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Spin Squeezing, Entanglement and Quantum Metrology
Spin Squeezing, Entanglement and Quantum Metrology

... spin squeezing might also involve states that are not minimal uncertainty states. One example is the “one axis twisting" scheme proposed in [1], which we use in the experiments described in the last chapter of this thesis. For these states, as for experimentally very important non-pure quantum state ...
Symmetries and Interactions in Topological Matter
Symmetries and Interactions in Topological Matter

final report - Cordis
final report - Cordis

"Loop Quantum Gravity" (Rovelli)
"Loop Quantum Gravity" (Rovelli)

Quantum Orders and Symmetric Spin Liquids
Quantum Orders and Symmetric Spin Liquids

... (AF) transition temperature TAF ∼ 250K, the superconducting transition temperature Tc ∼ 100K, and the spin pseudo-gap scale ∆ ∼ 40meV.[17–19] The insulating property is completely due to the strong correlations present in the high Tc materials. Thus the strong correlations are expect to play very im ...
New perspectives for Rashba spin–orbit coupling
New perspectives for Rashba spin–orbit coupling

... To discuss the physics induced by SO coupling in systems lacking inversion symmetry, let us consider the p‑linear Rashba SO coupling introduced previously. Equation  3 in Box  1 describes a Zeeman term that involves a magnetic field proportional to the electron momentum p. Consequently, when electro ...
The CKM Matrix and CP Violation
The CKM Matrix and CP Violation

... • Because we are dealing with quarks, which are only observed as bound states, this is a fairly complicated subject. Here we will approach it in two steps: • i) Consider particle – anti-particle oscillations without CP violation •ii) Then discuss the effects of CP violation  Many features in common ...
The development of the quantum-mechanical electron theory of metals
The development of the quantum-mechanical electron theory of metals

... the areas of applicability of the newly developed FermiDirac and Bose-Einstein quantum statistics? (See Fermi, 1926a, 1926b;. Dirac, 1926; Einstein, 1924, 1925; Bose, 1924). As he wrote on 22 November to Erwin Schrodinger, "Recently, I have also been occupied with gas degeneracy [Schrodinger, 1924]. ...
A Theoretical Study of Charge Transport in Molecular Crystals Elham Mozafari
A Theoretical Study of Charge Transport in Molecular Crystals Elham Mozafari

Double quantum dot as a spin rotator
Double quantum dot as a spin rotator

Thermal Brane Probes
Thermal Brane Probes

Quantum Field Theory in Condensed Matter Physics 2nd Ed.
Quantum Field Theory in Condensed Matter Physics 2nd Ed.

The Large Hadron Collider - the World`s Largest Microscope
The Large Hadron Collider - the World`s Largest Microscope

THE RENORMALIZATION GROUP AND CRITICAL PHENOMENA
THE RENORMALIZATION GROUP AND CRITICAL PHENOMENA

Properties and detection of spin nematic order in strongly correlated
Properties and detection of spin nematic order in strongly correlated

I. Bell`s Theorem (pdf file)
I. Bell`s Theorem (pdf file)

Gluon saturation and initial conditions for relativistic heavy
Gluon saturation and initial conditions for relativistic heavy

Interacting Anyons in a One-Dimensional Optical Lattice
Interacting Anyons in a One-Dimensional Optical Lattice

... is defined by a set of quantum numbers. In contrast to that for fermions, i.e. particles with half-integer spin, there is the Pauli blockade, which means that for a given set of quantum numbers only one particle can occupy such a state. One of the crucial points of the spin-statistics theorem is its ...
Three Myths About Time Reversal in Quantum Theory 1. Introduction
Three Myths About Time Reversal in Quantum Theory 1. Introduction

Effects of Spin-Orbit Coupling on Quantum Transport
Effects of Spin-Orbit Coupling on Quantum Transport

Three myths about time reversal in quantum theory
Three myths about time reversal in quantum theory

Quantum Theory of Chiral Interactions in Cholesteric Liquid Crystals
Quantum Theory of Chiral Interactions in Cholesteric Liquid Crystals

... between molecules. Such a formulation is required in cases where it is either necessary or desirable to include orientational correlations between interacting molecules. It was shown that for central-force interactions between atoms on different molecules, a nonzero effective chiral interaction betw ...
The effects of disorder in strongly interacting quantum systems
The effects of disorder in strongly interacting quantum systems

RADIATION REACTION AND SELF-FORCE IN CURVED SPACETIME IN A FIELD THEORY APPROACH
RADIATION REACTION AND SELF-FORCE IN CURVED SPACETIME IN A FIELD THEORY APPROACH

Quiet Readout of Superconducting Flux States
Quiet Readout of Superconducting Flux States

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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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