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@ARTICLE{Bagnaschi:394088,
      author       = {Bagnaschi, Emanuele and Sakurai, K. and Borsato, M. and
                      Buchmueller, O. and Citron, M. and Costa, J. and De Roeck,
                      A. and Dolan, M. J. and Ellis, J. R. and Flächer, H. and
                      Heinemeyer, S. and Lucio, M. and Santos, D. Martínez and
                      Olive, K. A. and Richards, A. and Spanos, V. C. and
                      Fernández, I. Suárez and Weiglein, G.},
      title        = {{L}ikelihood {A}nalysis of the p{MSSM}11 in {L}ight of
                      {LHC} 13-{T}e{V} {D}ata},
      reportid     = {PUBDB-2017-11875, KCL-PH-TH-2017-22. CERN-PH-TH-2017-087.
                      DESY-17-059. IFT-UAM-CSIC-17-035. FTPI-MINN-17-17.
                      UMN-TH-3701-17. arXiv:1710.11091},
      year         = {2017},
      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 $(g-2)_{\mu}$ 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 $m_{\tilde{q}}$ and a distinct
                      third-generation squark mass $m_{\tilde{q}_3}$, a common
                      mass for the first-and second-generation sleptons $m_{\tilde
                      l}$ and a distinct third-generation slepton mass $m_{\tilde
                      \tau}$, a common trilinear mixing parameter $A$, the Higgs
                      mixing parameter $\mu$, the pseudoscalar Higgs mass $M_A$
                      and $\tan\beta$. In the fit including $(g-2)_{\mu}$, a
                      Bino-like $\tilde\chi^0_1$ is preferred, whereas a
                      Higgsino-like $\tilde \chi^0_1$ is favoured when the
                      $(g-2)_{\mu}$ 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, $\tilde\chi^0_1$, into the range indicated by
                      cosmological data. In the fit including $(g-2)_{\mu}$,
                      coannihilations with $\tilde \chi^0_2$ and the Wino-like
                      $\tilde\chi^{\pm}_1$ or with nearly-degenerate first- and
                      second-generation sleptons are favoured, whereas
                      coannihilations with the $\tilde \chi^0_2$ and the
                      Higgsino-like $\tilde\chi^{\pm}_1$ or with first- and
                      second-generation squarks may be important when the
                      $(g-2)_{\mu}$ constraint is dropped. Prospects remain for
                      discovering strongly-interacting sparticles at the LHC as
                      well as for discovering electroweakly-interacting sparticles
                      at a future linear $e^+ e^-$ collider such as the ILC or
                      CLIC.},
      keywords     = {family: 3 (autogen) / slepton: mass (autogen) / squark:
                      mass (autogen) / Higgs particle: mass (autogen) / gaugino:
                      mass (autogen) / dark matter: scattering (autogen) /
                      magnetic moment (autogen) / CERN LHC Coll (autogen) /
                      sparticle (autogen) / mixing (autogen) / minimal
                      supersymmetric standard model (autogen) / relic density
                      (autogen) / pseudoscalar (autogen) / accelerator (autogen) /
                      frequentist (autogen) / neutralino (autogen) / CERN CLIC
                      (autogen) / ILC Coll (autogen)},
      cin          = {T},
      cid          = {I:(DE-H253)T-20120731},
      pnm          = {611 - Fundamental Particles and Forces (POF3-611) / SFB 676
                      B08 - Globale SM + BSM Fits mit Resultaten vom LHC und
                      anderen Experimenten (B08) (87303299) / INDIGO-DataCloud -
                      INtegrating Distributed data Infrastructures for Global
                      ExplOitation (653549) / BSMFLEET - Challenging the Standard
                      Model using an extended Physics program in LHCb (639068) /
                      HIGGSTOOLS - The Higgs quest - exploring electroweak
                      symmetry breaking at the LHC (316704)},
      pid          = {G:(DE-HGF)POF3-611 / G:(GEPRIS)87303299 /
                      G:(EU-Grant)653549 / G:(EU-Grant)639068 /
                      G:(EU-Grant)316704},
      experiment   = {EXP:(DE-MLZ)NOSPEC-20140101},
      typ          = {PUB:(DE-HGF)25 / PUB:(DE-HGF)29},
      eprint       = {1710.11091},
      howpublished = {arXiv:1710.11091},
      archivePrefix = {arXiv},
      SLACcitation = {$\%\%CITATION$ = $arXiv:1710.11091;\%\%$},
      doi          = {10.3204/PUBDB-2017-11875},
      url          = {https://bib-pubdb1.desy.de/record/394088},
}