
1.1 Construction of two band models
... along the z direction. Here we have set to be . Let's denote the angular momentum operator along the z direction to be and we introduce a Zeeman type of Hamiltonian for the coupling ...
... along the z direction. Here we have set to be . Let's denote the angular momentum operator along the z direction to be and we introduce a Zeeman type of Hamiltonian for the coupling ...
PPT - Louisiana State University
... H.Cable, C.Wildfeuer, H.Lee, S.Huver, W.Plick, G.Deng, R.Glasser, S.Vinjanampathy, K.Jacobs, D.Uskov, JP.Dowling, P.Lougovski, N.VanMeter, M.Wilde, G.Selvaraj, A.DaSilva Not Shown: M.A. Can, A.Chiruvelli, GA.Durkin, M.Erickson, L. Florescu, M.Florescu, M.Han, KT.Kapale, SJ. Olsen, S.Thanvanthri, Z.W ...
... H.Cable, C.Wildfeuer, H.Lee, S.Huver, W.Plick, G.Deng, R.Glasser, S.Vinjanampathy, K.Jacobs, D.Uskov, JP.Dowling, P.Lougovski, N.VanMeter, M.Wilde, G.Selvaraj, A.DaSilva Not Shown: M.A. Can, A.Chiruvelli, GA.Durkin, M.Erickson, L. Florescu, M.Florescu, M.Han, KT.Kapale, SJ. Olsen, S.Thanvanthri, Z.W ...
Lectures 12-13
... One of these functions, the radial function, depends on two quantum numbers, n and l, while the other function depends on both l and m. The overall wavefunctions are labeled with all three quantum numbers n, l, and m. The eigenvalues of hydrogen-like atoms are given by the equation ...
... One of these functions, the radial function, depends on two quantum numbers, n and l, while the other function depends on both l and m. The overall wavefunctions are labeled with all three quantum numbers n, l, and m. The eigenvalues of hydrogen-like atoms are given by the equation ...
Syllabus: Quantum computing - University of Hawaii Physics and
... Topics in current theoretical research; e.g., quantum informational representations of field theories. This course is an introduction to quantum information theory (qubits, quantum gates, and qubit systems). It covers a few selected quantum algorithms, yet the emphasis of the course is on quantum si ...
... Topics in current theoretical research; e.g., quantum informational representations of field theories. This course is an introduction to quantum information theory (qubits, quantum gates, and qubit systems). It covers a few selected quantum algorithms, yet the emphasis of the course is on quantum si ...
pages 851-900 - Light and Matter
... both at once. The wave happily does its wave tricks, like superposition and interference, and the particle acts like a respectable particle, resolutely refusing to be in two different places at once. If the wave, for instance, undergoes destructive interference, becoming nearly zero in a particular ...
... both at once. The wave happily does its wave tricks, like superposition and interference, and the particle acts like a respectable particle, resolutely refusing to be in two different places at once. If the wave, for instance, undergoes destructive interference, becoming nearly zero in a particular ...
4.4 The Bohr Atom
... Again, it would be a good idea to read this section for ideas, but I won't test you on it. The main idea is that electrons and nuclei orbit each other. The much more massive nucleus moves very little, just as the earth does most of the orbiting around the sun. However, on the atomic scale, the corre ...
... Again, it would be a good idea to read this section for ideas, but I won't test you on it. The main idea is that electrons and nuclei orbit each other. The much more massive nucleus moves very little, just as the earth does most of the orbiting around the sun. However, on the atomic scale, the corre ...
energy levels
... half-filled sublevels are not as stable as filled sublevels, they are more stable than other configurations. ...
... half-filled sublevels are not as stable as filled sublevels, they are more stable than other configurations. ...
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.