on the behaviour of composite resonances breaking lfu
play

On the behaviour of composite resonances breaking LFU Mikael Chala - PowerPoint PPT Presentation

Apr 07, 2023 •160 likes •745 views

On the behaviour of composite resonances breaking LFU Mikael Chala (IPPP) With M. Spannowsky. arXiv:1803.02364 MC4BSM, IPPP Durham, April 21, 2018 Several hints of violation of lepton fmavor universality, in particular: MC4BSM, IPPP Durham,

  1. On the behaviour of composite resonances breaking LFU Mikael Chala (IPPP) With M. Spannowsky. arXiv:1803.02364 MC4BSM, IPPP Durham, April 21, 2018

  2. Several hints of violation of lepton fmavor universality, in particular: MC4BSM, IPPP Durham, April 21, 2018

  3. Several hints of violation of lepton fmavor universality, - Very clean observable - Very clean observable in particular: - Below SM prediction - Below SM prediction in several measurements in several measurements MC4BSM, IPPP Durham, April 21, 2018

  4. Several hints of violation of lepton fmavor universality, - Very clean observable - Very clean observable in particular: - Below SM prediction - Below SM prediction in several measurements in several measurements MC4BSM, IPPP Durham, April 21, 2018

  5. Several hints of violation of lepton fmavor universality, - Very clean observable - Very clean observable in particular: - Below SM prediction - Below SM prediction in several measurements in several measurements few TeV size , so natural in other models of new physics (e.g. Composite Higgs models) MC4BSM, IPPP Durham, April 21, 2018

  6. The simplifjed Lagrangian MC4BSM, IPPP Durham, April 21, 2018

  7. The simplifjed Lagrangian Larger values in confmict with neutrino trident Smaller values disfavoured production. by [ L. Di Luzio, M. Kirk, and A. Lenz; '17] MC4BSM, IPPP Durham, April 21, 2018

  8. The simplifjed Lagrangian Larger values in confmict with neutrino trident Smaller values disfavoured production. by [ L. Di Luzio, M. Kirk, and A. Lenz; '17] MC4BSM, IPPP Durham, April 21, 2018

  9. The origin of these couplings in composite Higgs models MC4BSM, IPPP Durham, April 21, 2018

  10. The origin of these couplings in composite Higgs models 1510.07658 1503.03865 1608.02362 1611.03507 1703.06019 1712.07646 1712.02536 1508.00569 MC4BSM, IPPP Durham, April 21, 2018

  11. The composite Higgs paradigm (a high-energy copy of QCD) UV GeV scale IR MC4BSM, IPPP Durham, April 21, 2018

  12. The composite Higgs paradigm (a high-energy copy of QCD) UV quark condensate GeV scale IR MC4BSM, IPPP Durham, April 21, 2018

  13. The composite Higgs paradigm (a high-energy copy of QCD) UV quark condensate GeV scale IR MC4BSM, IPPP Durham, April 21, 2018

  14. The composite Higgs paradigm (a high-energy copy of QCD) UV quark condensate GeV scale IR MC4BSM, IPPP Durham, April 21, 2018

  15. The composite Higgs paradigm (a high-energy copy of QCD) UV TeV scale IR MC4BSM, IPPP Durham, April 21, 2018

  16. The composite Higgs paradigm (a high-energy copy of QCD) UV TeV scale IR MC4BSM, IPPP Durham, April 21, 2018

  17. The composite Higgs paradigm (a high-energy copy of QCD) UV parton condensate TeV scale IR MC4BSM, IPPP Durham, April 21, 2018

  18. The composite Higgs paradigm (a high-energy copy of QCD) UV parton condensate TeV scale IR MC4BSM, IPPP Durham, April 21, 2018

  19. The composite Higgs paradigm (a high-energy copy of QCD) UV parton condensate TeV scale IR MC4BSM, IPPP Durham, April 21, 2018

