Edinburgh Research Archive >
Physics, School of >
Physics thesis and dissertation collection >
Please use this identifier to cite or link to this item:
|Title: ||Proton decay matrix elements from lattice QCD|
|Authors: ||Cooney, Paul|
|Issue Date: ||2010|
|Publisher: ||The University of Edinburgh|
|Abstract: ||We present results for the matrix elements relevant for proton decay in Grand Unified Theories
(GUTs), using two methods. In the indirect method, we rely on an effective field theory description
of proton decay, where we need to estimate two low energy constants. We then relate
these low energy constants to the proton decay matrix elements using leading order chiral perturbation
theory. In the direct method, we calculate the required matrix elements directly; this
is computationally more expensive, but the calculation has no systematic error from the use of
chiral perturbation theory.
The calculations are performed with 2+1 flavors of domain wall fermions on lattices of size
163 × 32 and 243 × 64 with a fifth dimension of length 16. We work at fixed inverse lattice
spacing, a−1 = 1.73(3) GeV, leading to physical volumes of (1.8 fm)3 and (2.7 fm)3 for the
163 × 32 and 243 × 64 lattices respectively.
In the first four chapters we present the background theory. We start with a brief review of
the standard model and the motivation for GUTs. We show that GUTs must lead to proton
decay, and that the proton lifetime is an experimentally testable prediction which can be used
to constrain GUT parameters, or rule out classes of GUT which predict a minimum lifetime
shorter than the experimental minimum bound. We then review continuum and lattice QCD,
including outlines of the lattice methods used to calculate the proton decay matrix elements.
In the last three chapters we present the results and analysis. We calculate the nucleon and
pion two–point correlation functions, and determine their ground state masses and amplitudes.
These quantities will then be used to calculate the matrix elements using the indirect and direct
methods outlined above. The matrix elements can then be combined with experimental bounds
on the proton lifetime to bound parameters of individual GUTs.|
|Keywords: ||Grand Unified Theories|
|Appears in Collections:||Physics thesis and dissertation collection|
Items in ERA are protected by copyright, with all rights reserved, unless otherwise indicated.