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GAUGE MODEL OF UNPARTICLES Discovering the Unexpected

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Title: GAUGE MODEL OF UNPARTICLES Discovering the Unexpected


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GAUGE MODEL OF UNPARTICLESDiscovering the
Unexpected
  • Gennady A. Kozlov
  • Bogolyubov Laboratory of Theoretical Physics
  • JINR, Dubna

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Mediators, M
SM, m
CFT, m0
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  • The very high energy theory contains the fields
    of the SM and Banks-Zaks fields of a theory with
    a nontrivial IR fixed point.

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CONFORMAL INVARIANCE
  • At the quantum level, dimensionless couplings
    depend on scale renormalization group evolution
  • QED
    QCD
  • are not conformal
    theories

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g
Q
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CONFORMAL Symmetry Breaking High energy scale
  • 3 characteristic scales
  • -Hidden sector couples at M
  • Conformal
  • - EWSB CSB at

g
Q
LU
M
  • Unparticle physics is only possible in the
    conformal window
  • Width of this window depends on

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UNPARTICLE PHASE SPACE
  • The density of unparticle final states is the
    spectral density
  • Scale invariance ?
  • This is similar to the phase space for n massless
    particles
  • Unparticle with dU 1 is a massless particle.
    Unparticles with some other dimension dU look
    like a non-integral number dU of massless
    particles Georgi (2007)

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TOP-quark DECAY
  • Consider t ? u U decay through

Georgi (2007)
  • For dU ? 1, recover 2-body decay kinematics,
    monoenergetic u- jet.
  • For dU gt 1, however, get continuum of energies
    unparticle does not have a definite mass

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TOP-quark DECAY
  • Consider t ? u U decay through

Georgi (2007)
  • For dU ? 1, recover 2-body decay kinematics,
    monoenergetic u- jet.
  • For 2gtdU gt 1, however, get continuum of energies
    unparticle does not have a definite mass

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3 POINT COUPLINGS
  • 3-point coupling is determined, up to a constant,
    by conformal invariance
  • E.g., LHC gg ? O ? O O ? gggg
  • Rate controlled by value of the (strong)
    coupling, constrained only by experiment
  • Many possibilities ggZZ, ggee, ggmm,

Photon pT
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UNPARTICLE INTERACTIONS
  • Interactions depend on the dimension of the
    unparticle operator and whether it is scalar,
    vector, tensor,
  • Super-renormalizable couplings Most important
    (model will follow)

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SUMMARY. For experimentalists
  • Unparticles conformal energy window implies high
    energy colliders are the most useful machines
  • Real unparticle production ? missing energy
  • As for of the SM particles is concerned,
    - staff production looks the same as production
    of massless particles
  • Multi-unparticle production ? spectacular signals
  • Virtual unparticle production ? rare processes
  • Unparticles Quite distinguishable from other HE
    physics through own specific kinematic properties
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