  20. The composite Higgs paradigm (a high-energy copy of QCD) UV parton condensate TeV scale IR MC4BSM, IPPP Durham, April 21, 2018

  21. The composite Higgs paradigm (a high-energy copy of QCD) UV True for all composite resonances! parton condensate TeV scale IR MC4BSM, IPPP Durham, April 21, 2018

  22. The origin of these couplings in composite Higgs models MC4BSM, IPPP Durham, April 21, 2018

  23. The origin of these couplings in composite Higgs models MC4BSM, IPPP Durham, April 21, 2018

  24. The origin of these couplings in composite Higgs models MC4BSM, IPPP Durham, April 21, 2018

  25. The origin of these couplings in composite Higgs models Breaks the shift symmetry Must be small, so M must be small too MC4BSM, IPPP Durham, April 21, 2018

  26. The origin of these couplings in composite Higgs models Breaks the shift symmetry Must be small, so M must be small too So, this channel is open! It dominates the decay width! MC4BSM, IPPP Durham, April 21, 2018

  27. Current bounds on vector-like fermions MC4BSM, IPPP Durham, April 21, 2018

  28. Current bounds on vector-like fermions Heavy quarks are produced in pairs via QCD (no model dependence) 28 MC4BSM, IPPP Durham, April 21, 2018

  29. Current bounds on vector-like fermions This is strongly infmuenced by the minimal composite Higgs model. In non-minimal composite Higgs models: 4d UV completions, DM, BAU, … and most models are non-minimal! 29 MC4BSM, IPPP Durham, April 21, 2018

  30. Current bounds on vector-like fermions This is strongly infmuenced by the minimal composite Higgs model. In non-minimal composite Higgs models: 4d UV completions, DM, BAU, … and most models are non-minimal! [ MC , 1705.03013 ] 30 MC4BSM, IPPP Durham, April 21, 2018

  31. Current bounds on vector-like fermions Heavy leptons are produced in pairs via EW interactions, so much weaker constraints [1306.1525], [1007.4206] 31 MC4BSM, IPPP Durham, April 21, 2018

  32. The origin of these couplings in composite Higgs models Breaks the shift symmetry Must be small, so M must be small too So, this channel is open! It dominates the decay width! MC4BSM, IPPP Durham, April 21, 2018

  33. The actual reach of di-muon searches MC4BSM, IPPP Durham, April 21, 2018

  34. The actual reach of Naive di-muon bound (neglecting di-muon searches heavy fermions) MC4BSM, IPPP Durham, April 21, 2018

  35. Actual di-muon The actual reach of Naive di-muon bound (neglecting bound di-muon searches heavy fermions) MC4BSM, IPPP Durham, April 21, 2018

  36. Actual di-muon The actual reach of Naive di-muon bound (neglecting bound di-muon searches heavy fermions) almost one order of magnitude MC4BSM, IPPP Durham, April 21, 2018

  37. Leptonic Z decay gives very few events, so we consider hadronic decays of: MC4BSM, IPPP Durham, April 21, 2018

  38. Event selection MC4BSM, IPPP Durham, April 21, 2018

  39. Event selection Muons with pT > 50 GeV removed from hadrons in clustering process MC4BSM, IPPP Durham, April 21, 2018

  40. Event selection Muons with pT > 50 GeV removed from hadrons in clustering process Jets are clustered with R = 1.2 MC4BSM, IPPP Durham, April 21, 2018

  41. Event selection Muons with pT > 50 GeV removed from hadrons in clustering process Jets are clustered with R = 1.2 We require, fjrst, the presence of exactly two opposite charged muons and at least one jet MC4BSM, IPPP Durham, April 21, 2018

  42. Event selection Muons with pT > 50 GeV removed from hadrons in clustering process Jets are clustered with R = 1.2 We require, fjrst, the presence of exactly two opposite charged muons and at least one jet The leading pT jet is required to have a signifjcant mass drop. It is then fjltered MC4BSM, IPPP Durham, April 21, 2018

