Molecular Quantum Mechanics
... examples to provide the reader with further opportunities to see formulae in action. We have added new problems for each chapter. We have expanded the discussion on numerous occasions within the body of the text to provide further clarification for or insight into mathematical results. We have set a ...
... examples to provide the reader with further opportunities to see formulae in action. We have added new problems for each chapter. We have expanded the discussion on numerous occasions within the body of the text to provide further clarification for or insight into mathematical results. We have set a ...
A controlled quantum system of individual neutral atoms
... The heart of our apparatus is an optical dipole trap which confines atoms in the antinodes of a far off-resonance standing wave. This type of trap relies on the dipole force, arising from inhomogeneous light fields. The first proposal of using this force to trap atoms was made by V. Letokhov already ...
... The heart of our apparatus is an optical dipole trap which confines atoms in the antinodes of a far off-resonance standing wave. This type of trap relies on the dipole force, arising from inhomogeneous light fields. The first proposal of using this force to trap atoms was made by V. Letokhov already ...
Quantum Designs - Gerhard Zauner
... To my suprise it was discovered there a few years later and several dozens of articles cited it since. This English translation shall help to make it easier accessible. Quantum Designs are sets of orthogonal projection matrices in finite dimensional Hilbert Spaces (I used the letter b for the dimens ...
... To my suprise it was discovered there a few years later and several dozens of articles cited it since. This English translation shall help to make it easier accessible. Quantum Designs are sets of orthogonal projection matrices in finite dimensional Hilbert Spaces (I used the letter b for the dimens ...
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... Many of the above applications make use of atomic ensembles rather than single atoms, in which case the complete quantum description of the ensemble–cavity interaction is nontrivial as it in general involves a very large Hilbert space (Baragiola et al., 2010). (Under assumptions of symmetry, exact s ...
... Many of the above applications make use of atomic ensembles rather than single atoms, in which case the complete quantum description of the ensemble–cavity interaction is nontrivial as it in general involves a very large Hilbert space (Baragiola et al., 2010). (Under assumptions of symmetry, exact s ...
Geometric Aspects and Neutral Excitations in the Fractional Quantum Hall Effect
... the non-commutative geometry of the fractional quantum Hall effects (FQHE) plays an important role in the intra-Landau-level dynamics. The geometrical aspects of the FQHE will be illustrated by calculating the linear response to a spatially varying electromagnetic field, and by a numerical scheme fo ...
... the non-commutative geometry of the fractional quantum Hall effects (FQHE) plays an important role in the intra-Landau-level dynamics. The geometrical aspects of the FQHE will be illustrated by calculating the linear response to a spatially varying electromagnetic field, and by a numerical scheme fo ...
W. Ketterle
... are called surface modes. In a semiclassical picture these excitations can be considered the mesoscopic counterpart to tidal waves at the macroscopic level. Those excitations are of special interest since they show a crossover between collective and single-particle behavior, which is crucial for the ...
... are called surface modes. In a semiclassical picture these excitations can be considered the mesoscopic counterpart to tidal waves at the macroscopic level. Those excitations are of special interest since they show a crossover between collective and single-particle behavior, which is crucial for the ...
Download! - Edhole.com
... n-type: a Si atom is replaced by P atom with an extra e-. The P atom is called donor p-type: a Si atom is replaced by B atom with an extra hole. The B atom is called acceptor ...
... n-type: a Si atom is replaced by P atom with an extra e-. The P atom is called donor p-type: a Si atom is replaced by B atom with an extra hole. The B atom is called acceptor ...
ןב תטיסרבינוא - בגנב ןוירוג
... polarizations are tunable by these fields, and do not depend on the energy of the scattered electrons. Moreover, when the spin filtering conditions are obeyed, one can tune the interferometer parameters (site and hopping energies) so that the transmission of the fully polarized electrons is close t ...
