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Chiral Symmetries and Low Energy Searches for New Physics

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Title: Chiral Symmetries and Low Energy Searches for New Physics


1
Chiral Symmetries and Low Energy Searches for New
Physics
M.J. Ramsey-Musolf Caltech Wisconsin-Madison
2
Fundamental Symmetries Cosmic History
  • What were the fundamental symmetries that
    governed the microphysics of the early
    universe?
  • Were there additional (broken) chiral
    symmetries?
  • What insights can low energy (E ltlt MZ) precision
    electroweak studies provide?
  • How does the approximate chiral symmetry of
    QCD the affect low energy search for
    new symmetries?

3
Fundamental Symmetries Cosmic History
4
Fundamental Symmetries Cosmic History
Puzzles the Standard Model cant solve
  • Origin of matter
  • Unification gravity
  • Weak scale stability
  • Neutrinos

What are the symmetries (forces) of the early
universe beyond those of the SM?
5
What are the new fundamental symmetries?
Two frontiers in the search
Collider experiments (pp, ee-, etc) at higher
energies (E gtgt MZ)
Indirect searches at lower energies (E lt MZ) but
high precision
Particle, nuclear atomic physics
High energy physics
6
What are the new fundamental symmetries?
  • Why is there more matter than antimatter in the
    present universe?
  • What are the unseen forces that disappeared from
    view as the universe cooled?
  • What are the masses of neutrinos and how have
    they shaped the evolution of the universe?

Electric dipole moment dark matter searches
Precision electroweak weak decays e- scattering
Neutrino interactions 0nbb-decay
Tribble report
7
Fundamental Symmetries Cosmic History
Baryogenesis When? SUSY? Neutrinos? CPV?
WIMPy D.M. Related to baryogenesis?
New gravity? Grav baryogenesis?
?
8
What is the origin of baryonic matter ?
9
EDM Probes of New CP Violation
10
Baryogenesis New Electroweak Physics
90s Cohen, Kaplan, Nelson
Joyce, Prokopec, Turok
Unbroken phase
CP Violation
11
Baryogenesis Dark Matter SUSY
12
Baryogenesis Dark Matter SUSY
Chargino Mass Matrix
Neutralino Mass Matrix
13
EDM constraints SUSY CPV
14
Dark Matter Future Experiments
15
Precision Ewk Probes of New Symmetries
Unseen Forces Supersymmetry ?
  • Unification gravity
  • Weak scale stability
  • Origin of matter
  • Neutrinos

16
Weak decays new physics
See Moulson, Cirigliano
17
Weak decays SUSY
18
Weak decays SUSY Correlations
SUSY loop-induced operators
with mixing between L,R chiral supermultiplets
19
Pion leptonic decay SUSY
A non-zero DNEW would shift Fp
20
Pion leptonic decay SUSY
21
Lepton Scattering New Symmetries
Parity-Violating electron scattering
22
Probing SUSY with PV eN Interactions
Kurylov, Su, MR-M
23
Probing SUSY with PV eN Interactions
Kurylov, R-M, Su
??? SUSY dark matter
??? SUSY dark matter
24
Fundamental Symmetries Cosmic History
Neutrinos ?
LFV LNV ?
Are they their own antiparticles? Why are their
masses so small? Can they have magnetic
moments? Implications of mn for neutrino
interactions ?
25
Neutrino Mass Magnetic Moments
Bell, Cirigliano, Gorshteyn,R-M, Vogel, Wang,
Wise Davidson, Gorbahn, Santamaria
How large is mn ?
Experiment mn lt (10-10 - 10-12) mB e
scattering, astro limits
Radiatively-induced mn
Both operators chiral odd
26
Muon Decay Neutrino Mass
27
Correlations in Muon Decay mn
Model Independent Analysis
2005 Global fit Gagliardi et al.
Model Dependent Analysis
28
Neutrino Mass 0n bb - decay
29
Neutrino Mass 0n bb - decay
30
Neutrino Mass 0n bb - decay
Prezeau, R-M, Vogel
31
Conclusions
  • Low energy probes of physics beyond the SM give
    us a unique window on the fundamental symmetries
    of the early universe that complements direct
    searches for new physics at colliders
  • These symmetries - including broken chiral
    symmetries - are needed to explain the origin of
    matter, provide for stability of the electroweak
    scale, incorporate new forces implied by
    unification, and account for the properties of
    neutrinos
  • The broken chiral symmetry of QCD also provides
    an important tool for sharpening Standard Model
    predictions for low energy observables and making
    any deviations interpretable in terms of new
    symmetries
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