User contributions for StephanieReynolds
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27 June 2011
- 09:0509:05, 27 June 2011 diff hist +11 One-Dimensional Bound States →Infinite square well
- 09:0309:03, 27 June 2011 diff hist −40 One-Dimensional Bound States No edit summary
26 June 2011
- 17:5417:54, 26 June 2011 diff hist +2 m Some Consequences of the Uncertainty Principle No edit summary
- 17:5417:54, 26 June 2011 diff hist −75 Some Consequences of the Uncertainty Principle No edit summary
- 17:5117:51, 26 June 2011 diff hist +74 Some Consequences of the Uncertainty Principle No edit summary
- 17:4817:48, 26 June 2011 diff hist −180 Heisenberg Uncertainty Principle No edit summary
- 17:4517:45, 26 June 2011 diff hist +1 m Heisenberg Uncertainty Principle No edit summary
- 17:4417:44, 26 June 2011 diff hist −30 m Heisenberg Uncertainty Principle No edit summary
- 17:4117:41, 26 June 2011 diff hist +69 Heisenberg Uncertainty Principle No edit summary
- 17:3617:36, 26 June 2011 diff hist +22 m The Schrödinger Equation in Dirac Notation No edit summary
- 17:3517:35, 26 June 2011 diff hist +108 The Schrödinger Equation in Dirac Notation No edit summary
- 17:2617:26, 26 June 2011 diff hist +6 Relation Between the Wave Function and Probability Density No edit summary
- 17:1917:19, 26 June 2011 diff hist −1 m Stationary States No edit summary
- 17:1917:19, 26 June 2011 diff hist −53 Stationary States No edit summary
- 17:1717:17, 26 June 2011 diff hist +83 Stationary States No edit summary
- 17:1417:14, 26 June 2011 diff hist +67 Brief Derivation of Schrödinger Equation No edit summary
- 17:0717:07, 26 June 2011 diff hist 0 m Brief Derivation of Schrödinger Equation No edit summary
- 17:0517:05, 26 June 2011 diff hist +4 Brief Derivation of Schrödinger Equation No edit summary
- 17:0517:05, 26 June 2011 diff hist +2 m Brief Derivation of Schrödinger Equation No edit summary
25 June 2011
- 13:1313:13, 25 June 2011 diff hist +76 Original Idea of Schrödinger Equation No edit summary
24 June 2011
- 16:0016:00, 24 June 2011 diff hist +37 The Philosophy of Quantum Theory No edit summary
- 15:4015:40, 24 June 2011 diff hist +23 Stern-Gerlach Experiment →The discovery of spin
- 15:3015:30, 24 June 2011 diff hist 0 Stern-Gerlach Experiment No edit summary
- 15:2915:29, 24 June 2011 diff hist +13 Stern-Gerlach Experiment →External Links
- 15:2915:29, 24 June 2011 diff hist +19 Stern-Gerlach Experiment No edit summary
- 15:1715:17, 24 June 2011 diff hist +13 Double Slit Experiment No edit summary
- 15:1415:14, 24 June 2011 diff hist +5 m Double Slit Experiment No edit summary
- 15:0515:05, 24 June 2011 diff hist +4 m Stability of Matter No edit summary
- 15:0315:03, 24 June 2011 diff hist −5 Stability of Matter No edit summary
- 15:0115:01, 24 June 2011 diff hist +4 Stability of Matter No edit summary
- 14:5914:59, 24 June 2011 diff hist +103 Physical Basis of Quantum Mechanics No edit summary
- 14:5714:57, 24 June 2011 diff hist +1 Photoelectric Effect No edit summary
- 14:5414:54, 24 June 2011 diff hist +74 Photoelectric Effect No edit summary
21 June 2011
- 11:1711:17, 21 June 2011 diff hist +78 Basic Concepts and Theory of Motion No edit summary
- 11:1511:15, 21 June 2011 diff hist −1 Commutation Relations and Simultaneous Eigenvalues →Commutator=
- 11:1111:11, 21 June 2011 diff hist 0 m Basic Concepts and Theory of Motion No edit summary
- 11:1011:10, 21 June 2011 diff hist +68 Basic Concepts and Theory of Motion No edit summary
- 11:0011:00, 21 June 2011 diff hist +29 Basic Concepts and Theory of Motion No edit summary
- 11:0011:00, 21 June 2011 diff hist +83 m Basic Concepts and Theory of Motion No edit summary
19 June 2011
- 23:1223:12, 19 June 2011 diff hist +4,056 N Two particle scattering New page: Image:particle scattering.jpg Classically, if we wish to consider a collection of identical particles, say billiard balls, it is always possible to label all the balls such that we ca...
- 23:1123:11, 19 June 2011 diff hist +8,470 N Coulomb Potential Scattering New page: '''Example 1''' Let's look at an example of a Screened Coulomb (Yukawa) Potential, where we have a potential: :<math>V(r)=V_0e^{-\alpha r}\frac{1}{r}</math> The scattering amplitude can ...
- 23:1123:11, 19 June 2011 diff hist +6,598 N Born Approximation and Examples of Cross-Section Calculations New page: In scattering theory, especially in quantum menchanics, the Born approximation consists of taking the incident field in place of the total field as the driving field at each point in the s...
- 23:1023:10, 19 June 2011 diff hist +13,055 N Central Potential Scattering and Phase Shifts New page: Recall that for scattering, we have Green function method :<math>\psi_k =\psi_k^{(0)} +\int d^3 r' G(\mathbf r,\mathbf r')V(\mathbf r')\psi_k (\mathbf r'),</math> where the Green's functio...
- 23:0923:09, 19 June 2011 diff hist +9,796 N Differential Cross Section and the Green's Function Formulation of Scattering New page: Much of what we know about forces and interactions in atoms and nuclei has been learned from scattering experiments, in which say atoms in the target are bombarded with beams of particles....
- 23:0823:08, 19 June 2011 diff hist +1,373 N Continuous Eigenvalues and Collision Theory New page: In this chapter we shall investigate problems connected with a particle which, coming from infinity, encounters or "collides with" some atomic system and, after being scattered through a c...
- 23:0723:07, 19 June 2011 diff hist +34 N Central Forces New page: Introduction------------------etc.
- 23:0723:07, 19 June 2011 diff hist +903 N WKB in Spherical Coordinates New page: It is possible to apply WKB to the radial equation using a method by R. E. Langer (1937). Recall: <math>\ u(r)=rR(r)</math>, <math>\left[ -\frac{\hbar^2}{2m}\frac{\partial^2}{\part...
- 23:0623:06, 19 June 2011 diff hist +7,173 N Hydrogen Atom New page: [http://wiki.physics.fsu.edu/wiki/index.php/Phy5645/HydrogenAtomProblem Worked Problem] involving the hydrogen atom. Another [http://wiki.physics.fsu.edu/wiki/index.php/Phy5645/HydrogenAt...
- 23:0623:06, 19 June 2011 diff hist +3,866 N Isotropic Harmonic Oscillator New page: The radial part of the Schrodinger's Equation for a particle of mass M in an isotropic harmonic oscillator potential <math>V(r)=\frac{1}{2}Mw^{2}r^2</math> is given by: :<math>-\frac{\hb...
- 23:0523:05, 19 June 2011 diff hist +2,555 N Spherical Well New page: Let's consider spherical well potentials, :<math> V(\mathbf{r}) = \begin{cases} V_0, & 0\leq r< a \\ 0, & r>a \end{cases} </math> The schrodinger equations for these two regions can be ...
