4,512 research outputs found
Polarized parton distributions in perturbative QCD
We review the main results of next-to-leading order QCD analyses of polarized
deep-inelastic scattering data, with special attention to the assessment of
theoretical uncertainties.Comment: 4 pages Latex, 1 ps figure. Talk given at NUCLEON '99,
Frascati(Italy), June 7-9 199
Status of the Standard Model at the LHC Start
I present a concise review of where we stand in particle physics today.
First, I will discuss QCD, then the electroweak sector and finally the
motivations and the avenues for new physics beyond the Standard Model.Comment: Plenary Talk at the 5th Italian Workshop on p-p Physics at the LHC.
13 pages, no figure
Concluding talk: fundamental lessons and challenges from neutrinos
We present a concise review of the experimental developments on neutrino
mixing and their theoretical implications as presented and discussed at this
Conference. The recent data disfavour many models but the surviving ones still
span a wide range going from Anarchy (no structure, no symmetry in the neutrino
sector) to a maximum of symmetry, as for the models based on discrete
non-abelian flavour groups which can be improved following the indications from
the recent data.Comment: 20 pages, no figures. Talk given at the Pontecorvo 100 Symposium in
honour of Bruno Pontecorvo for the centennial of the birth, Pisa, 18-20
September 2013. arXiv admin note: text overlap with arXiv:1304.5047,
arXiv:1111.6421, arXiv:1210.346
An Overview of Neutrino Mixing
We present a concise review of the recent important experimental developments
on neutrino mixing (hints for sterile neutrinos, large , possible
non maximal , approaching sensitivity on ) and their
implications on models of neutrino mixing. The new data disfavour many models
but the surviving ones still span a wide range going from Anarchy (no
structure, no symmetry in the lepton sector) to a maximum of symmetry, as for
the models based on discrete non-abelian flavour groups.Comment: 6 pages, no figures. Talk given at the Fourth Workshop on Theory,
Phenomenology and Experiments in Flavour Physics, June 2012, Capri, Ital
The Standard Electroweak Theory and Beyond
1. Introduction, 2. Gauge Theories, 3. The Standard Model of Electroweak
Interactions, 4. The Higgs Mechanism, 5. The CKM Matrix, 6. Renormalisation and
Higher Order Corrections, 7. Why we do Believe in the Standard Model: Precision
Tests, 7.1.Precision Electroweak Data and the Standard Model, 7.2.A More
General Analysis of Electroweak Data, 8. Why we do not Believe in the Standard
Model, 8.1.Conceptual Problems, 8.2.Hints from Experiment, -8.2.1 Unification
of Couplings, -8.2.2 Dark Matter, -8.2.3 Neutrino Masses, -8.2.4 Baryogenesis,
9. Status of the Search for the Higgs and for New Physics, 10.ConclusionComment: 59 pages, 9 figures, Lectures given at the Nathiagali Summer School,
Pakistan and the PSI Zuoz Summer School, July - August 200
The crucial problem: the electroweak symmetry breaking
1. Why we do Believe in the Standard Model
2. Why we do not Believe in the Standard Model
2.1 Conceptual Problems
2.2 Hints from Experiment
2.2.1 Unification of Couplings
2.2.2 Dark Matter
2.2.3 Neutrino Masses
2.2.4 Baryogenesis
3. Status of the Search for the Higgs and for New Physics
4. ConclusionComment: 16 pages, Talk, XI Rencontres de Blois, Frontiers of Matter, 27
June-3 July 199
Neutrino Tribimaximal Mixing from A_4 Alone
Neutrino tribimaximal mixing is obtained from the breaking of A_4 to Z_3 in
the charged-lepton sector and to Z_2 in the neutrino sector. To enforce this
conflicting pattern, extra particles and symmetries are usually invoked, often
accompanied by nonrenormalizable interactions and even extra dimensions. It is
shown here in a specific renormalizable model how A_4 alone will accomplish
this, with only the help of lepton number.Comment: 8 pages, no figure, reference correcte
One light composite Higgs boson facing electroweak precision tests
We study analytically and numerically the bounds imposed by the electroweak
precision tests on a minimal composite Higgs model. The model is based on
spontaneous SO(5)/SO(4) breaking, so that an approximate custodial symmetry is
preserved. The Higgs arises as a pseudo-Goldstone boson at a scale below the
electroweak symmetry breaking scale. We show that one can satisfy the
electroweak precision constraints without much fine-tuning. This is the case if
the left-handed top quark is fully composite, which gives a mass spectrum
within the reach of the LHC. However a composite top quark is strongly
disfavoured by flavour physics. The alternative is to have a singlet top
partner at a scale much lighter than the rest of the composite fermions. In
this case the top partner would be light enough to be produced significantly at
the LHC.Comment: 15 pages, 4 figures; v2: figures and discussion improved, references
added; v3: minor changes, final version to appear in PR
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