  43. Event selection Muons with pT > 50 GeV removed from hadrons in clustering process Jets are clustered with R = 1.2 We require, fjrst, the presence of exactly two opposite charged muons and at least one jet The leading pT jet is required to have a signifjcant mass drop. It is then fjltered 0802.2470 MC4BSM, IPPP Durham, April 21, 2018

  44. Event selection Muons with pT > 50 GeV removed from hadrons in clustering process Jets are clustered with R = 1.2 We require, fjrst, the presence of exactly two opposite charged muons and at least one jet The leading pT jet is required to have a signifjcant mass drop. It is then fjltered MC4BSM, IPPP Durham, April 21, 2018

  45. Event selection Muons with pT > 50 GeV removed from hadrons in clustering process Jets are clustered with R = 1.2 We require, fjrst, the presence of exactly two opposite charged muons and at least one jet The leading pT jet is required to have a signifjcant mass drop. It is then fjltered MC4BSM, IPPP Durham, April 21, 2018

  46. MC4BSM, IPPP Durham, April 21, 2018

  47. Event selection pT muons above 200 GeV, leading jet mass in the range [80, 130] GeV MC4BSM, IPPP Durham, April 21, 2018

  48. Event selection pT muons above 200 GeV, leading jet mass in the range [80, 130] GeV MC4BSM, IPPP Durham, April 21, 2018

  49. MC4BSM, IPPP Durham, April 21, 2018

  50. Event selection We can then cut on mV and mL: MC4BSM, IPPP Durham, April 21, 2018

  51. Event selection We can then cut on mV and mL: MC4BSM, IPPP Durham, April 21, 2018

  52. Event selection We can then cut on mV and mL: MC4BSM, IPPP Durham, April 21, 2018

  53. Final results MC4BSM, IPPP Durham, April 21, 2018

  54. Final results MC4BSM, IPPP Durham, April 21, 2018

  55. Final results Assumes half of the cross section into the target fjnal state MC4BSM, IPPP Durham, April 21, 2018

  56. Conclusions Parameter space regions that were thought excluded by searches for di-muon resonances, are still allowed. They are not even ruled out by other beyond the Standard Model analyses, including multi-lepton searches for electroweakinos or heavy leptons. MC4BSM, IPPP Durham, April 21, 2018

Recommend

FORMATION OF NOVEL COMPOSITE FIBRES EXHIBITING THERMOCHROMIC BEHAVIOUR L. van der Werff 1,2,3 *,

FORMATION OF NOVEL COMPOSITE FIBRES EXHIBITING THERMOCHROMIC BEHAVIOUR L. van der Werff 1,2,3 *,

18 TH INTERNATIONAL CONFERENCE ON COMPOSITE MATERIALS FORMATION OF NOVEL COMPOSITE FIBRES EXHIBITING THERMOCHROMIC BEHAVIOUR L. van der Werff 1,2,3 *, I. L. Kyratzis 1 , A. Robinson 2 , R. Cranston 1 , G. Peeters 1 1 CSIRO Materials Science and

203 views • 5 slides
MULTI SCALE AND GEOMETRY EFFECT ON THE ELECTROMAGNETIC BEHAVIOUR OF Fe 3 O 4 /CARBON COMPOSITE

MULTI SCALE AND GEOMETRY EFFECT ON THE ELECTROMAGNETIC BEHAVIOUR OF Fe 3 O 4 /CARBON COMPOSITE

18 TH INTERNATIONAL CONFERENCE ON COMPOSITE MATERIALS MULTI SCALE AND GEOMETRY EFFECT ON THE ELECTROMAGNETIC BEHAVIOUR OF Fe 3 O 4 /CARBON COMPOSITE NANOFIBERS M. Bayat 1 , H. Yang 1 , D. Michelson 2 , F. K. Ko 1 * 1 Department of Materials

