Ultra cold atoms and Bose-Einstein condensation for quantum
... comprehensive reviews and to other lecture notes for further details on atom cooling, trapping and Bose-Einstein condensation. ...
... comprehensive reviews and to other lecture notes for further details on atom cooling, trapping and Bose-Einstein condensation. ...
- TDDFT.org
... rpump ¼ 87 fs, and rprobe ¼ 50 fs. From these results we observe that the peaks corresponding to the first image potential state are obtained at the correct energy position. The signal due to the image states of higher quantum number cannot be distinguished due to the small difference in energy that c ...
... rpump ¼ 87 fs, and rprobe ¼ 50 fs. From these results we observe that the peaks corresponding to the first image potential state are obtained at the correct energy position. The signal due to the image states of higher quantum number cannot be distinguished due to the small difference in energy that c ...
5. Nuclear Structure
... – At short distances is stronger than the Coulomb force: we know that nuclei comprise tightly packed protons, thus to keep these protons together the nuclear force has to beat the Coulomb repulsion. – The nuclear force is short range. This is supported by the fact that interactions among e.g. two ...
... – At short distances is stronger than the Coulomb force: we know that nuclei comprise tightly packed protons, thus to keep these protons together the nuclear force has to beat the Coulomb repulsion. – The nuclear force is short range. This is supported by the fact that interactions among e.g. two ...
General properties of overlap operators in disordered quantum spin
... [13]. In classical disordered Ising spin systems, the overlap Ra,b satisfies the GhirlandaGuerra identities which are valid universally [13, 21]. Sometimes, these identities are called Aizenman-Contucci identities [1, 7]. The Ghirlanda-Guerra identities are useful to understand properties of the ran ...
... [13]. In classical disordered Ising spin systems, the overlap Ra,b satisfies the GhirlandaGuerra identities which are valid universally [13, 21]. Sometimes, these identities are called Aizenman-Contucci identities [1, 7]. The Ghirlanda-Guerra identities are useful to understand properties of the ran ...
PDF
... Measuring the amplitude and absolute phase of a microwave field at a specific point of space and time, has many potential applications, including precise qubit rotations1,2,3 and wavelength quantum teleportation4,5,6. One possible approach for such a measurement is the use of high-speed diodes; howe ...
... Measuring the amplitude and absolute phase of a microwave field at a specific point of space and time, has many potential applications, including precise qubit rotations1,2,3 and wavelength quantum teleportation4,5,6. One possible approach for such a measurement is the use of high-speed diodes; howe ...
Quantum Mechanics
... wavelengths. This phenomenon allows us to analyze the atmosphere of planets or galaxies simply by looking at the light being emitted from them. ...
... wavelengths. This phenomenon allows us to analyze the atmosphere of planets or galaxies simply by looking at the light being emitted from them. ...
Laser Molecular Spectroscopy CHE466 Fall 2007
... fact that a molecule contains more than one electron that is somehow shared at different extents by a set of nuclei. In addition, the interaction between electrons is difficult to represent. These problems translate in our inability to solve the Schrodinger equation exactly for a molecule. Furthermo ...
... fact that a molecule contains more than one electron that is somehow shared at different extents by a set of nuclei. In addition, the interaction between electrons is difficult to represent. These problems translate in our inability to solve the Schrodinger equation exactly for a molecule. Furthermo ...
DFT - ermes@unt
... Central equation in electronic structure theory. Depending on the level of approximation we find this equation all over: • Semi-empirical methods (empirical pseudopotentials, tight-binding) • Density Functional Theory • Hartree-Fock and beyond Mathematically speaking, we need to solve a generalized ...
... Central equation in electronic structure theory. Depending on the level of approximation we find this equation all over: • Semi-empirical methods (empirical pseudopotentials, tight-binding) • Density Functional Theory • Hartree-Fock and beyond Mathematically speaking, we need to solve a generalized ...
Article PDF - IOPscience
... and 3.34544 × 103 for B = 1, 5 × 105 , and 5 × 109 (a.u.), respectively. As B increases, the shape of the wave function becomes highly distorted and spindling along the z-axis. 3.2. Energy Spectral Curves of the Ground and Excited States Against the Strength of Magnetic Field Understanding the behav ...
... and 3.34544 × 103 for B = 1, 5 × 105 , and 5 × 109 (a.u.), respectively. As B increases, the shape of the wave function becomes highly distorted and spindling along the z-axis. 3.2. Energy Spectral Curves of the Ground and Excited States Against the Strength of Magnetic Field Understanding the behav ...
epl draft Optical traps for electron produced by Pauli blocking
... waves [16] following an original proposal by Ivanov and Littlewood [15]. The present scheme focuses on a different situation, the semiconductor being here doped with electrons at very low density. Unlike electron-hole plasma, excitons or polaritons, these electrons do not recombine but remain in the ...
... waves [16] following an original proposal by Ivanov and Littlewood [15]. The present scheme focuses on a different situation, the semiconductor being here doped with electrons at very low density. Unlike electron-hole plasma, excitons or polaritons, these electrons do not recombine but remain in the ...
Lecture 2 - Harvard Condensed Matter Theory group
... • Detection of many-body phases using noise correlations • Fermions in optical lattices Magnetism and pairing in systems with repulsive interactions. Current experiments: Mott state ...
... • Detection of many-body phases using noise correlations • Fermions in optical lattices Magnetism and pairing in systems with repulsive interactions. Current experiments: Mott state ...
Eigenstates of a small Josephson junction coupled to a resonant... W. A. Al-Saidi and D. Stroud
... Here Hphoton is the Hamiltonian of the cavity mode, which we express in the form Hphoton ⫽ប (a † a⫹1/2), where a † and a are the usual photon creation and annihilation operators. HJ is the Josephson coupling energy, which we write in the form HJ ⫽⫺J cos ␥, where J is the Josephson energy of the ju ...
... Here Hphoton is the Hamiltonian of the cavity mode, which we express in the form Hphoton ⫽ប (a † a⫹1/2), where a † and a are the usual photon creation and annihilation operators. HJ is the Josephson coupling energy, which we write in the form HJ ⫽⫺J cos ␥, where J is the Josephson energy of the ju ...