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FCNC,LFV EDMFocus Point, SplitSupersymmety)dγµ es

Hidden sector Z~θθFGUT Hidden sectorGaugemediation

Ψ/ MθθGUTMM 1 /α M 2 /α M 3 /α M 1 M 2 M 3

Radiative Symmetry breakingHiggs mass GUT scale EW- L+R)+µ(R or L) = GUT scale EW+ - L or R)-

Super Higgs

Higgs

Really HiddensectorF 0Hidden sectorFMessenger sectorMGravitino mass bySuperhiggsMechanism F/Mor F 0 /Mmassless golostinoMSSM sectorM(SUSY)=F/M

LBHiggsR→→HR=1)Q L R=1)RU(1)Discrete LSPU R R=1)Q L R=1)U R R=1)x10 -29

SUGRAParameterS.Asai 2003JPS meeting

New Physics S.Asai JPS)

˜g˜χ 0 4, ˜χ + 2 ∼ ˜H + ɛ ˜W˜H˜χ 0 2, ˜χ + 1 ∼ ˜W˜χ 0 1 ∼ ˜Bsquark , slepton˜q˜lL , ˜ν L˜t, ˜b˜lR˜q, ˜l, ˜ν• m(squark) 500GeV, m(wino)200GeV P T =200GeV M = √ m 2 + p 2 + p → p = M 2 − m 22M• m(wino) 200GeV m(slepton)150 GeV-> PTGeV• P T =100GeVm 0 ≪ M 1/2 m 0 ≫ M 1/2

• LSP• QCDPT P T j > 100 GeV + 3 jet with P T jiE T (miss) > max(100GeV, 0.2M eff )M eff = ∑ |P T i | + P T (miss)q 1> 50 GeVp 1 p 2Q = p 1 − q 1• SM BG (W, t production) : SUSY = 10 4 :1 .•

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LHC LHC reach3+$,&'45660"14)6789)!"#$%&'(')'%"*&+,'-+."+ $ , " # " + $ * " # " !'()""##" # !"##$% &% /0"12! !"#$%&'()'*+,-./'%0%-1'+*''&%2"3%2'$4').31(&'56'71'2%8%-2'(-'9:9;'8.&.#%1%&*6'

LSPPT(jll)Endpoint jllsquark

Summary of endpoint study at SPS1a(from Gjelsten et al 2003, detail will be explained on June 10. )LHC/LC reportLSP mass(

• • WMAP• •

Decoupling

•

Lightest Neutralino WHGriest, Jungman ,Kamionkowski

Summary of endpoint study at SPS1a(from Gjelsten et al 2003, detail will be explained on June 10. )LHC/LC reportLSP mass, dark matter massHeavier ino mass M, μ(mixing angles)bulk contribution(co-annihilation is not easy for LHC)