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Oxford LHCb and CLEO-c

Denys Wilkinson Building
Keble Road
Oxford
OX1 3RH

LHCb Physics and Oxford Activities

At present, the specific physics foci of the Oxford group are

Guy Wilkinson is co-convenor of the CP Working Group, which oversees these two activities amonst others.

Feynman diagrams of B mixing The general physics programme at LHCb compasses a large and varied set of precise measurements of B and D meson decays that will provide information on physics beyond the Standard Model in a manner which is complementary to the direct particle searches carried out at ATLAS and CMS. Rare processes that are dominated by suppressed Feynman diagrams are driven by heavy virtual particles in so-called `loops'. For example, in the B mixing processes shown to the left, the dominant Standard Model contributions come from the diagrams with top quarks in the box loops. In general, however, new physics particles must also contribute to these loops, giving experimental signatures inconsistent with the Standard Model expectations.

The primary interest of B decays lies in the multitude of modes which can be studied to learn more about CP violation - the difference in behaviour between matter and anti-matter. In the Standard Model CP violation in introduced as a complex phase in the 3x3 unitarity `Cabibbo-Kobayashi-Maskawa (CKM) matrix', which parameterises the couplings in weak charged current quark interactions. A geometrical way to express this understanding is through the unitarity triangle, which is representation of the relationship between certain CKM elements in the (ρ-bar, η-bar) plane, where ρ-bar and η-bar are two of the four parameters of the matrix, η-bar being the imaginary component. If quark coupling and CP violation is fully described by the Standard Model, all experimental measurements will give results consistent with the uniarity triangle picture. As there is no known reason why new physics will have the same quark coupling and CP violation structure as the Standard Model, contributions from this source will give rise to discrepancies between measurements.

CKMFitter plot of Unitarity Triangle measurements as of FPCP 2007 Shown at right is the present status of the unitarity triangle as presented by the CKMfitter group.

Each coloured band represents a different measurement, most of which come from the B-meson sector, performed at BaBar and Belle. All measurements have associated contours which overlap in a yellow oval in the region (ρ-bar, η-bar) = (0.21,0.35), which is the top vertex of the triangle. This overlap of all measurements indicates that within the present experimental precision the CKM description of quark mixing and CP violation is correct. The fact that the overlap region is far-away from η-bar = 0 expresses the experimental evidence for CP violation.

LHCb will significantly improve the sensitivity of many of the measurements contributing to the unitarity triangle, in particular the very poor existing constraints on the angle γ as indicated by the beige shading. Making a precise measurement of γ is one of the most important goals of flavour physics in the coming decade. Taking on this challenge is a priority of the Oxford LHCb group.

There exist many other extremely important measurements which are best considered independently of the unitarity triangle context. These include:

More information on the LHCb physics programme can be found in LHCb's web pages.

 

 

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