tsuchiya
... Berenstein’s model Berenstein, Berenstein-Correa-Vazquez, Berenstein-Vazquez, Berenstein-Cotta, Berenstein-Cotta-Leonardi ...
... Berenstein’s model Berenstein, Berenstein-Correa-Vazquez, Berenstein-Vazquez, Berenstein-Cotta, Berenstein-Cotta-Leonardi ...
PhysRevB.89.020408 - FU Berlin
... many different magnetic orders are present [1,2], where an infinite number of degenerate ground states can be found [3]. From a theoretical perspective, not many rigorous results about the quantum phase diagram are known so far. Advanced mean field theories have provided important guidance as to wha ...
... many different magnetic orders are present [1,2], where an infinite number of degenerate ground states can be found [3]. From a theoretical perspective, not many rigorous results about the quantum phase diagram are known so far. Advanced mean field theories have provided important guidance as to wha ...
8 He - CEA-Irfu
... The GSM description is appropriate for modelling weakly bound nuclei with large radial extension. For 6He we observed an overall weak sensitivity for both correlation angle and charge radius. However, when adding 2 more neutrons in the system he details of each interaction are revealed. The next ...
... The GSM description is appropriate for modelling weakly bound nuclei with large radial extension. For 6He we observed an overall weak sensitivity for both correlation angle and charge radius. However, when adding 2 more neutrons in the system he details of each interaction are revealed. The next ...
Lec 6-7 - Theory of Condensed Matter
... In experiment, a beam of silver atoms were passed through inhomogeneous magnetic field and collected on photographic plate. Since silver involves spherically symmetric charge distribution plus one 5s electron, total angular momentum of ground state has L = 0. If outer electron in 5p state, L = 1 and ...
... In experiment, a beam of silver atoms were passed through inhomogeneous magnetic field and collected on photographic plate. Since silver involves spherically symmetric charge distribution plus one 5s electron, total angular momentum of ground state has L = 0. If outer electron in 5p state, L = 1 and ...
University of Toronto Strongly Repulsive Ultracold
... where n(i) are the lattice positions neighbouring i. In one dimension, this problem was solved by Ising, who discovered that there was no ferromagnetic transition in the model, from which he concluded that the simple Hamiltonian (1.3) could not explain ferromagnetic phase transitions. However, any h ...
... where n(i) are the lattice positions neighbouring i. In one dimension, this problem was solved by Ising, who discovered that there was no ferromagnetic transition in the model, from which he concluded that the simple Hamiltonian (1.3) could not explain ferromagnetic phase transitions. However, any h ...
PHZ 7427 SOLID STATE II: Electron-electron interaction and the
... other imperfections. Once a Friedel oscillation is formed, the effective potential barrier seen by other electrons is the sum of the bare potential plus the potential produced by the Friedel oscillation. Consider a simple example when 1D electrons interact via a contact potential U (x) = uδ (x) . Th ...
... other imperfections. Once a Friedel oscillation is formed, the effective potential barrier seen by other electrons is the sum of the bare potential plus the potential produced by the Friedel oscillation. Consider a simple example when 1D electrons interact via a contact potential U (x) = uδ (x) . Th ...
Spin current source based on a quantum point contact with local
... Let us first assume that the channel is homogenous (h̄ω = 0). The conductance without SO coupling depicted with the dashed curve in Fig. 2(a) has a sharp step-like dependence on the Fermi energy which corresponds to appearance of subsequent subbands at the Fermi level with increasing Ef and the resu ...
... Let us first assume that the channel is homogenous (h̄ω = 0). The conductance without SO coupling depicted with the dashed curve in Fig. 2(a) has a sharp step-like dependence on the Fermi energy which corresponds to appearance of subsequent subbands at the Fermi level with increasing Ef and the resu ...
Electromagnetic Study of the Chlorosome Antenna
... the pigment transitions due to the couplings between monomers. In order to understand which regions are of interest for energy transfer, we calculated the absorption and circular dichroism spectra of the structures. Due to the three-dimensional arrangement of the dipoles in a cylindrical structure, ...
... the pigment transitions due to the couplings between monomers. In order to understand which regions are of interest for energy transfer, we calculated the absorption and circular dichroism spectra of the structures. Due to the three-dimensional arrangement of the dipoles in a cylindrical structure, ...
Spectral Composition of Semantic Spaces
... whereas the less frequently encountered contexts may activate one of the four nominal and one verbal senses listed in WordNet. In other words, the term was correctly treated as a homonym by considering its senses as atoms in a molecule. Another example, the term courage does not have a true low-ener ...
... whereas the less frequently encountered contexts may activate one of the four nominal and one verbal senses listed in WordNet. In other words, the term was correctly treated as a homonym by considering its senses as atoms in a molecule. Another example, the term courage does not have a true low-ener ...
Excited state entanglement - FaMAF
... electron system as a function of the nuclear charge [5]. The ionization threshold, or critical point, for atomic-like systems is defined as the value of the nuclear charge for which a bound-state energy becomes absorbed or degenerate with the continuum. In [5] we have shown that the critical behavio ...