225 views • 6 slides
Emergent Electroweak Symmetry Breaking with Composite W, Z Bosons Yanou Cui Jefferson Physical

Emergent Electroweak Symmetry Breaking with Composite W, Z Bosons Yanou Cui Jefferson Physical

Introduction Model Setup Electroweak Precision Test WW Scattering Unitarity Signatures at the LHC Conclusions Emergent Electroweak Symmetry Breaking with Composite W, Z Bosons Yanou Cui Jefferson Physical Laboratory, Harvard University, USA

356 views • 17 slides
Composite Vectors and Scalars in Theories of Electroweak Symmetry Breaking Antonio Enrique C

Composite Vectors and Scalars in Theories of Electroweak Symmetry Breaking Antonio Enrique C

Composite Vectors and Scalars in Theories of Electroweak Symmetry Breaking Antonio Enrique C arcamo Hern andez. Scuola Normale Superiore di Pisa. LAPTH Seminar, 16th September of 2010. Based on: R. Barbieri, A. E. C arcamo Hern

730 views • 49 slides
Negotiation Behaviour and Breaking Deadlock Dr Karl Mackie CBE CEDR Conflict and Psychology

Negotiation Behaviour and Breaking Deadlock Dr Karl Mackie CBE CEDR Conflict and Psychology

Negotiation Behaviour and Breaking Deadlock Dr Karl Mackie CBE CEDR Conflict and Psychology Civil justice and commercial/civil The CEDR Story disputes A business disruptor campaign - Mediation vs Litigation - Mediation vs

272 views • 14 slides
IMPACT OF MECHANICAL LOADING ON THE ELECTROCHEMICAL BEHAVIOUR OF CARBON FIBERS FOR USE IN ENERGY

IMPACT OF MECHANICAL LOADING ON THE ELECTROCHEMICAL BEHAVIOUR OF CARBON FIBERS FOR USE IN ENERGY

18 TH INTERNATIONAL CONFERENCE ON COMPOSITE MATERIALS IMPACT OF MECHANICAL LOADING ON THE ELECTROCHEMICAL BEHAVIOUR OF CARBON FIBERS FOR USE IN ENERGY STORAGE COMPOSITE MATERIALS E. Jacques 1 *, M. H. Kjell 2 , D. Zenkert 1 , G. Lindbergh 2 , M.

181 views • 6 slides
Review on Hadron Spectroscopy and Spectroscopy and Resonances Resonances Chuan Liu

Review on Hadron Spectroscopy and Spectroscopy and Resonances Resonances Chuan Liu

Review on Hadron Review on Hadron Spectroscopy and Spectroscopy and Resonances Resonances Chuan Liu Introduction Chuan Liu The conventional spectrum Institute of Theoretical Physics and Center for High Energy Physics Single School of

955 views • 67 slides
Resonances in the 12 C( , ) 16 O reaction I have asked myself the question what is the

Resonances in the 12 C( , ) 16 O reaction I have asked myself the question what is the

Resonances in the 12 C( , ) 16 O reaction I have asked myself the question what is the consequences of the nuclear resonances in the proposed experiment in inverse kinematics of the capture reaction? So far, the reaction was discussed as

222 views • 10 slides
Session 14 Introduction to Behaviour that Challenges SECTION 5: 1 Behaviour Behaviour that is

Session 14 Introduction to Behaviour that Challenges SECTION 5: 1 Behaviour Behaviour that is

Session 14 Introduction to Behaviour that Challenges SECTION 5: 1 Behaviour Behaviour that is challenging We used to talk about problem behaviour or behavioural difficulties Now we see this as behaviour that challenges services.

