
Classical phase-space analysis of vibronically coupled systems
... distribution centered at x(0) = 3, which corresponds to the ground state of the harmonicoscillator potential. ...
... distribution centered at x(0) = 3, which corresponds to the ground state of the harmonicoscillator potential. ...
Complementarity in Quantum Mechanics and Classical Statistical
... 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 ...
... 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 ...
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 ...
... 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 ...
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 ...
... ⬍ 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 ...
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 ...
... 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 ...
test 3 practice
... time of its construction? (half life of 14C = 5 730 years) a. 0.425 b. 0.500 c. 0.517 d. 0.696 ____ 30. Approximately how many radioactive atoms are present in a tritium sample with an activity of 0.4 × 10−6 Ci and a half-life of 12.3 years? (1 Ci = 3.7 × 1010 decays/s) a. 1.3 × 108 b. 7 × 108 c. 3 ...
... time of its construction? (half life of 14C = 5 730 years) a. 0.425 b. 0.500 c. 0.517 d. 0.696 ____ 30. Approximately how many radioactive atoms are present in a tritium sample with an activity of 0.4 × 10−6 Ci and a half-life of 12.3 years? (1 Ci = 3.7 × 1010 decays/s) a. 1.3 × 108 b. 7 × 108 c. 3 ...
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 ...
... 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 ...
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 ...
... 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 ...
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) ...
... – 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
... 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 ...
... 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 ...
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 ...
... 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 ...
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.