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Lg ̃M & LoL @ LHC JiJi Fan Yale University

Lg ̃M & LoL @ LHC JiJi Fan Yale University. w/ A.D.Simone, M.Schmaltz and W.Skiba arXiv: 0808.2052 [hep-ph]. Low-scale gaugino mediation: lots of leptons at the LHC JiJi Fan Yale University. w/ A.D.Simone, M.Schmaltz and W.Skiba

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Lg ̃M & LoL @ LHC JiJi Fan Yale University

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  1. Lg̃M & LoL @ LHC JiJi Fan Yale University w/ A.D.Simone, M.Schmaltz and W.Skiba arXiv: 0808.2052 [hep-ph]

  2. Low-scale gaugino mediation:lots of leptons at the LHCJiJi Fan Yale University w/ A.D.Simone, M.Schmaltz and W.Skiba arXiv: 0808.2052 [hep-ph]

  3. Finally the LHC starts collecting data! Supersymmetry or MSSM will be tested. • MSSM: 105 soft parameters already constrained by FCNC and CP violation and must have some “organizing principle”. • Mediation Scheme: gravity mediation, gauge mediation, anomaly mediation, gaugino mediation….

  4. Sketches of sample spectrum from different models mSugra mGMSB w/ N5=1 • Sfermions not much lighter than gauginos:

  5. Motivation • Some different spectrum?! • Scalar superpartners much lighter than gauginos? • Spectrum of low-scale gaugino mediation

  6. Gaugino Mediation(Kaplan, Kribs and Schmaltz; Chacko, Luty, Nelson and Ponton 99’) • At • m0 generated radiatively from m1/2 : threshold effects at the messenger scale; : threshold effects at the gaugino mass scale; : Log running between the two scales. • In original models,

  7. Low-scale Gaugino Mediation( Lg̃M )A.D. Simone, J.F, M. Schmaltz and W. Skiba (arXiv:0808.2052(hep-ph)) • Low messenger scale, small Log running After including color factors and the log’s, scalar masses are still smaller than gaugino masses by a factor of a few (≥ 2).

  8. Spectrum of Lg̃M • Scalar superpartners much lighter than gauginos; Colored spaticles heavier than non-colored ones. • The lightest superparners, in the mass increasing order, are the gravitino, right-handed sleptons and left-handed sleptons. • Many decay chains pass through the left-handed sleptons and end in additional leptons. Typical signal: • Also

  9. A simple modelbased on “deconstructed g̃M” (Cheng, Kaplan, Schmaltz and Skiba; Csaki, Erlich, Grojean and Kribs 01’) • Setup • At Λ~5 TeV,

  10. Assume SUSY breaking only couples to the fields charged under B gauge group. (can be realized through extra dimension setup or gauge mediation with messengers only charged under GB…). • Phenomenologically, : SU(5)B gaugino soft mass; : link fields’ soft mass; • MSSM gaugino mass: at tree-level from the mixing of A and B gauge groups In the limit mB « M (M: heavy gauge boson masses)

  11. MSSM soft scalar masses: one-loop w/ gauge multiplets and the link fields and soft mass insertions. Gaugino loop Link field loop • To have EWSB, must consider a negative 2-loop top-stop-gluino contribution to soft masses of Hu.

  12. Sample Spectrum LSP: Gravitino NLSP: τ̃R NNLSP’s: Left-handed sleptons (Similar spectrum has been obtained through warped 5D constructions: Chacko, Ponton 03’; Medina, Wagner 06’)

  13. Decay chains

  14. Cross section for squark pair production and interesting final states with multi-leptons and Higgses at the LHC; each final state includes 2j+2 stable charged tracks.

  15. Conclusions and future directions • Lg̃̃̃M predicts that sfermions much lighter than gauginos; Hallmark of Lg̃M is that both left- and right- handed sleptons are lighter than all other sparticles except the gravitino. • Study of the different signatures and the searching strategies. • Distinguishing from other models with similar spectrum: Dirac gaugino model (“supersoft models” Fox, Nelson and Weiner 02’) ; GMSB w/ a large number of messengers (>30) … • Model building issues: generate the scale dynamically; mu/Bmu; gauge coupling unification.

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