... polarizations are tunable by these fields, and do not depend on the energy of the scattered electrons. Moreover, when the spin filtering conditions are obeyed, one can tune the interferometer parameters (site and hopping energies) so that the transmission of the fully polarized electrons is close t ...
Mean-field theory of the Kondo effect in quantum dots with... Mikio Eto and Yuli V. Nazarov
... singlet and -triplet states are almost degenerate. We have calculated the Kondo temperature T K as a function of ⌬, using the ‘‘poor man’s’’ scaling method.22–24 We have shown that T K(⌬) is maximal around ⌬⫽0 and decreases with increasing ⌬ obeying a power law, T K(⌬)⬀1/⌬ ␥ . The exponent ␥ is not ...
... singlet and -triplet states are almost degenerate. We have calculated the Kondo temperature T K as a function of ⌬, using the ‘‘poor man’s’’ scaling method.22–24 We have shown that T K(⌬) is maximal around ⌬⫽0 and decreases with increasing ⌬ obeying a power law, T K(⌬)⬀1/⌬ ␥ . The exponent ␥ is not ...
Wave in disordered media and localisation phenomena
... measured. The spin-orbit scattering of the pure Mg is determined as discussed above. The different experimental curves for different temperatures are theoretically distinguished by their different H, (i.e. the inelastic lifetime). This is the only adjustable parameter for a comparison with theory (a ...
... measured. The spin-orbit scattering of the pure Mg is determined as discussed above. The different experimental curves for different temperatures are theoretically distinguished by their different H, (i.e. the inelastic lifetime). This is the only adjustable parameter for a comparison with theory (a ...
6 Product Operators
... these energy levels which are detected in spectroscopy. To understand the spectrum, therefore, it is necessary to have a knowledge of the energy levels and this in turn requires a knowledge of the Hamiltonian operator. In NMR, the Hamiltonian is seen as having a more subtle effect than simply determ ...
... these energy levels which are detected in spectroscopy. To understand the spectrum, therefore, it is necessary to have a knowledge of the energy levels and this in turn requires a knowledge of the Hamiltonian operator. In NMR, the Hamiltonian is seen as having a more subtle effect than simply determ ...
experimental atomic physics
... The following introduction to the subject of experimental atomic physics is based upon a course that has been given to seniors and first-year graduate students during the past few years at Princeton University. The purpose of the course has been to present the subject from a predominantly experiment ...
... The following introduction to the subject of experimental atomic physics is based upon a course that has been given to seniors and first-year graduate students during the past few years at Princeton University. The purpose of the course has been to present the subject from a predominantly experiment ...
Shor`s Factoring Algorithm and Modern Cryptography. An Illustration
... .Bob creates his RSA public key system in the following fashion7 : He first selects two different large prime numbers p and q, and then computes their product N = pq. Next he also computes the product φ = (p-1)(q-1) = N +1-(p+q), and then selects a positive integer e which is coprime to φ (meaning e ...
... .Bob creates his RSA public key system in the following fashion7 : He first selects two different large prime numbers p and q, and then computes their product N = pq. Next he also computes the product φ = (p-1)(q-1) = N +1-(p+q), and then selects a positive integer e which is coprime to φ (meaning e ...
Hydrogen atom
A hydrogen atom is an atom of the chemical element hydrogen. The electrically neutral atom contains a single positively charged proton and a single negatively charged electron bound to the nucleus by the Coulomb force. Atomic hydrogen constitutes about 75% of the elemental (baryonic) mass of the universe.In everyday life on Earth, isolated hydrogen atoms (usually called ""atomic hydrogen"" or, more precisely, ""monatomic hydrogen"") are extremely rare. Instead, hydrogen tends to combine with other atoms in compounds, or with itself to form ordinary (diatomic) hydrogen gas, H2. ""Atomic hydrogen"" and ""hydrogen atom"" in ordinary English use have overlapping, yet distinct, meanings. For example, a water molecule contains two hydrogen atoms, but does not contain atomic hydrogen (which would refer to isolated hydrogen atoms).