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Ch.1 Identical particles
Ch.1 Identical particles

The Bohr Atom
The Bohr Atom

... in the case of the hydrogen atom, as the electron loses energy, it moves into an orbit of smaller radius, loses energy more rapidly and spirals into the nucleus within about 10−10 seconds. This cannot be correct since atoms certainly exist. This problem was solved by Bohr in an remarkable leap of th ...
Clustering of Particles in Turbulent Flows
Clustering of Particles in Turbulent Flows

... Particles move in a less dense fluid with velocity field Particles do not affect the velocity field, or interact (until they make contact). The equation of motion is assumed to be ...
Collective atomic recoil laser: an example of classical
Collective atomic recoil laser: an example of classical

Atoms
Atoms

r2 - SIUE
r2 - SIUE

Ensembles(b)
Ensembles(b)

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

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

Document
Document

Jon Abbatt - Earth, Atmospheric, and Planetary Physics
Jon Abbatt - Earth, Atmospheric, and Planetary Physics

Decoherence in Excited Atoms by Low-Energy Scattering
Decoherence in Excited Atoms by Low-Energy Scattering

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

... exerted by our model gas. This calculation will demonstrate how to tackle calculations of this type in kinetic theory. We consider the behaviour of a small number of typical particles and use Newton’s laws of mechanics to calculate their behaviour. We then average over all the particles using the di ...
ELEMENTARY PARTICLES OF MAXIMALLY LARGE MASSES
ELEMENTARY PARTICLES OF MAXIMALLY LARGE MASSES

lecture_11
lecture_11

Creation and Annihilation Operators
Creation and Annihilation Operators

... ◦ Obviously, HFS can contain linear combinations of states with different numbers of particles. While this may at first seem strange, it is no more “unnatural” than harmonic oscillator states, such as coherent states, that do not contain a definite number of phonons. Allowing the number of particles ...
Second Quantization
Second Quantization

Physics 102: Lecture 24 Heisenberg Uncertainty Principle Physics
Physics 102: Lecture 24 Heisenberg Uncertainty Principle Physics

Anyons in the fractional quantum Hall effect
Anyons in the fractional quantum Hall effect

Atomic Theory Review
Atomic Theory Review

Atomic Theory Review - hrsbstaff.ednet.ns.ca
Atomic Theory Review - hrsbstaff.ednet.ns.ca

Document
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Particle Physics Notes
Particle Physics Notes

... He plotted the spin ½ baryons and spin 0 mesons in so-called octets. There is a similarity between Mendeleev’s periodic table of elements and the super multiples of particles of Gell Mann. Both pointed out a deeper structure of matter. The strangeness QN is plotted vertically and decreases from 0 t ...
1 Introduction 2 Symmetry Under Interchange
1 Introduction 2 Symmetry Under Interchange

Lecture11
Lecture11

< 1 ... 3 4 5 6 7 8 9 10 11 ... 18 >

Geiger–Marsden experiment



The Geiger–Marsden experiment(s) (also called the Rutherford gold foil experiment) were a landmark series of experiments by which scientists discovered that every atom contains a nucleus where its positive charge and most of its mass are concentrated. They deduced this by measuring how an alpha particle beam is scattered when it strikes a thin metal foil. The experiments were performed between 1908 and 1913 by Hans Geiger and Ernest Marsden under the direction of Ernest Rutherford at the Physical Laboratories of the University of Manchester.
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