... electron system as a function of the nuclear charge [5]. The ionization threshold, or critical point, for atomic-like systems is defined as the value of the nuclear charge for which a bound-state energy becomes absorbed or degenerate with the continuum. In [5] we have shown that the critical behavio ...
Emergent quasicrystals in strongly correlated systems
... frustration between the lattice and magnetic length scales in the Hofstadter problem [27] gives rise to a fractal spectrum [28]. As we will describe in this work, naturally occurring strongly correlated electronic systems and other quantum theories having only ubiquitous kinetic hopping, Coulomb, an ...
... frustration between the lattice and magnetic length scales in the Hofstadter problem [27] gives rise to a fractal spectrum [28]. As we will describe in this work, naturally occurring strongly correlated electronic systems and other quantum theories having only ubiquitous kinetic hopping, Coulomb, an ...
Microwave Effect in Chemical Reactions Samuel P. Bowen1, David
... As will be discussed in the next section these non-adiabatic excited state probabilities will depend on certain matrix elements between the electronic states. This would imply that it may be possible to excite intermediate states that are quite different from the usual thermally e x c it e d states. ...
... As will be discussed in the next section these non-adiabatic excited state probabilities will depend on certain matrix elements between the electronic states. This would imply that it may be possible to excite intermediate states that are quite different from the usual thermally e x c it e d states. ...
file
... • A great advantage of the optimal control gate sequence is that the maximum exchange interaction is about 500 times smaller than the typical exchange interaction of J/h=10.2 GHz in the Kane’s originalproposal and yet the CNOT gate operation time is still 3 times faster than that in the globally con ...
... • A great advantage of the optimal control gate sequence is that the maximum exchange interaction is about 500 times smaller than the typical exchange interaction of J/h=10.2 GHz in the Kane’s originalproposal and yet the CNOT gate operation time is still 3 times faster than that in the globally con ...
III. Spin and orbital angular momentum
... Therefore, the force on the atom is parallel to ẑ and is given by Mz ∂B ∂z . The gradient ∂z is a property of the magnet used in the experiment and can be found by calibration. The deflection of the atom from the initial trajectory is therefore proportional to Mz . By measuring where the atom lands ...
... Therefore, the force on the atom is parallel to ẑ and is given by Mz ∂B ∂z . The gradient ∂z is a property of the magnet used in the experiment and can be found by calibration. The deflection of the atom from the initial trajectory is therefore proportional to Mz . By measuring where the atom lands ...
Spin squeezing and quantum correlations
... We have classified spin states into two mutually exclusive classes, namely, oriented and non-oriented states, and studied their squeezing properties. It is clear from our analysis that squeezing is exhibited only by non-oriented states. Considering in particular the nonoriented states of a spin-1 sy ...
... We have classified spin states into two mutually exclusive classes, namely, oriented and non-oriented states, and studied their squeezing properties. It is clear from our analysis that squeezing is exhibited only by non-oriented states. Considering in particular the nonoriented states of a spin-1 sy ...
S Heisenberg antiferromagnet layers
... mainly motivated by its relation to high-temperature superconductivity.1 According to the Mermin-Wagner theorem,2 the Néel antiferromagnetic 共AF兲 long-range order in 2D can exist only at zero temperature, but even then it can still be reduced by quantum fluctuations. It has been established that at ...
... mainly motivated by its relation to high-temperature superconductivity.1 According to the Mermin-Wagner theorem,2 the Néel antiferromagnetic 共AF兲 long-range order in 2D can exist only at zero temperature, but even then it can still be reduced by quantum fluctuations. It has been established that at ...
Magnetism and d-wave superconductivity on the half
... conductivity even at half-filling, provided the on-site interaction U / t is not too large. High-pressure studies that are common in the fields of heavy-fermion9,10 and organic superconductors5 have already revealed pressure-induced transitions in these compounds from antiferromagnetic insulators to ...
... conductivity even at half-filling, provided the on-site interaction U / t is not too large. High-pressure studies that are common in the fields of heavy-fermion9,10 and organic superconductors5 have already revealed pressure-induced transitions in these compounds from antiferromagnetic insulators to ...
Spin Transverse Force on Spin Current in an Electric Field
... hBi which contains the contribution from the SU(2) gauge field A as well as the conventional electromagnetic field. We have recovered the Ehrenfest theorem as one of the examples of the corresponding principle in quantum mechanics. The term, hrB Bi, results from the nonuniform magnetic field. ...
... hBi which contains the contribution from the SU(2) gauge field A as well as the conventional electromagnetic field. We have recovered the Ehrenfest theorem as one of the examples of the corresponding principle in quantum mechanics. The term, hrB Bi, results from the nonuniform magnetic field. ...
Phys. Rev. Lett. 110, 156402 - Institute for Quantum Optics and
... which satisfy the usual angular momentum commutation relations. The total system Hamiltonian can then be written as H ¼ !m ay a þ B Jz þ gðay J þ aJþ Þ; ...
... which satisfy the usual angular momentum commutation relations. The total system Hamiltonian can then be written as H ¼ !m ay a þ B Jz þ gðay J þ aJþ Þ; ...
