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... 45. A particle is in a potential V(x)=V0sin( 2x / a ), which is invariant under the transformation x→x+ma, where m is an integer. Is momentum conserved? Discuss the eigenvalues and eigenstates of the one-dimensional Hamiltonian. 46. Let R( ,n) be the operator that rotates a vector by about the ...
... 45. A particle is in a potential V(x)=V0sin( 2x / a ), which is invariant under the transformation x→x+ma, where m is an integer. Is momentum conserved? Discuss the eigenvalues and eigenstates of the one-dimensional Hamiltonian. 46. Let R( ,n) be the operator that rotates a vector by about the ...
KS-DFT formalism
... has invaded our thinking is marked by our constant use of concepts which have meaning only in terms of independent particle wave functions: shell structure, the occupation number, the Fermi sea and the Fermi surface, the representation of perturbation theory by Feynman diagrams. All of these concept ...
... has invaded our thinking is marked by our constant use of concepts which have meaning only in terms of independent particle wave functions: shell structure, the occupation number, the Fermi sea and the Fermi surface, the representation of perturbation theory by Feynman diagrams. All of these concept ...
wave function
... The Heisenberg Uncertainty Principle states if a measurement of the position of a particle is made with uncertainty Dx and a simultaneous measurement of its x component of momentum is made with uncertainty Dp, the product of the two uncertainties can never be smaller ...
... The Heisenberg Uncertainty Principle states if a measurement of the position of a particle is made with uncertainty Dx and a simultaneous measurement of its x component of momentum is made with uncertainty Dp, the product of the two uncertainties can never be smaller ...
Slide 1
... atoms Worked w/ all atoms e- in orbitals e- clouds Can not pinpoint location of e- and path at a given ...
... atoms Worked w/ all atoms e- in orbitals e- clouds Can not pinpoint location of e- and path at a given ...
HOMEWORK ASSIGNMENT 12
... magnetic dipole moments for the |200i → |100i, |210i → |100i, and |211i → |100i transitions in hydrogen. Be sure to show your work. For the electric dipole moments, we need to compute ehi|Z|f i = ehi|R cos Θ|f i. The selection rules are mf = mi and Lf = Li ± 1. Of these three transitions, only |210i ...
... magnetic dipole moments for the |200i → |100i, |210i → |100i, and |211i → |100i transitions in hydrogen. Be sure to show your work. For the electric dipole moments, we need to compute ehi|Z|f i = ehi|R cos Θ|f i. The selection rules are mf = mi and Lf = Li ± 1. Of these three transitions, only |210i ...
The Wave
... the wave theory of light. So other experiments were done and found it could behave as both:: 1) The Photo-Electric Effect (particle) 2) The Compton Effect (particle) 3) Taylor’s experiment (wave) 4) DeBroglie Wavelength (wave) ...
... the wave theory of light. So other experiments were done and found it could behave as both:: 1) The Photo-Electric Effect (particle) 2) The Compton Effect (particle) 3) Taylor’s experiment (wave) 4) DeBroglie Wavelength (wave) ...
PHYS 305 - Modern Physics (Spring 2016) Department of Physics
... The following general education goals and objective will be addressed by this course: • Effective communication through speaking and writing. • Critical thinking and problem solving. • Incorporate computational intelligence and knowledge for solving problems. METHODS OF EVALUATION Homework for each ...
... The following general education goals and objective will be addressed by this course: • Effective communication through speaking and writing. • Critical thinking and problem solving. • Incorporate computational intelligence and knowledge for solving problems. METHODS OF EVALUATION Homework for each ...
Particle in a box

In quantum mechanics, the particle in a box model (also known as the infinite potential well or the infinite square well) describes a particle free to move in a small space surrounded by impenetrable barriers. The model is mainly used as a hypothetical example to illustrate the differences between classical and quantum systems. In classical systems, for example a ball trapped inside a large box, the particle can move at any speed within the box and it is no more likely to be found at one position than another. However, when the well becomes very narrow (on the scale of a few nanometers), quantum effects become important. The particle may only occupy certain positive energy levels. Likewise, it can never have zero energy, meaning that the particle can never ""sit still"". Additionally, it is more likely to be found at certain positions than at others, depending on its energy level. The particle may never be detected at certain positions, known as spatial nodes.The particle in a box model provides one of the very few problems in quantum mechanics which can be solved analytically, without approximations. This means that the observable properties of the particle (such as its energy and position) are related to the mass of the particle and the width of the well by simple mathematical expressions. Due to its simplicity, the model allows insight into quantum effects without the need for complicated mathematics. It is one of the first quantum mechanics problems taught in undergraduate physics courses, and it is commonly used as an approximation for more complicated quantum systems.