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Particle Physics
Particle Physics

... 5. This is a problem set about QED. a. Prove that an electron in isolation cannot emit one photon because of momentum conservation. That is, the process e   p1   e  ( p 2 )    p3  (the letters in the parentheses are the corresponding momenta) is prohibited. b. However, if electron gets a s ...
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3-D Schrodinger`s Equation, Particle inside a 3

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Weakton Model of Elementary Particles and Decay Mechanisms

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The Kinetic Theory of Gases (1)

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From Maxwell to Higgs - James Clerk Maxwell Foundation

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E2-2004-4 M. I. Shirokov* DECAY LAW OF MOVING UNSTABLE

Elements of Statistical Mechanics
Elements of Statistical Mechanics

Feedback!control and! fluctuation!theorems! in! classical systems!
Feedback!control and! fluctuation!theorems! in! classical systems!

Wave Packets - Centro de Física Teórica
Wave Packets - Centro de Física Teórica

... Imagine an experiment where at instant t = 0 we measure the position of a quantum particle. The experiment is 100 times repeated. The time starts counting everytime at the beginning of the experiment. One obtains the following result. The particle is never found for x < −4.5, or for x > 5.5, 3 times ...
Gamow`s Theory of Alpha Decay
Gamow`s Theory of Alpha Decay

Chapter 5 The Wavelike - UCF College of Sciences
Chapter 5 The Wavelike - UCF College of Sciences

QUANTUM HETERODOXY: REALISM AT THE PLANK LENGTH Q
QUANTUM HETERODOXY: REALISM AT THE PLANK LENGTH Q

Macroscopic system: Microscopic system:
Macroscopic system: Microscopic system:

Particle Detectors - Forschungszentrum Jülich
Particle Detectors - Forschungszentrum Jülich



... direct test using inequalities (2), since none followed the scheme of Fig. 1 closely enough. Some experiments were performed with pairs of pho- ...
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Arrows of Time

Limits of classical physics II.
Limits of classical physics II.

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- EPJ Web of Conferences

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The energy conservation law in classical electrodynamics

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Chapter 13 Ideal Fermi gas

Full-Text PDF
Full-Text PDF

... the logarithm of the number of the accessible microstates in the phase space. The definition of the entropy is called Boltzmann entropy in which it is adopted in popular textbooks [1–4]. The microstates numbers for distinguishable and indistinguishable particles are certainly different and then thei ...
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Physical Composition

ppt 2.1MB - Weizmann Institute of Science
ppt 2.1MB - Weizmann Institute of Science

uncertainty: einstein, heisenberg, bohr, and the struggle for the soul
uncertainty: einstein, heisenberg, bohr, and the struggle for the soul

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Title of PAPER - Department of Physics and Astronomy

< 1 ... 67 68 69 70 71 72 73 74 75 ... 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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