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Introduction to Quantum Computation THE JOY OF ENTANGLEMENT
Introduction to Quantum Computation THE JOY OF ENTANGLEMENT

... mechanics is incomplete, as EPR claimed. These hidden variables are local because their local interaction with a measuring device determines the measurement result. To be explicit, let us assume that the particles reach Alice and Bob with prepared answers to the questions that Alice and Bob ask. The ...
Quantum Computing with Majorana Fermions Coupled to
Quantum Computing with Majorana Fermions Coupled to

Monogamy and ground-state entanglement in highly
Monogamy and ground-state entanglement in highly

Chapter 1 - BYU Physics and Astronomy
Chapter 1 - BYU Physics and Astronomy

Models of wave-function collapse
Models of wave-function collapse

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Lecture 1

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ATLAS and CMS

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372.pdf

of a quantum system or state - Hal-SHS
of a quantum system or state - Hal-SHS

The Status of our Ordinary Three Dimensions in a Quantum Universe 1
The Status of our Ordinary Three Dimensions in a Quantum Universe 1

1 Transport of Dirac Surface States
1 Transport of Dirac Surface States

Th tical lifetime eore Positronium:  A
Th tical lifetime eore Positronium: A

... the Klein-Gordon equation (which was the first relativistic wave equation) . The KGequation is covered mostly for the purpose of facilitating the discussion of Dirac's equation. We will therefore familiarize ourselves with the relativistic wave equation and its solutions by studying the KG equation. ...
Review of the Safety of LHC Collisions
Review of the Safety of LHC Collisions

- Philsci
- Philsci

... partition according to the measurements’ outcomes, in such a way that by the end of stage 4 their spins get correlated to their positions. The coupling between the spin and position is brought about by ‘opening’ the boxes and sending the particles either to the right, if the z-spin is up, or to the ...
The Quark model
The Quark model

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Paper

... quantum statistics and interactions profoundly change their properties. For example, they can even undergo a phase transition to a remarkable state of matter called a superfluid, which has no resistance to flow. Ultracold gases provide a valuable tool with which to study condensed-matter phenomena b ...
Paired Hall states
Paired Hall states

quantum - Word Format
quantum - Word Format

Interpreting Quantum Mechanics in Terms of - Philsci
Interpreting Quantum Mechanics in Terms of - Philsci

Spin Hamiltonians and Exchange interactions
Spin Hamiltonians and Exchange interactions

A Theoretical Study of Atomic Trimers in the Critical Stability Region
A Theoretical Study of Atomic Trimers in the Critical Stability Region

... ; it is a sum of three pairwise long-range Coulomb potentials. In molecular or nuclear (three-body) systems, we do not know the potential exactly 3 . Here the three particles are complex, i.e. composed of other particles. This means that the total potential of the (three-body) system can no longer b ...
Thesis - Institut für Physik
Thesis - Institut für Physik

Black Hole Entropy: From Shannon to Bekenstein
Black Hole Entropy: From Shannon to Bekenstein

... where in a very general context, pk denotes the probability of the system being in k-th state. For the particle entropy, it is numerically equal to maximum entropy ln 2 if the chances of the particle existing or not are both equal to 1/2. Hence it was not clear if the Shannon formula was capable of ...
DOC - UF Physics - University of Florida
DOC - UF Physics - University of Florida

ppt file - Manchester HEP
ppt file - Manchester HEP

< 1 ... 6 7 8 9 10 11 12 13 14 ... 171 >

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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