionic Higgs Boson Decays in pp Collisions at ATLAS and CMS Romain Madar on behalf of ATLAS and CMS collaboration Physikalisches Institut
More informationPHYSICS BEYOND SM AND LHC. (Corfu 2010)
PHYSICS BEYOND SM AND LHC (Corfu 2010) We all expect physics beyond SM Fantastic success of SM (LEP!) But it has its limits reflected by the following questions: What is the origin of electroweak symmetry
More informationSearches for electroweak production of supersymmetric gauginos and sleptons with the ATLAS detector
Searches for electroweak production of supersymmetric gauginos and sleptons with the ATLAS detector Christopher Bock on behalf of the ATLAS Collaboration SUSY5 - August 7, 5 Introduction Outline Introduction
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 informationEW Naturalness in Light of the LHC Data. Maxim Perelstein, Cornell U. ACP Winter Conference, March
EW Naturalness in Light of the LHC Data Maxim Perelstein, Cornell U. ACP Winter Conference, March 3 SM Higgs: Lagrangian and Physical Parameters The SM Higgs potential has two terms two parameters: Higgs
More informationNew Phenomenology of Littlest Higgs Model with T-parity
New Phenomenology of Littlest Higgs Model with T-parity Alexander Belyaev Michigan State University A.B., C.-R. Chen, K. Tobe, C.-P. Yuan hep-ph/0609179 A.B., A. Pukhov, C.-P. Yuan hep-ph/07xxxxx UW-Madison,
More informationThe electroweak fit at NNLO and prospects for LHC and ILC. Klaus Mönig
The electroweak fit at NNLO and prospects for LHC and ILC Klaus Mönig The idea of electroweak fits Electroweak interactions are the puzzling part of the Standard Model: parity (and CP) violation non-trivial
More informationJ. C. Vasquez CCTVal & USM
Maorana Higgses at Colliders arxiv:1612.06840 J. C. Vasquez CCTVal & USM ( Work in collaboration with F. esti and M. emevsek) University of Massachusetts, October 2017 Outline The minimal LR model Decay
More informationSummary Introduction Description of the Resonances s-channel Processes Fusion Processes Drell-Yan Processes Conclusions
Prospective Study on Muon Colliders Strong Electroweak Symmetry Breaking at Muon Colliders Roberto Casalbuoni Firenze and Geneva Universities with A. Deandrea, S. De Curtis, D. Dominici, R. Gatto and J.F.
More informationSearch for a heavy scalar boson decaying into a pair of Z bosons in the 2l2ν final state in CMS
Search for a heavy scalar boson decaying into a pair of Z bosons in the 2l2ν final state in CMS Li Yuan Beihang University CLHCP 2016 December 18, 2016 1 Outline Introduction Overview Analysis Strategy
More informationThe Super-little Higgs
The Super-little Higgs Csaba Csaki (Cornell) with Guido Marandella (UC Davis) Yuri Shirman (Los Alamos) Alessandro Strumia (Pisa) hep-ph/0510294, Phys.Rev.D73:035006,2006 Padua University, July 4, 2006
More informationRicerca di nuova fisica a HERA
Ricerca di nuova fisica a HERA Incontro sulla Fisica delle Alte Energie, Lecce 23-26 aprile 2003 S.Dusini, INFN Padova 1 Overview Introduction to Hera Results from HERA I Contact Interaction: Compositness,
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 informationSearch strategies for vector-like quark partners at LHC run-ii
EPJ Web of Conferences will be set by the publisher DOI: will be set by the publisher c Owned by the authors, published by EDP Sciences, 26 Search strategies for vector-like quark partners at LHC run-ii
More informationDark matter and collider signatures from extra dimensions
KAIST TF, A. Menon, Z. Sullivan, PRD 86 (2012) 093006 L. Edelhäuser, TF, M. Krämer, JHEP 1308 (2013) 091 TF, KC Kong, SC Park, JHEP 1305 (2013) 111, arxiv:1309.xxxx COSMO 2013, Cambridge Outline Universal
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 informationSearch for single production of vector-like quarks decaying into a W-boson and a b-quark at 13 TeV
SNSN-33-63 November 0 06 Search for single production of vector-like quarks decaying into a W-boson and a b-quark at 3 TeV Dustin Biedermann on behalf of the ATLAS Collaboration Institut für Physik Humboldt-Universität
