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Quantum Field Theory, its Concepts Viewed from a Semiotic
Quantum Field Theory, its Concepts Viewed from a Semiotic

Short introduction to quantum mechanics
Short introduction to quantum mechanics

... . By completely is implied that the function Ψ(q1 , q2 , q3 , ..., qn ; t) contains all information obtainable by experiments. The qi , i = 1, .., n, are called characteristic variables such as space coordinates, t is the time dependence. The functions Ψ are called state functions or wavefunctions. ...
powerpoint - University of Illinois Urbana
powerpoint - University of Illinois Urbana

Majorana returns - MIT Center for Theoretical Physics
Majorana returns - MIT Center for Theoretical Physics

Berry Curvature as a Multi-Band Effect in Boltzmann Equations
Berry Curvature as a Multi-Band Effect in Boltzmann Equations

Quantum computation of scattering in scalar quantum field theories
Quantum computation of scattering in scalar quantum field theories

Theory and simulation of polar and nonpolar polarizable fluids
Theory and simulation of polar and nonpolar polarizable fluids

... we study both kinds of fluids. In fluids containing polar molecules that are also polarizable the molecules are modeled as anisotropic Drude oscillators in which the electronic motion along the direction of the permanent dipole and perpendicular to it have different force constants, or equivalently ...
Nonperturbative quantum geometries
Nonperturbative quantum geometries

Deconfined Quantum Critical Points
Deconfined Quantum Critical Points

Polarized Light and Quantum Mechanics
Polarized Light and Quantum Mechanics

Quantum Field Theory in a Non-Commutative Space: Sphere ?
Quantum Field Theory in a Non-Commutative Space: Sphere ?

... expects to observe deviations with respect to the quantum theory on the commutative sphere. Although the derivation of the non-commutative anomaly in [61] was worked out for the µ2 > 0 case, one may expect that a similar phenomenon occurs when µ2 < 0, too. For QFT on the commutative sphere, the latt ...
Kinetics of decay of metastable gas phase of polarized atomic
Kinetics of decay of metastable gas phase of polarized atomic

... background (see Ref. 8). This decrease of the energy A& increases with decreasing density, and if l AE l becomes larger than 2p,H, then the process of depolarization will have no threshold. Close to the usual density of the condensed state, the parameter I AE I is replaced by the width of the energy ...
Atomic motion in laser light: connection between semiclassical and
Atomic motion in laser light: connection between semiclassical and

An equation for the waves - University College London
An equation for the waves - University College London

msc_pre_phy_p2b1
msc_pre_phy_p2b1

The origin of the phase in the interference of Bose
The origin of the phase in the interference of Bose

Elements of QFT in Curved Space-Time
Elements of QFT in Curved Space-Time

... There are covariant equations for the matter (fields and particles, fluids etc) and Einstein equations for the gravitational field gµν ...
Chapter 3 Basic quantum statistical mechanics of spin
Chapter 3 Basic quantum statistical mechanics of spin

The Identification of Particles Using Diagrams and Distributions of
The Identification of Particles Using Diagrams and Distributions of

An introduction to topological phases of electrons
An introduction to topological phases of electrons

arXiv:quant-ph/0610027v1 4 Oct 2006
arXiv:quant-ph/0610027v1 4 Oct 2006

String Backgrounds
String Backgrounds

Atomic motion in laser light
Atomic motion in laser light

Did we discover the Higgs?
Did we discover the Higgs?

Fast converging path integrals for time-dependent potentials
Fast converging path integrals for time-dependent potentials

... and W represents the ideal effective potential, which ensures the exactness of the above expression. The latter depends not only on the coordinate mid-point x = (a + b)/2, the discretized velocity δ = b − a, and the time interval ε = tb − ...
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Propagator

In quantum mechanics and quantum field theory, the propagator gives the probability amplitude for a particle to travel from one place to another in a given time, or to travel with a certain energy and momentum. In Feynman diagrams, which calculate the rate of collisions in quantum field theory, virtual particles contribute their propagator to the rate of the scattering event described by the diagram. They also can be viewed as the inverse of the wave operator appropriate to the particle, and are therefore often called Green's functions.
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