Non-equilibrium QFT Applied to Electroweak Baryogenesis
Non-equilibrium QFT Applied to Electroweak Baryogenesis
Non-equilibrium QFT Applied to Electroweak Baryogenesis
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<strong>Non</strong>-Equilibrium Quantum Field Theory<br />
<strong>Applied</strong> <strong>to</strong> <strong>Electroweak</strong> <strong>Baryogenesis</strong><br />
Chris<strong>to</strong>pher Lee<br />
Institute for Nuclear Theory,<br />
University of Washing<strong>to</strong>n<br />
With<br />
Vincenzo Cirigliano<br />
Michael Ramsey-Musolf<br />
and Sean Tulin<br />
California Institute of Technology
Outline<br />
Closed Time-Path Formalism<br />
Quantum Transport Equations<br />
Solution for Baryon Asymmetry
Goal<br />
Derive transport equations for particle<br />
densities:<br />
Thermal expectation values of currents:<br />
where<br />
Bosons<br />
Fermions
<strong>Non</strong><strong>equilibrium</strong> <strong>QFT</strong><br />
Consider a matrix element:<br />
In <strong>equilibrium</strong> T=0<br />
field theory:<br />
<strong>Non</strong>-adiabaticity<br />
Degeneracy
<strong>Non</strong><strong>equilibrium</strong> <strong>QFT</strong><br />
Consider a matrix element:<br />
“path-ordering”<br />
+<br />
–<br />
x 0
Green’s s Functions<br />
<br />
Four possible Green’s functions on con<strong>to</strong>ur:<br />
x 0
Schwinger-Dyson Equations<br />
Apply <strong>to</strong> both sides:
Quantum Transport Equations<br />
<br />
Subtract resulting equations, take “
Examples of Self-Energies<br />
<br />
Fermion and scalar interactions with Higgs vevs, Higgs<br />
particles, and Higgsinos<br />
CP<br />
CP<br />
CP<br />
(In progress!)
Example: The Squark Source<br />
Riot<strong>to</strong><br />
CP-violating contribution <strong>to</strong> source:<br />
“Decoherence”<br />
ε d<br />
Resonant enhancement<br />
when<br />
“Plasma”<br />
ε p
Example: The Squark Source<br />
CP-conserving contribution <strong>to</strong> source:<br />
Cirigliano,<br />
CL,<br />
Ramsey-<br />
Musolf<br />
Keep chemical potential <strong>to</strong> first order in<br />
ε µ<br />
ε p<br />
Resonant enhancement<br />
when
Solving the Diffusion Equations<br />
<br />
Coupled transport equations for particle densities:<br />
e.g.<br />
In progress:<br />
cf. Huet,<br />
Nelson<br />
(semiclassical)<br />
• CTP calculation of Γ Y<br />
• Including all relevant<br />
linear combs. of densities<br />
• Numerical solution of<br />
coupled equations
Solution for Baryon Density<br />
Insert solution for<br />
in<strong>to</strong> equation for<br />
Baryon density left over inside bubble of broken<br />
EW phase:<br />
(constant)<br />
Resonant enhancements of relaxation terms mitigate<br />
but do not cancel out those of CP-violating sources
The Future of <strong>Baryogenesis</strong><br />
More complete, consistent calculation of BAU<br />
with non-<strong>equilibrium</strong> <strong>QFT</strong><br />
Experimental searches for EDMs, new particles<br />
? ?<br />
Where will<br />
the bands<br />
move?<br />
?<br />
CMB BBN<br />
?<br />
d e<br />
BAU<br />
d e<br />
d n<br />
BAU<br />
d Hg<br />
d Hg<br />
d n