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Electric Dipole Moments and the Origin of Baryonic Matter

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Explaining non-zero rB requires CP-violation beyond that of the ... Anomalous Processes. Different vacua: D(B L)= DNCS. Kuzmin, Rubakov, Shaposhnikov McLerran, ... – PowerPoint PPT presentation

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Title: Electric Dipole Moments and the Origin of Baryonic Matter


1
Electric Dipole Moments and the Origin of
Baryonic Matter
PRD 71 075010 (2005) Caltech MAP-312 (in prep)
2
What is the origin of baryonic matter ?
3
What is the origin of baryonic matter ?
4
Baryogenesis and EDMs Theoretical Tasks
  • Attaining reliable computations that relate
    particle physics models of new CP-violation to
    EDMs of complex systems (neutron, atoms, nuclei)
  • Attaining reliable computations of the baryon
    asymmetry from fundamental particle physics
    theories with new CP-violation

Nonperturbative QCD, atomic nuclear structure
  • Non-equilibrium quantum transport
  • Non-zero T and m
  • Spacetime dynamics of cosmic phase transitions

5
Outline
6
Baryon Asymmetry of the Universe (BAU)
7
Baryogenesis Ingredients
Sakharov Criteria
  • B violation
  • C CP violation
  • Nonequilibrium dynamics

Sakharov, 1967
8
Baryogenesis Ingredients
9
Baryogenesis Ingredients
Sakharov Criteria
  • B violation
  • C CP violation
  • Nonequilibrium dynamics

Sakharov, 1967
10
Leptogenesis
11
EW Baryogenesis Standard Model
Anomalous Processes
Different vacua D(BL) DNCS
Sphaleron Transitions
12
EW Baryogenesis Standard Model
13
Baryogenesis New Electroweak Physics
Unbroken phase
CP Violation
14
EDM Probes of New CP Violation
15
Present n-EDM limit

Proposed n-EDM limit


Matter-Antimatter Asymmetry in the Universe
?
M. Pendlebury B. Filippone
n-EDM has killed more theories than any other
single experiment
16
Baryogenesis and EDMs Better Theory ?
Non-equilibrium quantum transport
RHIC
Violent departure from equilibrium
Electroweak Baryogenesis
Gentle departure from equilibrium
17
Systematic Baryogenesis
Goal Derive dependence of YB on parameters
Lnew systematically (controlled approximations)

18
Systematic Baryogenesis MSSM
LEP EWWG
See, e.g., Kang et al for U(1)
19
Systematic Baryogenesis
Cohen, Kaplan, Nelson Joyce, Prokopec,
Turok
snow
20
Systematic Baryogenesis
Riotto Carena et al Lee, Cirigliano, Tulin,
R-M
Quantum Transport Equation
Schwinger-Dyson Equations
21
Systematic Baryogenesis
Departure from equilibrium
  • Non-adiabatic evolution of states
    degeneracies
  • Non-thermal distributions

Generalized Greens Functions Closed Time Path
Exploit scale hierarchy expand in scale ratios e
22
Scale Hierarchy
Time Scales
Plasma time tP 1/GP
23
Quantum Decoherence
L
L DL
24
Scale Hierarchy
25
Quantum Transport Equations
26
EDM constraints SUSY CPV
Different choices for SUSY parameters
27
EDM constraints SUSY CPV
28
II. Theory Non-equilibrium QFT Quantum
Transport
29
Non-equilibrium Quantum Field Theory
Closed Time Path (CTP) Formulation
Conventional, T0 equilibrium field theory
30
Non-equilibrium Quantum Field Theory
Two assumptions
  • Non-degenerate spectrum
  • Adiabatic switch-on of LI

LI
31
Non-equilibrium Tgt0 Evolution
Time Scales
Plasma time tP 1/GP
32
Non-equilibrium Tgt0 Evolution
33
Non-equilibrium Tgt0 Evolution
Generalized Greens Functions
34
Non-equilibrium Tgt0 Evolution
Schwinger-Dyson Equations
A few formal manipulations
35
Quantum Transport
36
Scale Hierarchy
37
Systematic Expansion
Distribution functions
38
Systematic Expansion
Small e expansion
39
Supersymmetric Sources (mSUGRA)
40
Supersymmetric Sources (mSUGRA)
41
Supersymmetric Sources (mSUGRA)
42
Supersymmetric Sources (mSUGRA)
43
Supersymmetric Sources (mSUGRA)
44
Supersymmetric Sources (mSUGRA)
Previous work
GY gtgt G(-,)
Effect decouples
O (em ep)
45
Supersymmetric Sources (mSUGRA)
(Super) gauge interactions
46
Supersymmetric Sources (mSUGRA)
O (emep)
47
Supersymmetric Sources (mSUGRA)
Resonance Effects
48
Supersymmetric Transport Equations
Coupled Transport Equations
Baryon number production
49
Baryon Number
50
Baryon Number
51
Baryon Number GY
52
Baryon Number GY
53
III. Phenomenology
54
SUSY Inputs
55
Sources Relaxation
56
Baryon Number
57
CP Violating Phases
58
EDM Constraints
199Hg
59
Summary Outlook
  • EWB remains a viable option for explaining the
    cosmic baryon asymmetry that can be tested and
    constrained using EDMs, precision electroweak,
    and collider input
  • New developments using non-equilibrium QFT are
    putting YB computations on a more systematic
    footing that will allow for detailed
    confrontations with lab experiments
  • Considerable (hard) work remains to be completed
  • Exciting field involving an interplay between
    cosmology and particle/nuclear physics in both
    theory and experiment

Complete set of transport coefficients, refined
studies of bubble dynamics, applications to
various scenarios for new CP-violation,
phenomenology (EDM, B physics, precision
electroweak, collider)
60
Non-equilibrium Quantum Transport
61
Supersymmetric Sources (mSUGRA)
62
Supersymmetric Sources (mSUGRA)
CP Violating Source
O (edep)
63
Supersymmetric Sources (mSUGRA)
64
Supersymmetric Sources (mSUGRA)
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