314 views • 7 slides
Searching for graviton resonances at the LHC M.A.Parker Cambridge Extra dimension models

Searching for graviton resonances at the LHC M.A.Parker Cambridge Extra dimension models

Searching for graviton resonances at the LHC M.A.Parker Cambridge Extra dimension models can contain massive graviton resonances In some models, these resonances are well spaced in mass With universal couplings, the resonance

415 views • 19 slides
On spectral renormalization group and the theory of tion group resonances in non-relativistic

On spectral renormalization group and the theory of tion group resonances in non-relativistic

Spectral RG and resonances J er emy Faupin The model Spectral renormaliza- On spectral renormalization group and the theory of tion group resonances in non-relativistic QED Resonances and lifetime of metastable states J

1.25k views • 86 slides
EMMA MA RF System C. Ohmori and J. S. Berg EMMA MA System * Many FFAG applications require slow

EMMA MA RF System C. Ohmori and J. S. Berg EMMA MA System * Many FFAG applications require slow

EMMA MA RF System C. Ohmori and J. S. Berg EMMA MA System * Many FFAG applications require slow acceleration * Linear non-scaling FFAGs cross many resonances - Nonlinear resonances - Imperfection resonances * Resonances damage beam

594 views • 12 slides
Resonances and chaos in the dynamics of exoplanets I. I. Shevchenko Pulkovo Observatory

Resonances and chaos in the dynamics of exoplanets I. I. Shevchenko Pulkovo Observatory

Resonances and chaos in the dynamics of exoplanets I. I. Shevchenko Pulkovo Observatory Introduction The dynamics of exoplanetary systems (of both single and binary stars) is considered. An especial attention is paid to resonances and

605 views • 38 slides
Breaking out of the box Understanding rela5onships between learning and assessment Breaking

Breaking out of the box Understanding rela5onships between learning and assessment Breaking

Dr Nick Saville Breaking out of the box Understanding rela5onships between learning and assessment Breaking out of the box - a metaphor for thinking about rela5onships and interpreta5ons breaking out breaking out of the box of the

895 views • 68 slides
PROCESSING AND MECHANICAL BEHAVIOUR OF HALLOYSITE FILLED POLYAMIDE-6 NANOCOMPOSITES K.

PROCESSING AND MECHANICAL BEHAVIOUR OF HALLOYSITE FILLED POLYAMIDE-6 NANOCOMPOSITES K.

18 TH INTERNATIONAL CONFERENCE ON COMPOSITE MATERIALS PROCESSING AND MECHANICAL BEHAVIOUR OF HALLOYSITE FILLED POLYAMIDE-6 NANOCOMPOSITES K. Prashantha*, H. Schmitt, M. F. Lacrampe, P. Krawczak Ecole des Mines de Douai, Department of Polymers and

395 views • 5 slides
Fatigue and Fracture Behaviour of Al-SiC p MMC NDE by IR detection D.P.Myriounis, S.T.Hasan

Fatigue and Fracture Behaviour of Al-SiC p MMC NDE by IR detection D.P.Myriounis, S.T.Hasan

18 TH INTERNATIONAL CONFERENCE ON COMPOSITE MATERIALS Fatigue and Fracture Behaviour of Al-SiC p MMC NDE by IR detection D.P.Myriounis, S.T.Hasan Sheffield Hallam University, ACES, Engineering and Mathematics, City Campus, S1 1WB, Sheffield, UK

104 views • 6 slides
Semiclassical Resonances of Schr odinger operators as zeroes of regularized determinants

Semiclassical Resonances of Schr odinger operators as zeroes of regularized determinants

Semiclassical Resonances of Schr odinger operators as zeroes of regularized determinants Jean-Marc Bouclet Vincent Bruneau Abstract We prove that the resonances of long range perturbations of the (semiclassical) Laplacian are the

746 views • 37 slides
ANTI SOCIAL BEHAVIOUR WHAT IS ANTISOCIAL WHAT IS ANTISOCIAL BEHAVIOUR BEHAVIOUR Bullying

