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Relativistic Description of Two-body Scattering
Relativistic Description of Two-body Scattering

Classical phase-space analysis of vibronically coupled systems
Classical phase-space analysis of vibronically coupled systems

... distribution centered at x(0) = 3, which corresponds to the ground state of the harmonicoscillator potential. ...
Comment on “Non-representative Quantum Mechanical Weak Values”
Comment on “Non-representative Quantum Mechanical Weak Values”

Complementarity in Quantum Mechanics and Classical Statistical
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... the dynamical state of a microparticle by methods of classical mechanics, then precision of such description is limited. In fact, the classical state of microparticle turns out to be badly defined. While the coordinate-momentum uncertainty forbids the classical notion of trajectory, the energy-time u ...
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Particle Spin and the Stern

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Quantum Mechanical Laws

... the energy hν , above the minimum necessary to leave the metal. Despite this, the experimentalists tried to check whether the light absorption in the photoeffect, had no characteristics of a continuous accumulation. In crucial experiments (Joffe 1913; Meyer and Gerlach 1914), the light beam was fall ...
A maximality result for orthogonal quantum groups
A maximality result for orthogonal quantum groups

Optical probing of the spin state of a single magnetic impurity in a
Optical probing of the spin state of a single magnetic impurity in a

... ⬍ 0, where the parameter W0 contains the interband optical matrix element Pcv between the Bloch states. At the same time, the average spin of the photoexcited hole is ...
Approximate solutions to the quantum problem of two opposite
Approximate solutions to the quantum problem of two opposite

Integrated optomechanics and linear optics quantum circuits
Integrated optomechanics and linear optics quantum circuits

... • Very good sensitivity ...
Quantum Mechanical Laws
Quantum Mechanical Laws

Is Quantum Indeterminism Relevant to Free Will?
Is Quantum Indeterminism Relevant to Free Will?

New Spin-Orbit-Induced Universality Class in the Integer Quantum Hall Regime
New Spin-Orbit-Induced Universality Class in the Integer Quantum Hall Regime

... Thus, for short-range correlations, calculations suggest the existence of a band of weakly localized states. It is interesting to compare our results with previous works. Lee [7] and Hanna et al. [8] studied a Hamiltonian with a spin-dependent term Hr  S, in which Hr is a random field that coup ...
Electronic transport for armchair graphene nanoribbons with a
Electronic transport for armchair graphene nanoribbons with a

test 3 practice
test 3 practice

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Qualification Exam: Quantum Mechanics
Qualification Exam: Quantum Mechanics

... µ-meson; suppose these particles are both in their lowest energy states. Give reasons why the electron wave function can be approximated as Ψe = π −1/2 ae−3/2 e−r/ae while the µ-meson wave function is approximately Ψµ = π −1/2 23/2 aµ−3/2 e−2r/aµ Here ae and aµ are the Bohr radii for the electron an ...
Edge States and Contacts in the Quantum Hall Effect
Edge States and Contacts in the Quantum Hall Effect

Topological Chern Indices in Molecular Spectra
Topological Chern Indices in Molecular Spectra

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Quantum Theories of Mind

... but observation changes quanta. 6000 (c), 40000 (d), 140000 (e). Thus, we cannot say they are what we observe prior to their being observed. Quantum observations are like asking leading questions. In doing so, we give information that can influence the answer. So we can’t be sure the answer reflects ...
Steven Simon
Steven Simon

... Numerical work by Rezayi, Haldane, Morf, and others strongly suggests that… ...
PEPS, matrix product operators and the Bethe ansatz
PEPS, matrix product operators and the Bethe ansatz

... – The properties of such a state are described by a (1+1) dimensional theory (eigenvectors of transfer matrices) – Those eigenvectors are well described by MPS – Properties of MPS are trivial to calculate: reduction to a partition function of a 1-D system (1+0) ...
Quantum Computing Using Linear Optics
Quantum Computing Using Linear Optics

... of single photons, as illustrated in Fig. 1a. Polarizationencoded qubits are more resistant to certain kinds of experimental errors and easier to manipulate than the “path-encoded” qubits of Fig. 1b. The use of polarization-based qubits allowed us to design a CNOT gate using only two polarizing beam ...
Analog Quantum Simulators - Kirchhoff
Analog Quantum Simulators - Kirchhoff

Meson-Baryon and Baryon-Antiharyon Ratios in Two Way Quark
Meson-Baryon and Baryon-Antiharyon Ratios in Two Way Quark

Quantum Computation with Topological Phases of Matter
Quantum Computation with Topological Phases of Matter

... tected from scattering. Theory and experiments have found an important new family of such materials. Topological insulators are materials with a bulk insulating gap, exhibiting quantum-Hall-like behaviour in the absence of a magnetic field. Such systems are thought to provide an avenue for the reali ...
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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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