CPH Theory

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Cern Experiment and Violatin of Newton's Second Law

LEIBNIZ'S MONADS AND JAVADI'S CPH

World Science Database

General Science Journal

Hadronic Journal

National Research Council Canada

November 2, 2011: CERN Experiment and Violation of Newton’s Second Law Englishview

October 13, 2011: CERN Experiment and Violation of the Newton’s Second Law Persianview

November 24, 2008: A New Definition of Gravitonview

July 10, 2007: Zero Point Energy and the Dirac Equationview

June 28, 2007: Unification and CPH Theoryview

June 14, 2007: Summary of Physics Conceptsview

June 14, 2007: Strong Interaction and CPH Theory Rview

June 4, 2007: Quantum Electrodynamics and CPH Theoryview

November 30, 2006: Vocabulary of CPH Theoryview

November 17, 2006: Thermodynamic Laws Entropy and CPH Theoryview

November 17, 2006: Time Function and Absolute Black Holeview

October 14, 2006: CPH and Timeview

October 13, 2006: CPH Theory and Newton's Second Lawview

October 13, 2006: Time Function and Work Energy Theoremview

October 13, 2006: CPH Theory and Special Relativityview

October 13, 2006: Properties of CPHview

July 31, 2006: A New Mechanism of Higgs Bosons in Producing Charge Particlesview

May 14, 2006: Speed of Light and CPH Theoryview

April 28, 2006: Color Charges Curve Spaceview

April 17, 2006: Effective Nuclear Chargeview

April 12, 2006: Maxwell's Equations in a Gravitational Fieldview

April 11, 2006: Realization Hawking - End of Physics by CPHview

April 7, 2006: Questions and Answers on CPH Theoryview

April 7, 2006: Opinions on CPH Theoryview

April 7, 2006: Questions and Answers on CPH Theoryview

March 23, 2006: Analysis of CPH Theoryview

March 21, 2006: Logical Foundation of CPH Theoryview

March 21, 2006: Definition Principle and Explanation of CPH Theoryview

March 21, 2006: Logical Foundation of CPH Theoryview

March 21, 2006: Definition Principle and Explanation of CPH Theoryview

March 21, 2006: Experimental Foundation of CPH Theoryview

March 19, 2006: Color Charge/Color Magnet and CPHview

March 19, 2006: Sub-Quantum Chromodynamicsview

Phenomenology of Charged Higgs Bosons and B-meson Decays

Phenomenology of Charged Higgs Bosons and B-meson Decays

Author:

Eriksson, David (Uppsala University, Division of Nuclear and Particle Physics)

Title:

Phenomenology of Charged Higgs Bosons and B-meson Decays

Department:

Uppsala University, Teknisk-naturvetenskapliga vetenskapsområdet, Physics, Department of Physics and Astronomy, Division of Nuclear and Particle Physics

Abstract(en) :

For more than 30 years the Standard Model has been the theoretical foundation for particle physics. The theory has been veriﬁed successfully by experimental tests. Its biggest shortcoming is the non-discovery of the Higgs boson,responsible for giving the other particles masses. Despite its success there are hints that the Standard Model is not the complete theory and many extensions of it, such as supersymmetry, have been proposed.

Extended theories often predict the existence of a charged Higgs boson and its detection will be a clear sign of physics beyond the Standard Model. The main focus in this thesis is on various phenomenological aspects of the charged Higgs boson. For favorable mass and couplings direct detection is shown to be possible at the Large Hadron Collider in production with an associated W boson. It is also shown how a light charged Higgs can have measurable effects on spin correlations in decays of pair-produced top quarks. The charged Higgs boson can also be seen indirectly, in for example B-meson decays, which can be used to put constraints on its mass and fermion couplings. Exclusion limits in two supersymmetric models are given together with a comparison with the discovery potentials for the LHC experiments. A tool for calculating properties, such as masses and decays, of both charged and neutral Higgs bosons in the Two-Higgs-Doublet Model is also presented.

B-meson decays can also be used to test aspects of the strong interaction. Part of this thesis deals with improving and applying phenomenological models to B-meson decays. Although these models are not derived from ﬁrst principles, their success shows that they capture important features of non-perturbative strong interactions.

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