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here - islam-science.net
here - islam-science.net

Slide 101
Slide 101

- Snistnote
- Snistnote

January - Life Learning Cloud
January - Life Learning Cloud

June 2006 - 6677 Mechanics M1 - Question paper
June 2006 - 6677 Mechanics M1 - Question paper

Read Notes #1 - Faculty Website Listing
Read Notes #1 - Faculty Website Listing

Quantum states
Quantum states

CS267: Introduction - UCSD Department of Physics
CS267: Introduction - UCSD Department of Physics

Physics 535 lecture notes: - 10 Oct 4th, 2007 Homework: 6.2, 6.3
Physics 535 lecture notes: - 10 Oct 4th, 2007 Homework: 6.2, 6.3

We live in the quantum 4-dimensional Minkowski space-time
We live in the quantum 4-dimensional Minkowski space-time

Lab: Atoms and Eggs—Datasheet Name___________________
Lab: Atoms and Eggs—Datasheet Name___________________



slides
slides

Atom Notes
Atom Notes

Heisenburg uncertainty principle
Heisenburg uncertainty principle

...  Their model defines the laws for all known interactions except gravity. ...
Antimatter
Antimatter

... Electrons he visualised as spinning like tiny gyroscopes but surprisingly they always have the same amount of “angular momentum” Which we now call spin. ...
GonzalesMestres
GonzalesMestres

... shower maximum and its fluctuations indicate a trend toward heavy nuclei with increasing energy. Although the measurements available now are only up to about 55 EeV, the trend suggests that primary CRs are likely to be dominated by heavy nuclei at higher energies. This interpretation of the shower d ...
Talk, 15 MB - Seth Aubin - College of William and Mary
Talk, 15 MB - Seth Aubin - College of William and Mary

3 - Sezione di Fisica
3 - Sezione di Fisica

Spin excitations and many particle effects in molecules studied with
Spin excitations and many particle effects in molecules studied with

Lecture 4
Lecture 4

... Questions for the class Is ground state of helium triplet, singlet, or can be either one and can not be determined from the given information? The helium excited states have form one electron in the ground state and one electron in the excited state. Do these states have to be singlet, triplet state ...
Diffusion of Individual Atoms
Diffusion of Individual Atoms

Beyond the Cookie Cutter Paradigm
Beyond the Cookie Cutter Paradigm

... The possibility of re-identification may exist for two reasons, either because the two particles possess distinguishing properties or because they are distinct substances to which proper names can be permanently attached. In reality the possibility of reidentification does not exist, and this means ...
1 16. The grand canonical ensemble theory for a system in
1 16. The grand canonical ensemble theory for a system in

ORMEs -- Superconductive but maybe not Monatomic
ORMEs -- Superconductive but maybe not Monatomic

< 1 ... 112 113 114 115 116 117 118 119 120 ... 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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