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On the Flavor Problem in Strongly Coupled Theories - THEP Mainz

On the Flavor Problem in Strongly Coupled Theories - THEP Mainz

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<strong>On</strong>e of <strong>the</strong> most fasc<strong>in</strong>at<strong>in</strong>g <strong>in</strong>sights of <strong>the</strong> last fifteen years regard<strong>in</strong>g new physics is<br />

that, due to a conjecture by Maldacena, one can describe concepts <strong>in</strong> strongly coupled<br />

<strong>the</strong>ories by a five dimensional (5D) model, based on a compact extra dimension with<br />

an unfactorizable Anti-de Sitter metric, <strong>the</strong> Randall Sundrum (RS) model. It adds<br />

to <strong>the</strong> fasc<strong>in</strong>ation, that <strong>the</strong> concept of partial compositeness is automatically implemented<br />

<strong>in</strong> <strong>the</strong>se models by mak<strong>in</strong>g <strong>the</strong> quarks 5D fields.<br />

In <strong>the</strong> first half of Chapter 2, this duality will be motivated, and <strong>the</strong> two different ways<br />

of describ<strong>in</strong>g <strong>the</strong> same physics will be used for a deeper understand<strong>in</strong>g of <strong>the</strong> analyses<br />

<strong>in</strong> <strong>the</strong> latter parts of <strong>the</strong> <strong>the</strong>sis. As a new result, a dual <strong>in</strong>terpretation of <strong>the</strong> small<br />

momentum expansion of <strong>the</strong> 5D propagator for gauge bosons will be presented <strong>the</strong>re.<br />

The rest of Chapter 2 will be devoted to <strong>the</strong> technical formulation of <strong>the</strong> fundamentals<br />

of <strong>the</strong> RS model. Important <strong>in</strong> this context is <strong>the</strong> geometrical explanation of how <strong>the</strong><br />

suppression of FCNCs is realized by <strong>the</strong> RS-GIM mechanism.<br />

Chapter 3 <strong>in</strong>cludes an update on <strong>the</strong> RS contributions to electroweak precision measurements,<br />

<strong>in</strong>clud<strong>in</strong>g <strong>the</strong> consequences of a new global fit for <strong>the</strong> oblique parameters<br />

S and T and <strong>the</strong> impact of new <strong>the</strong>oretical results on <strong>the</strong> conclusions drawn from <strong>the</strong><br />

Z ¯ bb for <strong>the</strong> RS parameter space. The effectiveness of <strong>the</strong> RS-GIM mechanism will be<br />

demonstrated on <strong>the</strong> basis of observables connected to <strong>the</strong> decay of Bs and Bd mesons<br />

to muons and Bs − ¯ Bs mix<strong>in</strong>g. The heavy b quark makes <strong>the</strong>m well suited to test <strong>the</strong><br />

limits of <strong>the</strong> RS-GIM mechanism, because <strong>the</strong> suppression of FCNCs becomes less effective<br />

<strong>the</strong> heavier <strong>the</strong> <strong>in</strong>volved flavors are. While it turns out that <strong>the</strong>se observables<br />

generically agree even with <strong>the</strong> small errors from recent LHCb measurements, one<br />

f<strong>in</strong>ds that <strong>the</strong> CP violat<strong>in</strong>g quantity <strong>in</strong> K − ¯ K mix<strong>in</strong>g, ɛK will <strong>in</strong>duce a f<strong>in</strong>e-tun<strong>in</strong>g<br />

of <strong>the</strong> order of one percent if no additional suppression of <strong>the</strong> RS contributions is<br />

implemented.<br />

This is rooted <strong>in</strong> a chiral enhancement and large renormalization group effects, and<br />

<strong>the</strong>refore it is a largely model <strong>in</strong>dependent problem for any new physics with vector<br />

coupl<strong>in</strong>gs to quarks. In RS models it is <strong>the</strong> only observable which needs f<strong>in</strong>e-tun<strong>in</strong>g<br />

and this issue has <strong>the</strong>refore been termed <strong>the</strong> “RS flavor problem”. After <strong>the</strong> explanations<br />

proposed <strong>in</strong> <strong>the</strong> literature are collected and <strong>in</strong>terpreted <strong>in</strong> <strong>the</strong> dual <strong>the</strong>ory, a<br />

novel solution based on an extension of <strong>the</strong> color gauge group will be presented and<br />

discussed <strong>in</strong> detail. This solution is especially attractive, because it preserves <strong>the</strong> anarchical<br />

flavor structure of <strong>the</strong> Yukawa matrices, which is essential <strong>in</strong> order to expla<strong>in</strong><br />

<strong>the</strong> hierarchies <strong>in</strong> quark masses and mix<strong>in</strong>gs. In <strong>the</strong> extended model <strong>the</strong> aforementioned<br />

observables will be computed, as well as <strong>the</strong> cross section for direct detection<br />

of <strong>the</strong> <strong>in</strong>volved new resonances at <strong>the</strong> LHC.<br />

The fact that <strong>the</strong> size of <strong>the</strong> coupl<strong>in</strong>gs of RS gauge fields to quarks depends on <strong>the</strong><br />

<strong>the</strong> quark mass, makes top observables an ideal candidate to look for effects of <strong>the</strong> RS<br />

model. Possible contributions to <strong>the</strong> forward-backward asymmetry measured by CDF<br />

and DØ , as well as <strong>the</strong> agreement with <strong>the</strong> total cross section <strong>in</strong> top antitop pairs<br />

will <strong>the</strong>refore be studied <strong>in</strong> Chapter 4. In a model-<strong>in</strong>dependent analyses, <strong>the</strong> impact<br />

of general new physics <strong>in</strong> <strong>the</strong> s and t channel will be computed and <strong>in</strong> particular <strong>the</strong><br />

effects <strong>in</strong> <strong>the</strong> RS model as well as <strong>in</strong> <strong>the</strong> RS model with <strong>the</strong> proposed extension will<br />

be shown.<br />

Conclud<strong>in</strong>g remarks and an outlook on future work <strong>in</strong> Chapter 5 will complete <strong>the</strong><br />

<strong>the</strong>sis.

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