2015
DOI: 10.1146/annurev-nucl-102014-022231
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Rare b Hadron Decays at the LHC

Abstract: With the completion of Run I of the CERN Large Hadron Collider, particle physics has entered a new era. The production of unprecedented numbers of heavy-flavoured hadrons in high energy proton-proton collisions allows detailed studies of flavour-changing processes.The increasingly precise measurements allow the Standard Model to be tested to a new level of accuracy. Rare b hadron decays provide some of the most promising approaches for such tests, since there are several observables which can be cleanly interp… Show more

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Cited by 28 publications
(50 citation statements)
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“…[13] for a review). In general, since the final states contain particles that do not undergo strong interactions, the hadronic uncertainties in the SM predictions for these observables are reduced compared to fully transitions have been carried out.…”
Section: Studies Of Cp Violation In B → Qγ and B → Q + − Transitionsmentioning
confidence: 99%
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“…[13] for a review). In general, since the final states contain particles that do not undergo strong interactions, the hadronic uncertainties in the SM predictions for these observables are reduced compared to fully transitions have been carried out.…”
Section: Studies Of Cp Violation In B → Qγ and B → Q + − Transitionsmentioning
confidence: 99%
“…In addition to the rates of semileptonic decays and of neutral B meson oscillations, mentioned above, important constraints can also be obtained from rare B meson decays such as B 0 (s) → µ + µ − [13]. The rare kaon decays, K + → π + νν and K 0 L → π 0 νν, also provide constraints on the apex of the Unitarity Triangle [21,22].…”
Section: Future Prospectsmentioning
confidence: 99%
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“…A powerful test of MFV is provided by the study of ratios between b → d and b → s transitions, because their Hamiltonians share the same structure. One particularly important example is the ratio between the decay rates of B 0 and B 0 s into dimuons [33], as this is a purely leptonic decay free from hadronic uncertainties. In the SM such ratios are approximately equal to |V td /V td | ∼ 1/25, only modified by phase space and hadronic matrix elements, while they can take very different values in non-MFV models.…”
Section: Flavour and Bsm Theoriesmentioning
confidence: 99%
“…A complete basis is given by a set of 10 operators, where O 1,2 are the tree level W operators; O 3−6,8 are penguin diagrams mediated by gluons; and O 7,9,10 , which are the operators that are relevant for radiative and leptonic penguin processes are defined as [33]:…”
Section: Operatorsmentioning
confidence: 99%