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Two-level quantum dot in the Aharonov–Bohm ring. Towards understanding “phase lapse”  P.
Two-level quantum dot in the Aharonov–Bohm ring. Towards understanding “phase lapse” P.

... functions under assumption that the γ = 1 QD level is well coupled to the leads and active in electron transport, whereas γ = 2 level wave function has only a small, finite overlap with the states in the leads but does not directly participate in transport. It is indirectly coupled to the γ = 1 leve ...
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Full Text PDF

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... 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 ...
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... what will you see from each atom? A. All atoms will emit the same colors. B. Atom 1 will emit more colors than 2 which will emit more colors than 3 C. Atom 3 will emit more colors than 2 which will emit more colors than 1 D. Atom 3 will emit more colors than 2. Atom 1 will emit no colors. E. Impossi ...
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... Note that we could have written X(x) = Ae±ikx , but we can get both choices of sign by choosing k positive or negative, so for simplicity we drop the ±. Keep in mind, though, that for a given ! there are two independent solutions for X(x), namely e±i|k|x . Since is complex-valued, there is no obviou ...
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... in the quantum realm, where phasesensitive measurements are crucial, both for fundamental studies of quantum physics6 and for future communication applications. Zhang et al. have analysed a particular type of homodyne detector in which one of the outputs of the mixing beam splitter is detected by ei ...
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... Protons and neutrons are moving in opposite directions (the opposite phase keeps the center of mass of the nucleus stationary) or “out of phase” with respect to each other g isovector mode of excitation. Note: if protons and neutrons are moving in phase, it is an isoscalar dipole vibration (entire ...
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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.
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