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Simple Harmonic Oscillator
Simple Harmonic Oscillator

CCR 7: Derivation of the Boltzmann Distribution
CCR 7: Derivation of the Boltzmann Distribution

The Kinetic Theory of Gases (2)
The Kinetic Theory of Gases (2)

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ppt - HEP Educational Outreach

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Animator Help Session

... Distinct may mean forces whose values are calculated with different equations (gravity and drag are distinct because gravity eq is of form f=ma, where drag is defined in terms of a drag coefficient and velocity) Alternatively (and better): distinct may mean that one force is a unary force and anothe ...
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Group and phase velocity

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Exam questions - Grand Valley State University

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from last time:

... often done by educated guessing, and there may be more than one solution. Apply boundary conditions – these will often limit your values of energy. Evaluate any undetermined constants (like amplitudes), e.g. by using boundary conditions, applying normalisation. Check your solution, if it gives you s ...
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Chapter 4.2 Notes

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Words for Matter Chapter 2

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Chapter41_VG

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Collider: Step inside the World`s Greatest Experiment

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... quantum system stop existing as a mixture of states and become one or the other? (More technically, when does the actual quantum state stop being a linear combination of states, each of which resemble different classical states, and instead begin to have a unique classical description?) If the cat s ...
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CHEM 532 Physical Chemistry II (Quantum Chemistry) Fall 2013

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Intro to Quantum Mechanics

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statpp2006

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if on the Internet, Press  on your browser to
if on the Internet, Press on your browser to

... At first, Georgi didn't believe his own findings. "I did think I was crazy," he recalls. "It was such an interesting result. I thought I was either wrong or that everyone had seen it before." Other physicists, however, confirmed that he wasn't having delusions: Unparticles were indeed something ent ...
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Slide1

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black_holes_Hamburg_2016

PHYSICS DEPARTMENT Syllabus: Phys 217 (3 cr.) – Mechanics
PHYSICS DEPARTMENT Syllabus: Phys 217 (3 cr.) – Mechanics

PY 482: Computation for Experimental Particle Physics
PY 482: Computation for Experimental Particle Physics

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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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