On the Flavor Problem in Strongly Coupled Theories - THEP Mainz
On the Flavor Problem in Strongly Coupled Theories - THEP Mainz
On the Flavor Problem in Strongly Coupled Theories - THEP Mainz
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UNIVERSITY OF MAINZ<br />
ABSTRACT<br />
THEORETICAL HIGH ENERGY PHYSICS (<strong>THEP</strong>)<br />
INSTITUT FÜR PHYSIK<br />
Doctor rerum naturalium<br />
by Mart<strong>in</strong> Bauer<br />
This <strong>the</strong>sis is on <strong>the</strong> flavor problem of Randall Sundrum models and <strong>the</strong>ir strongly<br />
coupled dual <strong>the</strong>ories. These models are particularly well motivated extensions of <strong>the</strong><br />
Standard Model, because <strong>the</strong>y simultaneously address <strong>the</strong> gauge hierarchy problem<br />
and <strong>the</strong> hierarchies <strong>in</strong> <strong>the</strong> quark masses and mix<strong>in</strong>gs. In order to put this <strong>in</strong>to context,<br />
special attention is given to concepts underly<strong>in</strong>g <strong>the</strong> <strong>the</strong>ories which can expla<strong>in</strong><br />
<strong>the</strong> hierarchy problem and <strong>the</strong> flavor structure of <strong>the</strong> Standard Model (SM). The<br />
AdS/CFT duality is <strong>in</strong>troduced and its implications for <strong>the</strong> Randall Sundrum model<br />
with fermions <strong>in</strong> <strong>the</strong> bulk and general bulk gauge groups is <strong>in</strong>vestigated. It will be<br />
shown that <strong>the</strong> different terms <strong>in</strong> <strong>the</strong> general 5D propagator of a bulk gauge field can<br />
be related to <strong>the</strong> correspond<strong>in</strong>g diagrams of <strong>the</strong> strongly coupled dual, which allows<br />
for a deeper understand<strong>in</strong>g of <strong>the</strong> orig<strong>in</strong> of flavor chang<strong>in</strong>g neutral currents generated<br />
by <strong>the</strong> exchange of <strong>the</strong> Kaluza Kle<strong>in</strong> excitations of <strong>the</strong>se bulk fields.<br />
In <strong>the</strong> numerical analysis, different observables which are sensitive to corrections from<br />
<strong>the</strong> tree-level exchange of <strong>the</strong>se resonances will be presented on <strong>the</strong> basis of updated<br />
experimental data from <strong>the</strong> Tevatron and LHC experiments. This <strong>in</strong>cludes electroweak<br />
precision observables, namely corrections to <strong>the</strong> S and T parameters followed by corrections<br />
to <strong>the</strong> Zb ¯ b vertex, flavor chang<strong>in</strong>g observables with flavor changes at one<br />
vertex, viz. B(Bd → µ + µ − ) and B(Bs → µ + µ − ), and two vertices, viz. Sψφ and |ɛK|,<br />
as well as bounds from direct detection experiments.<br />
The analysis will show that all of <strong>the</strong>se bounds can be brought <strong>in</strong> agreement with a<br />
new physics scale ΛNP <strong>in</strong> <strong>the</strong> TeV range, except for <strong>the</strong> CP violat<strong>in</strong>g quantity |ɛK|,<br />
which requires ΛNP = O(10) TeV <strong>in</strong> <strong>the</strong> absence of f<strong>in</strong>e-tun<strong>in</strong>g. The numerous modifications<br />
of <strong>the</strong> Randall Sundrum model <strong>in</strong> <strong>the</strong> literature, which try to attenuate this<br />
bound are reviewed and categorized.<br />
Subsequently, a novel solution to this flavor problem, based on an extended color<br />
gauge group <strong>in</strong> <strong>the</strong> bulk and its thorough implementation <strong>in</strong> <strong>the</strong> RS model, will be<br />
presented, as well as an analysis of <strong>the</strong> observables mentioned above <strong>in</strong> <strong>the</strong> extended<br />
model. This solution is especially motivated from <strong>the</strong> po<strong>in</strong>t of view of <strong>the</strong> strongly<br />
coupled dual <strong>the</strong>ory and <strong>the</strong> implications for strongly coupled models of new physics,<br />
which do not possess a holographic dual, are exam<strong>in</strong>ed.<br />
F<strong>in</strong>ally, <strong>the</strong> top quark plays a special role <strong>in</strong> models with a geometric explanation of<br />
flavor hierarchies and <strong>the</strong> predictions <strong>in</strong> <strong>the</strong> Randall-Sundrum model with and without<br />
<strong>the</strong> proposed extension for <strong>the</strong> forward-backward asymmetry At FB <strong>in</strong> top pair<br />
production are computed.