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Dux - ASDEX Upgrade
Dux - ASDEX Upgrade

The Nobel Prize in Physics 1901-2000
The Nobel Prize in Physics 1901-2000

Quantum mechanical description of stress and force in
Quantum mechanical description of stress and force in

Summarising Constraints On Dark Matter At The Large Hadron
Summarising Constraints On Dark Matter At The Large Hadron

These notes
These notes

... theories, which investigate the formation of composite particles when electrons bind to flux tubes, have been very fruitful [15, 16, 17]. These theories , based on their topological character, have given flesh to the notion of strange phenomena such as charge fractionalization, fractional statistics ...
Quantum Computation - University of Denver
Quantum Computation - University of Denver

Statistical Thermodynamics
Statistical Thermodynamics

Quantum reflection and dwell times of
Quantum reflection and dwell times of

... Where N – number of particles within the barrier and j – incident flux given as Does not distinguish if the particles got reflected or transmitted Büttiker: The extent to which the spin undergoes a Larmor precession is determined by the dwell time of a particle in the barrier. Hauge: the above state ...
Many-Body Localization
Many-Body Localization

... Closed-System Quantum Thermalization • In quantum system, initial state information perfectly preserved ...
Top Condensation as a Motivated Explanation of the Top Forward
Top Condensation as a Motivated Explanation of the Top Forward

... charged Higgses and pseudoscalar in two-Higgs doublet models, but couple only to the third generation, at leading order. Topcolor also generically has a top-Higgs, which is the scalar tt bound state. In addition, there should be angular and radial excitations. The lightest of these, in analogy to QC ...
An Introduction to the Quark Model
An Introduction to the Quark Model

Quantum mechanical approaches to the virial S.LeBohec
Quantum mechanical approaches to the virial S.LeBohec

... evolution of expectation values. Considering an observable A, the expectation value of this observable is denoted hAi = hφ(t)|A|φ(t)i when the considered system is in the quantum state |φ(t)i. The Ehrenfest theorem provides an expression for the time derivative of expectation values. In order to est ...
The Wave Function
The Wave Function

... A similar statement applies if ∆p = 0. In fact, this last possibility is the case for the example of a single harmonic wave function considered in Section 3.1. However, the uncertainty relation does not say that we cannot measure the position and the momentum at the same time. We certainly can, but ...
Gibbs paradox of entropy of mixing: Experimental facts, its rejection, and the theoretical consequences
Gibbs paradox of entropy of mixing: Experimental facts, its rejection, and the theoretical consequences

Why is not Double Negation Attested in Unwritten Kartvelian
Why is not Double Negation Attested in Unwritten Kartvelian

... Perspective: As far as the category of negation is a universal language phenomenon and different types of data are attested in Kartvelian languages in this respect, it is important to carry on the research, study the mixing of speech codes, discover the semantic meanings of the negative particle. ...
Reflections on the deBroglie–Bohm Quantum Potential
Reflections on the deBroglie–Bohm Quantum Potential

Against Field Interpretations of Quantum Field Theory - Philsci
Against Field Interpretations of Quantum Field Theory - Philsci

... φ̂(f ) represents the value that φ̂(x) would give (if it were definable), if we integrated it against f . As I said, this will be important later. Note that the field operators by themselves do not form a field configuration, in the strictest sense. Even a complete specification of the field operato ...
powerpoint - University of Illinois Urbana
powerpoint - University of Illinois Urbana

Real-Time Simulation of Dust Behavior
Real-Time Simulation of Dust Behavior

Light shining through walls
Light shining through walls

NON-RELATIVISTIC QUANTUM MECHANICS - Philsci
NON-RELATIVISTIC QUANTUM MECHANICS - Philsci

Neoclassical Transport
Neoclassical Transport

Investigation of magnetite formation from the systems Fe(III)/Fe(II
Investigation of magnetite formation from the systems Fe(III)/Fe(II

Soft Contribution to the Hard Ridge
Soft Contribution to the Hard Ridge

Quintet pairing and non-Abelian vortex string in spin-3/2 cold atomic... Congjun Wu, Jiangping Hu, and Shou-Cheng Zhang
Quintet pairing and non-Abelian vortex string in spin-3/2 cold atomic... Congjun Wu, Jiangping Hu, and Shou-Cheng Zhang

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Identical particles

Identical particles, also called indistinguishable or indiscernible particles, are particles that cannot be distinguished from one another, even in principle. Species of identical particles include, but are not limited to elementary particles such as electrons, composite subatomic particles such as atomic nuclei, as well as atoms and molecules. Quasiparticles also behave in this way. Although all known indistinguishable particles are ""tiny"", there is no exhaustive list of all possible sorts of particles nor a clear-cut limit of applicability; see particle statistics #Quantum statistics for detailed explication.There are two main categories of identical particles: bosons, which can share quantum states, and fermions, which do not share quantum states due to the Pauli exclusion principle. Examples of bosons are photons, gluons, phonons, helium-4 nuclei and all mesons. Examples of fermions are electrons, neutrinos, quarks, protons, neutrons, and helium-3 nuclei.The fact that particles can be identical has important consequences in statistical mechanics. Calculations in statistical mechanics rely on probabilistic arguments, which are sensitive to whether or not the objects being studied are identical. As a result, identical particles exhibit markedly different statistical behavior from distinguishable particles. For example, the indistinguishability of particles has been proposed as a solution to Gibbs' mixing paradox.
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