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Duality Theory of Weak Interaction
Duality Theory of Weak Interaction

... is the universality of physical laws, i.e. the validity of laws of Nature is independent of the coordinate systems expressing them. Consequently, the symmetries in (2.17) cannot be broken at both levels of (2.15) and (2.16). However, the physical implication of the gauge symmetry is different at the ...
The metron model - Max-Planck
The metron model - Max-Planck

Compton Scattering Sum Rules for Massive Vector
Compton Scattering Sum Rules for Massive Vector

... Purpose of this Study A particle of arbitrary spin j has in general 2j + 1 electromagnetic moments. While there have been several studies on generalizing the GDH to higher spins [Pai67, LC75] and the extension of the GDH to arbitrary spin has proven to be valid [DHK+ 04], there has been no rigorous ...
Quantum Spin Hall Effect and their Topological Design of Devices
Quantum Spin Hall Effect and their Topological Design of Devices

... A very important achievement was the realization that the quantum spin Hall state remain to be non-trivial even after the introduction of spin-up spin-down scattering,[3] which destroy the quantum spin Hall effect. In order experiment was introduced a topological Z 2 , invariant who characterizes a ...
Physics of the Large Hadron Collider Lecture 1: Fundamentals of the
Physics of the Large Hadron Collider Lecture 1: Fundamentals of the

On Unitary Evolution in Quantum Field Theory in
On Unitary Evolution in Quantum Field Theory in

... hypersurfaces in a one-to-one correspondence, the associated quantum operator should be unitary. In a quantization context this comes from a one-to-one correspondence between classical solutions near the hypersurfaces. Such a correspondence occurs of course in the standard case of spacelike Cauchy h ...
Why High Energy Physics At UTA??
Why High Energy Physics At UTA??

Open-Closed String Duality in Field Theory? - damtp
Open-Closed String Duality in Field Theory? - damtp

... Everybody loves a good D-brane. These objects have underpinned much of the progress in high-energy theoretical physics for the past ten years, culminating in the miraculous AdS/CFT correspondence which, at its heart, relies on the equivalence of open and closed string descriptions of D-brane dynamic ...
The phase diagram of dense QCD
The phase diagram of dense QCD

gravitational interaction of fermions
gravitational interaction of fermions

Lecture 1 - Particle Physics Research Centre
Lecture 1 - Particle Physics Research Centre

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Introduction to Supersymmetry

The Matter Glitch
The Matter Glitch

The Matter Glitch
The Matter Glitch

... a. Why don’t protons decay as neutrons do? b. Why is the universe made of matter and not anti-matter? c. Why do neutrinos have a tiny but variable mass? a. Why are there three particle “generations” then no more? b. Why do electrons "half spin"? c. Why does mass vary enormously but charge doesn’t? d ...
Working Group Talks Gobinda Majumdar Issues In The Construction
Working Group Talks Gobinda Majumdar Issues In The Construction

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Dual approaches for defects condensation

Functional RG for few
Functional RG for few

... → reproduces fixed-points and power counting found using Wilsonian RG → extends results to nonzero total momentum • highlights issues that will need to be addressed in improved applications to dense fermionic matter ◦ violations of Galilean invariance ◦ nonanalytic terms generated by sharp cut-offs ...
Stringy holography and the modern picture of QCD and hadrons
Stringy holography and the modern picture of QCD and hadrons

ppt - Nikhef
ppt - Nikhef

... SUSY: ‘solves’ the hierarchy problem: All ΔMh terms between particles and super-partners magically cancel fermions ...
2014 version - Elementary Particle Physics @ Birmingham
2014 version - Elementary Particle Physics @ Birmingham

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Lecture 2: Bogoliubov theory of a dilute Bose gas Abstract
Lecture 2: Bogoliubov theory of a dilute Bose gas Abstract

High Energy Cross Sections by Monte Carlo
High Energy Cross Sections by Monte Carlo

... Compton derived these formulas simply by using relativistic kinematics and conservation of energy and momentum. They are valid for scattering of a photon from a spinless charged particle. ...
Adiabatic Preparation of Topological Order
Adiabatic Preparation of Topological Order

... terms of a nonlocal order parameter, e.g., the expectation value of string operators (operators formed by tensor products of local operators taken along a string). Another arena in which topological order has found profound applications is quantum computation, in particular, in the context of system ...
4 Canonical Quantization
4 Canonical Quantization

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Quantum chromodynamics

In theoretical physics, quantum chromodynamics (QCD) is the theory of strong interactions, a fundamental force describing the interactions between quarks and gluons which make up hadrons such as the proton, neutron and pion. QCD is a type of quantum field theory called a non-abelian gauge theory with symmetry group SU(3). The QCD analog of electric charge is a property called color. Gluons are the force carrier of the theory, like photons are for the electromagnetic force in quantum electrodynamics. The theory is an important part of the Standard Model of particle physics. A huge body of experimental evidence for QCD has been gathered over the years.QCD enjoys two peculiar properties:Confinement, which means that the force between quarks does not diminish as they are separated. Because of this, when you do separate a quark from other quarks, the energy in the gluon field is enough to create another quark pair; they are thus forever bound into hadrons such as the proton and the neutron or the pion and kaon. Although analytically unproven, confinement is widely believed to be true because it explains the consistent failure of free quark searches, and it is easy to demonstrate in lattice QCD.Asymptotic freedom, which means that in very high-energy reactions, quarks and gluons interact very weakly creating a quark–gluon plasma. This prediction of QCD was first discovered in the early 1970s by David Politzer and by Frank Wilczek and David Gross. For this work they were awarded the 2004 Nobel Prize in Physics.The phase transition temperature between these two properties has been measured by the ALICE experiment to be well above 160 MeV. Below this temperature, confinement is dominant, while above it, asymptotic freedom becomes dominant.
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