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Particle Physics 2016

December 08-10, 2016

Volume 4 Issue 3(Suppl)

J Astrophys Aerospace Technol

ISSN: 2329-6542 JAAT, an open access journal

conferenceseries

.com

December 08-10, 2016 Dallas, Texas, USA

Astrophysics and Particle Physics

International Conference on

J Astrophys Aerospace Technol 2016, 4:3(Suppl)

http://dx.doi.org/10.4172/2329-6542.C1.006

Diphoton Higgs decay in an U(1)′ model

Juan Pablo Rubio

1,2

1

Universidad Nacional de Colombia, Colombia

2

Ciudad Universitaria, Mexico

A

t present, the possible confirmation by the LHC of a scalar particle identified as the Higgs boson has increased the study

of its different decay channels, where the diphoton decay is one of the most prominent processes, because of the excess

reported by LHC. These excesses may be associated with new symmetries in models beyond the standard model. In particular,

family non-universal U(1)’ symmetry models have many motivations to be considered, because they involve a large number

of phenomenological consequences and theoretical aspects as flavor physics, physics of neutrinos, dark matter, among other

effects. These models also involve a new neutral boson Z’, something else new anomalies appear. It is necessary to extend of

the fermionic spectrum in order to obtain a chiral theory free of anomalies. On the other hand, the new symmetries require

extended scalar sectors to generate the spontaneous breaking of the new Abelian symmetry and to get masses for the new

gauge boson Z’ and the extra fermionic content. In particular, the scalar sector is extended with two scalar doublets and two

singlets, where one of the singlets is postulated as a dark matter (DM) candidate. The purpose of this work is to calculate the

new contribution to the diphoton channel decay width of the Higgs, as it offers a clear signal of new physics associated with

the scalar sector, where loop contribution from charged Higgs bosons are taken into account. Also, since the signal strength

depends on the ratio with the total of Higgs boson decay, it is possible to evaluate the effects of a light DM component as an

invisible final state.

jprubioo@unal.edu.co

Measurements with diverse concepts in quantum/particle physics

Payman Sheriff

Heriot-Watt University, UK

M

uch of particle physics uses data from new measurements, average measured properties of gauge bosons, leptons, quarks,

mesons and baryons; there are many that are new or heavily revised including those on quark-mixing matrix, top quark,

muon anomalous magnetic moment, extra dimensions, particle detectors, cosmic background radiation, dark matter, cosmological

parameters andbigbang cosmology.Themodel is basedongauge theories, ofwhich thefirstwas quantumelectrodynamics, describing

the interactions of light with matter. The core element of particle physics analysis as the name suggests is the physical characteristics

that form the basis of themeasurement. Decoherence theorists, who use various non-standard interpretations of quantummechanics

that deny the projection postulate quantum jumps and even the existence of particles, define the measurement problem as the failure

to observe superpositions such as Schrödinger's cat. Measurements are described with diverse concepts in quantum physics such

as; wave functions/probability amplitudes, evolving unitary and deterministic/preserving information, according to the linear

Schrödinger equation, superposition of states, i.e., linear combinations of wave functions with complex coefficients that carry phase

information and produce interference effects/the principle of superposition, quantum jumps between states accompanied by the

"collapse" of the wave function that can destroy or create information, probabilities of collapses and jumps given by the square of the

absolute value of the wave function for a given state, values for possible measurements given by the eigenvalues associated with the

eigenstates of the combined measuring apparatus and measured system. The expected consequence of Niels Bohr's "Copenhagen

interpretation" of quantum mechanics, was to explain how our measuring instruments, which are mostly macroscopic objects and

treatable with classical physics, can give us information about the microscopic world of atoms and subatomic particles like electrons

and photons. Some define the problem of measurement simply as the logical contradiction between two laws describing the motion

of quantum systems; the unitary, continuous, and deterministic time evolution of the Schrödinger equation versus the non-unitary,

discontinuous, and indeterministic collapse of the wave function. Here, I intend to present a unified dynamics framework using

particles connected by constraints as the fundamental infrastructure that let us treat measurements in a unified manner.

Peymsheff@yahoo.com