More informationThe Higgs discovery - a portal to new physics
The Higgs discovery - a portal to new physics Department of astronomy and theoretical physics, 2012-10-17 1 / 1 The Higgs discovery 2 / 1 July 4th 2012 - a historic day in many ways... 3 / 1 July 4th 2012
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 informationExploring Universal Extra-Dimensions at the LHC
Exploring Universal Extra-Dimensions at the LHC Southampton University & Rutherford Appleton Laboratory 1 Problems to be addressed by the underlying theory The Nature of Electroweak Symmetry Breaking The
More informationHiggs prospects at the LHC
Higgs prospects at the LHC Marta Felcini IFCA, Santander LHCPhenoNet Kick-off meeting 1-4 February 2011, Valencia, Spain 1 LHC Status and Plans 2 LHC Integrated Luminosity in 2010 >50% of data collected
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 informationLooking through the Higgs portal with exotic Higgs decays
Looking through the Higgs portal with exotic Higgs decays Jessie Shelton University of Illinois, Urbana-Champaign Unlocking the Higgs Portal (U. Mass. Amherst) May 1, 2014 A light SM-like Higgs is narrow
More informationMeasurement of the Higgs Couplings by Means of an Exclusive Analysis of its Diphoton decay
Measurement of the Higgs Couplings by Means of an Exclusive Analysis of its Diphoton decay i.e. what do we know about the Higgs Marco Grassi The Discovery of a New Boson Evidence of a new boson with 5
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 informationProbing Dark Matter at the LHC
July 15, 2016 PPC2016 1 Probing Dark Matter at the LHC SM SM DM DM Search for production of DM particles from interacting SM particles Models tested at ATLAS assume DM WIMP Infer DM production through
More informationPhysics at TeV Energy Scale
Physics at TeV Energy Scale Yu-Ping Kuang (Tsinghua University) HEP Society Conference, April 26, 2008, Nanjing I. Why TeV Scale Is Specially Important? SM is SU(3) c SU(2) U(1) gauge theory. M g, M γ
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 informationTop quark at LHC. M. Villa. Bologna, oggi
Top quark at LHC M. Villa Bologna, oggi 1 Outline Top quark characteristics Top production and decay Measurements 2 Outline Top quark characteristics Top production and decay Measurements 3 Top quark I.D.
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 informationCharged Higgs Beyond the MSSM at the LHC. Katri Huitu University of Helsinki
Charged Higgs Beyond the MSSM at the LHC Katri Huitu University of Helsinki Outline: Mo;va;on Charged Higgs in MSSM Charged Higgs in singlet extensions H ± à aw ± Charged Higgs in triplet extensions H
More informationWZ di-boson production at CMS
WZ di-boson production at CMS 1 Outline Physics motivations Existing results (Tevatron s = 1.96TeV) Existing prospects for CMS at s = 14TeV Preliminary prospects for CMS at s = 7TeV 2 WZ Physics motivation
More informationThe Higgs boson. as a window to Beyond the Standard Model Physics. Roberto Contino. Università di Roma La Sapienza
The Higgs boson as a window to Beyond the Standard Model Physics Roberto Contino Università di Roma La Sapienza 1. what have we discovered so far...... and why we need an EWSB sector The physics discovered
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 informationHiggs couplings Beyond the Standard Model
25 th Rencontres de Blois 2013 Higgs couplings Beyond the Standard Model based on arxiv:1210.8120 Guillaume Drieu La Rochelle drieu@ipnl.in2p3.fr IPN, Lyon, France May 29, 2013 G. Drieu La Rochelle Higgs
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 informationT -Parity in Little Higgs Models a
T -Parity in Little Higgs Models a David Krohn a Based on arxiv:0803.4202 [hep-ph] with Itay Yavin, and work in progress with I.Y., Lian-Tao Wang, and Hsin-Chia Cheng Outline Review of little Higgs models
More information