
my Work 4 U
... Pauli's Principle means that can be only two electrons for any given values of n, l and ml; one has spin 1/2 and the other 1/2. Similarly, for any given values of n and l, there can only be 2l +1 pairs of electrons, corresponding to the allowable values of ml. ...
... Pauli's Principle means that can be only two electrons for any given values of n, l and ml; one has spin 1/2 and the other 1/2. Similarly, for any given values of n and l, there can only be 2l +1 pairs of electrons, corresponding to the allowable values of ml. ...
Elementary Particle Mixing for Maximum Channel Capacity in Measured Decays
... and momentum; and that the generational (u,c,t), (d,s,b), (e,µ,τ ), (νe ,νµ ,ντ ) elementary fermionic patterns complement spin. In this picture fermionic generations arise as a Poincare group representation that generalizes the natural left-right mixing in the Dirac equation. This paper further con ...
... and momentum; and that the generational (u,c,t), (d,s,b), (e,µ,τ ), (νe ,νµ ,ντ ) elementary fermionic patterns complement spin. In this picture fermionic generations arise as a Poincare group representation that generalizes the natural left-right mixing in the Dirac equation. This paper further con ...
Communicating Research to the General Public
... ultraviolet radiation, which has a shorter wavelength, and thus more energy per photon, than visible light or infrared light. Ozone accomplishes this task because light in that range of wavelengths matches the separation between energy levels in the ozone molecules (we would say that the light is re ...
... ultraviolet radiation, which has a shorter wavelength, and thus more energy per photon, than visible light or infrared light. Ozone accomplishes this task because light in that range of wavelengths matches the separation between energy levels in the ozone molecules (we would say that the light is re ...
Development of electrostatically controlled quantum Hall
... for [M n1 ] and dχ/dn > 0 for [M n2 ] for the back gate. For the formation of well defined h-DWs we want to control B ∗ with a minimal change of n in order to remain at the same filling factor ν, or maximize |dχ/dn|. Quantum Hall effect in sample A is shown in Fig. 3a. A small peak at B ∗ = 7 Tesla ...
... for [M n1 ] and dχ/dn > 0 for [M n2 ] for the back gate. For the formation of well defined h-DWs we want to control B ∗ with a minimal change of n in order to remain at the same filling factor ν, or maximize |dχ/dn|. Quantum Hall effect in sample A is shown in Fig. 3a. A small peak at B ∗ = 7 Tesla ...
Stopping Potential
... When I started this unit, I hoped to finally quell a lot of confusion in this area for myself. But what I have found so far, I now have more questions than when I started. Like a Feynman question…. The truth is that a lot of this is still being debated. Much of it is based on Math that you won’t see ...
... When I started this unit, I hoped to finally quell a lot of confusion in this area for myself. But what I have found so far, I now have more questions than when I started. Like a Feynman question…. The truth is that a lot of this is still being debated. Much of it is based on Math that you won’t see ...
Free Fields - U.C.C. Physics Department
... In the real world, the effect is due to the vacuum fluctuations of the electromagnetic field, with the boundary conditions imposed by conducting plates. Here we model this effect with a scalar. But there is a problem. E is infinite! What to do? The problem comes from the arbitrarily high momentum mo ...
... In the real world, the effect is due to the vacuum fluctuations of the electromagnetic field, with the boundary conditions imposed by conducting plates. Here we model this effect with a scalar. But there is a problem. E is infinite! What to do? The problem comes from the arbitrarily high momentum mo ...
O_4 Theory (III) QUANTUM MECHANICAL STUDY OF THE FLEISCHMANN-PONS EFFECT
... under the conditions of the FPE cell, is extremely small. As stated in ref. [1], “it is necessary to reconsider the quantum mechanics of electrons and deuterons in such host lattices.” The goal of this paper is to predict possible changes in the probability of d-d fusion, caused by perturbations to ...
... under the conditions of the FPE cell, is extremely small. As stated in ref. [1], “it is necessary to reconsider the quantum mechanics of electrons and deuterons in such host lattices.” The goal of this paper is to predict possible changes in the probability of d-d fusion, caused by perturbations to ...
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.