ANTI SOCIAL BEHAVIOUR WHAT IS ANTISOCIAL WHAT IS ANTISOCIAL BEHAVIOUR BEHAVIOUR Bullying

ANTI SOCIAL BEHAVIOUR WHAT IS ANTISOCIAL WHAT IS ANTISOCIAL BEHAVIOUR BEHAVIOUR Bullying in School & out of School Vandalism or graffiti Playing music too loudly Shouting, screaming or swearing Drinking alcohol

121 views • 10 slides
HEP seminar Josu Cantero (OSU) Heavy resonances 1 / 36 Introduction Theories beyond the

HEP seminar Josu Cantero (OSU) Heavy resonances 1 / 36 Introduction Theories beyond the

Search for heavy resonances decaying into third generation quarks with the ATLAS detector Josu Cantero (Oklahoma State University) July 15, 2020 HEP seminar Josu Cantero (OSU) Heavy resonances 1 / 36 Introduction Theories beyond the

699 views • 38 slides
DEGRADATION BEHAVIOUR OF TEXTILE-REINFORCED POLYPROPYLENE UNDER FATIGUE LOADING M. Gude, W.

DEGRADATION BEHAVIOUR OF TEXTILE-REINFORCED POLYPROPYLENE UNDER FATIGUE LOADING M. Gude, W.

18 TH INTERNATIONAL CONFERENCE ON COMPOSITE MATERIALS DEGRADATION BEHAVIOUR OF TEXTILE-REINFORCED POLYPROPYLENE UNDER FATIGUE LOADING M. Gude, W. Hufenbach, I. Koch* Institute of Lightweight Engineering and Polymer Technology, TU Dresden,

68 views • 5 slides
t n e m Behaviour Influences Behaviour u c o D y c a g e L g n i Pearlcatchers

t n e m Behaviour Influences Behaviour u c o D y c a g e L g n i Pearlcatchers

t n e m Behaviour Influences Behaviour u c o D y c a g e L g n i Pearlcatchers Ltd n r a e L Objectives Header here max 30 characters t n e m u c o Raise awareness of the importance of leadership behaviours and D

469 views • 23 slides
CHARACTERISATION OF IMPACT BEHAVIOUR OF CARBON FIBRE LAMINATES M. Mateos*, H. Zabala, J. I.

CHARACTERISATION OF IMPACT BEHAVIOUR OF CARBON FIBRE LAMINATES M. Mateos*, H. Zabala, J. I.

18 TH INTERNATIONAL CONFERENCE ON COMPOSITE MATERIALS CHARACTERISATION OF IMPACT BEHAVIOUR OF CARBON FIBRE LAMINATES M. Mateos*, H. Zabala, J. I. Mgica, L. Aretxabaleta, M. Sarrionandia Mechanical Engineering and Industrial Manufacturing

429 views • 5 slides
Weyl asymptotics of resonances and resonance states completeness for quantum graphs Igor Popov

Weyl asymptotics of resonances and resonance states completeness for quantum graphs Igor Popov

Weyl asymptotics of resonances and resonance states completeness for quantum graphs Igor Popov ITMO University St. Petersburg, Russia joint work with I.Blinova Resonances. Introduction An interesting example is given by the Helmholtz

799 views • 32 slides
MECHANICAL BEHAVIOUR OF FRP-CONFINED CONCRETE COLUMNS UNDER AXIAL COMPRESSIVE LOAD V.Tamus*,

MECHANICAL BEHAVIOUR OF FRP-CONFINED CONCRETE COLUMNS UNDER AXIAL COMPRESSIVE LOAD V.Tamus*,

18 TH INTERNATIONAL CONFERENCE ON COMPOSITE MATERIALS MECHANICAL BEHAVIOUR OF FRP-CONFINED CONCRETE COLUMNS UNDER AXIAL COMPRESSIVE LOAD V.Tamus*, V.Valdmanis Institute of Polymer Mechanics, University of Latvia, 23 Aizkraukles St., Riga,

67 views • 4 slides

More recommend