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Search for extra gauge bosons in Little Higgs Models at a linear collider

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Title: Search for extra gauge bosons in Little Higgs Models at a linear collider


1
Search for extra gauge bosons in Little Higgs
Models at a linear collider
  • Gi-Chol Cho
  • (Ochanomizu Univ.)
  • LCWS2004, Apr.21.2004
  • in collaboration with Aya Omote

2
Introduction
  • Little Higgs Model alternative candidate to
    solve the hierarchy problem
  • setup
  • global symmetry
  • local symmetry ( GSM)
  • global/local symmetries are broken
    simultaneously
  • Higgs boson ? pseudo Goldstone boson via global
    symmetry breaking
  • extra particles acquire masses sym.breaking
    scale
  • quadratic divergences of mh2 are cancelled
    _at_1-loop
  • cut-off scale O(10TeV)

3
Littlest Higgs Model (Arkani-Hamed etal.)
  • a simplest structure
  • global symmetry SU(5) ? SO(5)
  • local symmetry SU(2)xU(1)1xSU(2)xU(1)2?GSM
  • extra particles
  • triplet Higgs
  • vector-like quark (t)
  • extra gauge bosons (AH, ZH, WH)

4
Extra gauge bosons
  • before symmetry breaking
  • after symmetry breaking (SU(2)xU(1)1xSU(2)xU(1)
    2?GSM)
  • W, B massive O(f) (decay constant of pseudo
    GS)
  • EW sym. breaking
  • charged states
  • neutral states
  • Free parameters

5
Mass of extra neutral gauge bosons
  • AH is relatively lighter than the other extra
    particles because of the hypercharge coupling
  • could be as light as 1TeV in sizable parameter
    space

6
  • LHC has a detectability of TeV Z boson in some
    class of models
  • What can LC do if LHC find a Z boson (lt 1TeV)?
  • If Z mass is smaller than the CM energy of LC,
    it can be produced in s-channel
  • Can LC tell us that if discovered Z boson is in
    Littlest Higgs model or SUSY E6 models?

7
  • focus at the resonance of Z
  • high statistics
  • reduce number of parameters

8
Z bosons in SUSY E6 models
9
Z-f-f couplings
and extra fields to make a complete multiplet of
E6
10
peak cross section
  • AH gives a few times larger cross section than Z
    in E6 models
  • couplings of depend on

11
  • cross section (AH) decreases rapidly at
  • ? comparable to the other models
  • ? hard to distinguish

m500GeV
12
Forward-backward asymmetry
  • asymmetry in LHM depends charges only (not mixing
    angles)
  • ratio of left- and right-handed charges to Z
    boson determine the asymmetry

parameter rf does not depend on
13
FB asymmetry
14
why AcFB0?
10
16
5
  • E6 models extra U(1) charges of quarks/leptons
    in rep. of SU(5) are common
  • (uL, uR) belong to the 10 rep. of SU(5) ? no
    asymmetry!

15
beyond E6?
  • deviation of eL, eR charges from little higgs
    model
  • cross section 10-100pb, lt O(1) measurement may
    be possible
  • 10 deviation of the couplings can be measured?

16
Summary
  • possibility to distinguish Z boson in Littlest
    Higgs model and SUSY-E6 models are studied (after
    Z discovery at LHC)
  • peak cross section of in
    Littlest Higgs models is sizably larger than E6
    models in most of parameter space, but becomes
    comparable when
  • for b-, c-quarks are useful for our
    purpose because it is independent of
  • in E6 models because of the
    SU(5) symmetry, while it is 0.4 in Littlest Higgs
    model ? clear signal?
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