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Supplementary Material
Supplementary Material

+1/2 - WordPress.com
+1/2 - WordPress.com

... Calculation of Nα/Nβ What would be the value of DE for protons if Bo = 9.4 T. It is 4 x 10-5 Kcal / mol. What is the frequency, ν, ? (400MHz ?) Use this equation for energy: ∆E = hgB0/2π And this for frequency: ν = gB0/2π Then use this for Boltzmann Excess: Nα/Nβ = 1 + ∆E/kT Or Nα/Nβ = 1 + hν/kT Th ...
Polarized excitons in nanorings and the optical Aharonov
Polarized excitons in nanorings and the optical Aharonov

... to measure the relative phases of alternative paths in electronic interferometers,6 and proposed as a mechanism to distinguish singlet and triplet states in coupled quantum dots in connection with their use in solid state quantum computers.7,8 Excitons in quantum dots with a few tens of nanometers i ...
Low-Energy Excitations and Ground State Selection in Quantum
Low-Energy Excitations and Ground State Selection in Quantum

... was then used to calculate the thermodynamic properties of the Hamiltonian Eq. (1) and a comparison to experiment was made. Figure 3(a) shows the heat capacity calculated using Eq. (1), together with that measured in a previous study18 . The data is reasonably reproduced by the calculation for T ≥ 1 ...
Problem Set 11 Solutions - Illinois State Chemistry
Problem Set 11 Solutions - Illinois State Chemistry

Deconfined Quantum Criticality
Deconfined Quantum Criticality

The rotation of a homonuclear linear molecule
The rotation of a homonuclear linear molecule

... not required (recall that for an IR vibrational mode to be active it is necessary only that it should have an oscillating dipole moment). Electronic transitions don’t even need that, and the H2 molecule does have a UV spectrum. Electronic energy levels are split by the molecule’s vibration, and for ...
ESI Bose-Einstein Condensation as a Quantum Phase Transition in an Optical Lattice
ESI Bose-Einstein Condensation as a Quantum Phase Transition in an Optical Lattice

PPTX
PPTX

Report - IISER Pune
Report - IISER Pune

... if we pass a stream of atoms possessing nonzero magnetic moments is directed to pass through a nonuniform magnetic field, the magnetic forces involved will split up the stream into a number of substreams , with one substream for each possible value of the z-component of µ (usually written as µz ). S ...
Low-energy spectrum and finite temperature properties of quantum
Low-energy spectrum and finite temperature properties of quantum

... a radial mode. The ring radius can be related to the onedimensional density parameter rs . The resulting relations are R = N rs /π and ω0 = CF ~2 π 2 /(32mrs2 ). The Heisenberg coupling energy of the model Hamiltonian can be fitted to the splitting of the lowest band (vibrational ground state) at a ...
Document
Document

VI. ELECTRONIC SPECTROSCOPY The visible (V) and ultraviolet
VI. ELECTRONIC SPECTROSCOPY The visible (V) and ultraviolet

... cannot cause ISC (unless the two electrons have different g-factors) because it is homogeneous on a molecular scale, affects both spins equally, and cannot twist one spin relative to the other. However, a magnetic field from within a molecule may be able to rephase the spins. For example, the spin-o ...
Quantum Hall effect
Quantum Hall effect

... This means that to pass from one IQHE state to another requires a quantum phase transition: this corresponds to the point at which the edge state delocalizes and “percolates” through the bulk ...
Latest Lattice Results for Baryon Spectroscopy
Latest Lattice Results for Baryon Spectroscopy

Atomic Spectra - Rutgers Physics
Atomic Spectra - Rutgers Physics

Giant spin Seebeck effect in a non
Giant spin Seebeck effect in a non

ppt - Harvard Condensed Matter Theory group
ppt - Harvard Condensed Matter Theory group

IR Optical Taggants
IR Optical Taggants

letters - mceuen group
letters - mceuen group

Rubidium 87 D Line Data
Rubidium 87 D Line Data

... In this reference we present many of the physical and optical properties of 87 Rb that are relevant to various quantum optics experiments. In particular, we give parameters that are useful in treating the mechanical effects of light on 87 Rb atoms. The measured numbers are given with their original r ...
EXCHANGE CONTRIBUTIONS TO SPIN POLARIZATION IN LOW
EXCHANGE CONTRIBUTIONS TO SPIN POLARIZATION IN LOW

Quantum Hall effect and the topological number in graphene
Quantum Hall effect and the topological number in graphene

Section 1.6 - 1 1.6 Term Symbols A brief general review of atomic
Section 1.6 - 1 1.6 Term Symbols A brief general review of atomic

... Total Angular Momentum in Many Electron Atoms: Finding J and MJ Applying the Russel-Saunders Scheme: to our C example… • As the carbon atom is a light atom we can now use the Russell-Saunders coupling scheme to account for spin-orbit coupling and its effects. • Considering only the 9 microstates of ...
Lecture 3
Lecture 3

< 1 ... 30 31 32 33 34 35 36 37 38 ... 61 >

Nitrogen-vacancy center



The nitrogen-vacancy center (N-V center) is one of numerous point defects in diamond. Its most explored and useful property is photoluminescence, which can be easily detected from an individual N-V center, especially those in the negative charge state (N-V−). Electron spins at N-V centers, localized at atomic scales, can be manipulated at room temperature by applying a magnetic field, electric field, microwave radiation or light, or a combination, resulting in sharp resonances in the intensity and wavelength of the photoluminescence. These resonances can be explained in terms of electron spin related phenomena such as quantum entanglement, spin-orbit interaction and Rabi oscillations, and analysed using advanced quantum optics theory. An individual N-V center can be viewed as a basic unit of a quantum computer, and it has potential applications in novel, more efficient fields of electronics and computational science including quantum cryptography and spintronics.
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