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Likelihood analysis of the pMSSM11 in light of LHC 13-TeV data.
Bagnaschi, E; Sakurai, K; Borsato, M; Buchmueller, O; Citron, M; Costa, J C; De Roeck, A; Dolan, M J; Ellis, J R; Flächer, H; Heinemeyer, S; Lucio, M; Martínez Santos, D; Olive, K A; Richards, A; Spanos, V C; Suárez Fernández, I; Weiglein, G.
Afiliação
  • Bagnaschi E; 1DESY, Notkestraße 85, 22607 Hamburg, Germany.
  • Sakurai K; 2Faculty of Physics, Institute of Theoretical Physics, University of Warsaw, ul. Pasteura 5, 02-093 Warsaw, Poland.
  • Borsato M; 3Instituto Galego de Física de Altas Enerxías, Universidade de Santiago de Compostela, Santiago de Compostela, Spain.
  • Buchmueller O; 4High Energy Physics Group, Blackett Laboratory, Imperial College, Prince Consort Road, London, SW7 2AZ UK.
  • Citron M; 4High Energy Physics Group, Blackett Laboratory, Imperial College, Prince Consort Road, London, SW7 2AZ UK.
  • Costa JC; 4High Energy Physics Group, Blackett Laboratory, Imperial College, Prince Consort Road, London, SW7 2AZ UK.
  • De Roeck A; 5Experimental Physics Department, CERN, 1211 Geneva 23, Switzerland.
  • Dolan MJ; 6Antwerp University, 2610 Wilrijk, Belgium.
  • Ellis JR; 7ARC Centre of Excellence for Particle Physics at the Terascale, School of Physics, University of Melbourne, 3010 Melbourne, Australia.
  • Flächer H; 8Theoretical Particle Physics and Cosmology Group, Department of Physics, King's College London, London, WC2R 2LS UK.
  • Heinemeyer S; 9National Institute of Chemical Physics and Biophysics, Rävala 10, 10143 Tallinn, Estonia.
  • Lucio M; 10Theoretical Physics Department, CERN, 1211 Geneva 23, Switzerland.
  • Martínez Santos D; 11H.H. Wills Physics Laboratory, University of Bristol, Tyndall Avenue, Bristol, BS8 1TL UK.
  • Olive KA; 12Campus of International Excellence UAM+CSIC, Cantoblanco, 28049 Madrid, Spain.
  • Richards A; 13Instituto de Física Teórica UAM-CSIC, C/ Nicolas Cabrera 13-15, 28049 Madrid, Spain.
  • Spanos VC; 14Instituto de Física de Cantabria (CSIC-UC), Avda. de Los Castros s/n, 39005 Santander, Spain.
  • Suárez Fernández I; 3Instituto Galego de Física de Altas Enerxías, Universidade de Santiago de Compostela, Santiago de Compostela, Spain.
  • Weiglein G; 3Instituto Galego de Física de Altas Enerxías, Universidade de Santiago de Compostela, Santiago de Compostela, Spain.
Eur Phys J C Part Fields ; 78(3): 256, 2018.
Article em En | MEDLINE | ID: mdl-31258409
ABSTRACT
We use MasterCode to perform a frequentist analysis of the constraints on a phenomenological MSSM model with 11 parameters, the pMSSM11, including constraints from ∼ 36 /fb of LHC data at 13 TeV and PICO, XENON1T and PandaX-II searches for dark matter scattering, as well as previous accelerator and astrophysical measurements, presenting fits both with and without the ( g - 2 ) µ constraint. The pMSSM11 is specified by the following parameters 3 gaugino masses M 1 , 2 , 3 , a common mass for the first-and second-generation squarks m q ~ and a distinct third-generation squark mass m q ~ 3 , a common mass for the first-and second-generation sleptons m ℓ ~ and a distinct third-generation slepton mass m τ ~ , a common trilinear mixing parameter A, the Higgs mixing parameter µ , the pseudoscalar Higgs mass M A and tan ß . In the fit including ( g - 2 ) µ , a Bino-like χ ~ 1 0 is preferred, whereas a Higgsino-like χ ~ 1 0 is mildly favoured when the ( g - 2 ) µ constraint is dropped. We identify the mechanisms that operate in different regions of the pMSSM11 parameter space to bring the relic density of the lightest neutralino, χ ~ 1 0 , into the range indicated by cosmological data. In the fit including ( g - 2 ) µ , coannihilations with χ ~ 2 0 and the Wino-like χ ~ 1 ± or with nearly-degenerate first- and second-generation sleptons are active, whereas coannihilations with the χ ~ 2 0 and the Higgsino-like χ ~ 1 ± or with first- and second-generation squarks may be important when the ( g - 2 ) µ constraint is dropped. In the two cases, we present χ 2 functions in two-dimensional mass planes as well as their one-dimensional profile projections and best-fit spectra. Prospects remain for discovering strongly-interacting sparticles at the LHC, in both the scenarios with and without the ( g - 2 ) µ constraint, as well as for discovering electroweakly-interacting sparticles at a future linear e + e - collider such as the ILC or CLIC.

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Tipo de estudo: Qualitative_research Idioma: En Revista: Eur Phys J C Part Fields Ano de publicação: 2018 Tipo de documento: Article

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Tipo de estudo: Qualitative_research Idioma: En Revista: Eur Phys J C Part Fields Ano de publicação: 2018 Tipo de documento: Article