No Slide Title
... the phaseonium as a high refractive index material. However, the control required by the Quantum Fredkin gate necessitates the atoms be in the GHZ state between level a and b Which could be possible for upto 1000 atoms. Question: Would 1000 atoms give sufficiently high refractive index? ...
... the phaseonium as a high refractive index material. However, the control required by the Quantum Fredkin gate necessitates the atoms be in the GHZ state between level a and b Which could be possible for upto 1000 atoms. Question: Would 1000 atoms give sufficiently high refractive index? ...
Lecture Notes for Chemistry 543, Part III
... The ± superscript refers to reflection symmetry of the electronic wave function. Although it applies to any value of Λ, it only appears in Σ states because the electronic eigenfunctions for Λ > 0 are actually superpositions of Λ+ and Λ− states. The ± superscript should not be confused with the ± pari ...
... The ± superscript refers to reflection symmetry of the electronic wave function. Although it applies to any value of Λ, it only appears in Σ states because the electronic eigenfunctions for Λ > 0 are actually superpositions of Λ+ and Λ− states. The ± superscript should not be confused with the ± pari ...
L10 QM H atom and spin
... where μB = eħ/2me is the Bohr magneton. How can we explain this effect? An electron moving in a circular orbit of radius r, at speed v, produces a current I = ev/2πr and a magnetic moment μz = I(πr2) = evr/2 = eLz/2me. Since Lz = mħ, we have μz = μBm. The corresponding extra potential term for the h ...
... where μB = eħ/2me is the Bohr magneton. How can we explain this effect? An electron moving in a circular orbit of radius r, at speed v, produces a current I = ev/2πr and a magnetic moment μz = I(πr2) = evr/2 = eLz/2me. Since Lz = mħ, we have μz = μBm. The corresponding extra potential term for the h ...
Physics 3 for Electrical Engineering
... where μB = eħ/2me is the Bohr magneton. How can we explain this effect? An electron moving in a circular orbit of radius r, at speed v, produces a current I = ev/2πr and a magnetic moment μz = I(πr2) = evr/2 = eLz/2me. Since Lz = mħ, we have μz = μBm. The corresponding extra potential term for the h ...
... where μB = eħ/2me is the Bohr magneton. How can we explain this effect? An electron moving in a circular orbit of radius r, at speed v, produces a current I = ev/2πr and a magnetic moment μz = I(πr2) = evr/2 = eLz/2me. Since Lz = mħ, we have μz = μBm. The corresponding extra potential term for the h ...
Quantum (wave) mechanics
... Quantum Mechanics Concepts In classical physics, given an initial position and initial velocity for a particle then if one knew the forces acting on the particle, Newton’s second law could be solved to accurately predict the position and velocity in the future. This concept is not true, especially i ...
... Quantum Mechanics Concepts In classical physics, given an initial position and initial velocity for a particle then if one knew the forces acting on the particle, Newton’s second law could be solved to accurately predict the position and velocity in the future. This concept is not true, especially i ...
Document
... Allowed values for K and J: both must, by conditions of quantum mechanics, be integral or zero. The total angular momentum can be as large as we like – i.e., (except that a real molecule will be disrupted at very high rotational speeds) Once we have chosen J, however, K is more limited. ...
... Allowed values for K and J: both must, by conditions of quantum mechanics, be integral or zero. The total angular momentum can be as large as we like – i.e., (except that a real molecule will be disrupted at very high rotational speeds) Once we have chosen J, however, K is more limited. ...
Alkali Elements Alkali Elements: Excited States
... Most of the energetics of these atoms is well described by the Hartree model; however, in detail (e.g. in high-resolution spectroscopy), spin-orbit coupling and the residual coulomb interaction are important. Residual Coulomb Interaction: The Coulomb interaction that is not captured by the effective ...
... Most of the energetics of these atoms is well described by the Hartree model; however, in detail (e.g. in high-resolution spectroscopy), spin-orbit coupling and the residual coulomb interaction are important. Residual Coulomb Interaction: The Coulomb interaction that is not captured by the effective ...
Quantum mechanics in one dimension
... Quantum mechanics in one dimension Following the rules of quantum mechanics, we have seen that the state of a quantum particle, subject to a scalar potential V (r), is described by the time-dependent Schrödinger equation, i!∂t Ψ(r, t) = ĤΨ(r, t) , ...
... Quantum mechanics in one dimension Following the rules of quantum mechanics, we have seen that the state of a quantum particle, subject to a scalar potential V (r), is described by the time-dependent Schrödinger equation, i!∂t Ψ(r, t) = ĤΨ(r, t) , ...
Momentum
... Momentum Momentum and changing momentum Momentum = mass x velocity (p = mv) Momentum is a vector quantity and is measured in Ns or kgms-1. ...
... Momentum Momentum and changing momentum Momentum = mass x velocity (p = mv) Momentum is a vector quantity and is measured in Ns or kgms-1. ...
