Catálogo de publicaciones - libros
IFAE 2006: Incontri di Fisica delle Alte Energie Italian Meeting on High Energy Physics
Guido Montagna ; Oreste Nicrosini ; Valerio Vercesi (eds.)
Resumen/Descripción – provisto por la editorial
No disponible.
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Disponibilidad
Institución detectada | Año de publicación | Navegá | Descargá | Solicitá |
---|---|---|---|---|
No detectada | 2007 | SpringerLink |
Información
Tipo de recurso:
libros
ISBN impreso
978-88-470-0529-7
ISBN electrónico
978-88-470-0530-3
Editor responsable
Springer Nature
País de edición
Reino Unido
Fecha de publicación
2007
Información sobre derechos de publicación
© Springer-Verlag Italia 2007
Cobertura temática
Tabla de contenidos
Rare decays at the -Factories
Concetta Cartaro
The present contribution summarizes some results from the BaBar and Belle collaborations on the following categories of rare decays: Hadronic rare decays will not be treated in this contribution.
- Parallel Session: Flavour Physics (S. Giagu and L. Silvestrini, conveners) | Pp. 243-246
violation and CKM parameters determination in BaBar
Nicola Neri
violation (), first detected in → decays in 1964 [], is accomodated in the Standard Model (SM) by a -violating phase in the CKM matrix, the matrix which describes the mixing of the quarks (under the weak interaction) []. From the unitarity constraints of the CKM matrix, we have + + = 0, the so-called Unitarity Triangle relation, represented in Fig. 1. is proportional to the area of the triangle and requires the angles and sides to be different from zero. The main goal of the BaBar experiment [] is to overconstrain the Unitarity Triangle parameters, measuring the sides and the angles directly from the data of and meson decays, in order to test the consistency of the SM.
- Parallel Session: Flavour Physics (S. Giagu and L. Silvestrini, conveners) | Pp. 247-250
Semileptonic and nonleptonic decays of
Mikhail A. Ivanov; Jürgen G. Körner; Pietro Santorelli
Using our relativistic constituent quark model we present results on the exclusive nonleptonic and semileptonic decays of the -meson. The nonleptonic decays are studied in the framework of the factorization approximation. We calculate the branching ratios for a large set of exclusive nonleptonic and semileptonic decays of the meson and compare our results with the results of other models.
- Parallel Session: Flavour Physics (S. Giagu and L. Silvestrini, conveners) | Pp. 251-255
Aspects of non leptonic decays
R. Ferrandes
Non perturbative strong interaction effects make difficult a theoretical description of non leptonic weak decays of hadrons; so it is relevant the possibility to obtain predictive parametrizations of decay amplitudes. It is noticeable that the widths of a set of two-body transitions can be predicted using the symmetries of QCD and available information on decays [].
- Parallel Session: Flavour Physics (S. Giagu and L. Silvestrini, conveners) | Pp. 257-260
Measurement of the oscillation frequency at CDF
Giuseppe Salamanna
The first precise measurement of the oscillation frequency Δ with the CDFII experiment [] is summarized in this talk.
- Parallel Session: Flavour Physics (S. Giagu and L. Silvestrini, conveners) | Pp. 261-264
Prospects for heavy flavor physics at LHC
G. Passaleva
In the last decade, the flavor sector of the Standard Model, parametrized by the Cabibbo-Kobayashi-Maskawa (CKM) matrix [], has been studied and constrained with unprecedented precision thanks to the beautiful results obtained on Kaon CP violation experiments E731, KLOE and NA48, by the -factories KEKB and PEPII, by the charm factory CESR and by the experiments at Tevatron. The impact of these results on the experimental tests of the Standard Model is pictorially represented on the plane where the constraints on the Unitarity Triangle (UT) are displayed []. The Large Hadron Collider (LHC) in construction at CERN, is expected to deliver a large amount of events containing heavy flavors due to the high luminosity (10–10 cms) and high production cross sections (() ∼ 0.5mb).
- Parallel Session: Flavour Physics (S. Giagu and L. Silvestrini, conveners) | Pp. 265-268
QED corrections and the → π puzzle
Elisabetta Baracchini
We discuss the theoretical and experimental treatment of radiative corrections in hadronic decays. We present analytic expressions to describe the leading effects induced by both real and virtual (soft) photons in the generic process → (), where and are scalar or pseudoscalar particles. After discussing the procedures to be adopted in experimental analysis for a clear definition of the observables, we show how it is possible to explain the “ → π puzzle” in view of an (2) analysis taking into account QED corrections as a source of isospin breaking.
- Parallel Session: Flavour Physics (S. Giagu and L. Silvestrini, conveners) | Pp. 269-273
Status of the Unitarity Triangle analysis
M. Bona; M. Ciuchini; E. Franco; V. Lubicz; G. Martinelli; F. Parodi; M. Pierini; P. Roudeau; C. Schiavi; L. Silvestrini; V. Sordini; A. Stocchi; V. Vagnoni
The analysis of the Unitarity Triangle (UT) and CP violation provides nowadays a unique opportunity to look for New Physics (NP) effects beyond the Standard Model (SM).
- Parallel Session: Flavour Physics (S. Giagu and L. Silvestrini, conveners) | Pp. 275-278
Non-perturbative inputs for Flavour Physics
Federico Mescia
In the pursuit of improving our knowledge of short-distance physics from weak hadron decay (i. e. the CKM couplings in the Standard Model), reliable theoretical estimates of QCD non-perturbative effects are needed. For many decays from to physics (see Fig. 1), Lattice QCD remains the only tool to achieve this task. Once masses heavier than are integrated out, low-energy QCD effects are encoded into hadronic matrix elements of some local operator.
- Parallel Session: Flavour Physics (S. Giagu and L. Silvestrini, conveners) | Pp. 279-283
Bounds on the supersymmetric flavour space
Valentina Porretti
We introduce the supersymmetric flavour problem (Sect. 2) focusing on mixing processes in the quark sector (Sect. 3) and present updated plots of the bounds on squark mass matrices obtained in the mass insertion approximation (Sect. 4).
- Parallel Session: Flavour Physics (S. Giagu and L. Silvestrini, conveners) | Pp. 285-288