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Thomson`s Model of the Atom
Thomson`s Model of the Atom

Notes #2 Chem 341
Notes #2 Chem 341

Chapter 8 Microcanonical ensemble
Chapter 8 Microcanonical ensemble

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An Ontological Interpretation of the Wave Function - Philsci
An Ontological Interpretation of the Wave Function - Philsci

Quantum computers
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... important thing: To do all that can be done with a qubit, there is a very limited timeframe to work in. That is because superpositions of states (states of the form: a |0> + b |1> ) are generally very unstable, and will collapse into one of the pure states |0> or |1> quickly as a result of interacti ...
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Notes from Chapter 9

Path integral Monte Carlo study of the interacting quantum double-well... Quantum phase transition and phase diagram
Path integral Monte Carlo study of the interacting quantum double-well... Quantum phase transition and phase diagram

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The Essentials of Quantum Mechanics

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Unified rotational and permutational symmetry and selection rules in

Spacetime structures of continuous
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Limits of fractality: Zeno boxes and relativistic particles
Limits of fractality: Zeno boxes and relativistic particles

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Chapter 40

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mc2007_ATLAS_Neil

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THE CROSSOVER TO THE KPZ EQUATION We consider the one

ESI Bose-Einstein Condensation as a Quantum Phase Transition in an Optical Lattice
ESI Bose-Einstein Condensation as a Quantum Phase Transition in an Optical Lattice

Field Formulation of Many-Body Quantum Physics {ffmbqp
Field Formulation of Many-Body Quantum Physics {ffmbqp

... By applying S or A to an arbitrary n-particle wave function one obtains completely symmetric or completely antisymmetric n-particle wave functions. In nature, both signs can occur. Particles with symmetric wave functions are called bosons, the others fermions. Examples for bosons are photons, mesons ...
P410M: Relativistic Quantum Fields
P410M: Relativistic Quantum Fields

The Zeno`s paradox in quantum theory
The Zeno`s paradox in quantum theory

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Quantum mechanics: Myths and facts

A Very Short Introduction to Quantum Field Theory
A Very Short Introduction to Quantum Field Theory

The roads not taken: empty waves, wavefunction collapse and
The roads not taken: empty waves, wavefunction collapse and

Full Text PDF - Science and Education Publishing
Full Text PDF - Science and Education Publishing

General description of the Universe - School of Physics
General description of the Universe - School of Physics

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pdf

... Next ยป condensates could be made from fermions as well as bosons. For this reason, we were stunned and delighted sample issue to learn that Deborah Jin, Cindy Regal and Markus Greiner at Request a sample issue the JILA laboratory in the US have created the first fermionic condensate by cooling a gas ...
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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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