92, 075445 (2015)
... (2) Moreover, also in a general fashion, we demonstrate that the intrinsic behavior of excitations within and in the vicinity of the light cone would be that of the 2D exciton polaritons as determined by the full electromagnetic (rather than just electrostatic [23]) coupling of valley excitons takin ...
... (2) Moreover, also in a general fashion, we demonstrate that the intrinsic behavior of excitations within and in the vicinity of the light cone would be that of the 2D exciton polaritons as determined by the full electromagnetic (rather than just electrostatic [23]) coupling of valley excitons takin ...
Lecture notes
... The text is somewhat easier to read than H & M and is more up-to-date (2008) (e.g. neutrino oscillations) but on the other hand has a somewhat less robust treatment in deriving the equations. The introduction chapter of this book gives a very readable popular history of particle physics. ...
... The text is somewhat easier to read than H & M and is more up-to-date (2008) (e.g. neutrino oscillations) but on the other hand has a somewhat less robust treatment in deriving the equations. The introduction chapter of this book gives a very readable popular history of particle physics. ...
Destructive quantum interference in spin tunneling problems
... In this Letter we point out that when there are several different symmetry-related tunneling paths connecting the same degenerate classical ground states, the topological phase can lead to destructive quantum interference between their amplitudes, and hence to a total tunneling amplitude that is exa ...
... In this Letter we point out that when there are several different symmetry-related tunneling paths connecting the same degenerate classical ground states, the topological phase can lead to destructive quantum interference between their amplitudes, and hence to a total tunneling amplitude that is exa ...
Early-stage relaxation of hot electrons by LO phonon emission Herve´ Castella
... 共SBE’s兲, which give the time evolution of the density distributions in both bands, and of the interband polarization.4 The scattering processes, however, are taken into account by instantaneous scattering rates as in Boltzmann equations, thus treating relaxation as totally incoherent and energy cons ...
... 共SBE’s兲, which give the time evolution of the density distributions in both bands, and of the interband polarization.4 The scattering processes, however, are taken into account by instantaneous scattering rates as in Boltzmann equations, thus treating relaxation as totally incoherent and energy cons ...
A study of the electron structure of endohedrally confined atoms
... where U0 is the well depth of the square well and is the thickness of equation (1), while it is assumed that w0 = U0 . Following Connerade et al [38], it is assumed that = 1 Å, leading σ = 0.57 Å to the C60 cage. This choice is rather arbitrary, and there are other possibilities. One eventuall ...
... where U0 is the well depth of the square well and is the thickness of equation (1), while it is assumed that w0 = U0 . Following Connerade et al [38], it is assumed that = 1 Å, leading σ = 0.57 Å to the C60 cage. This choice is rather arbitrary, and there are other possibilities. One eventuall ...
Chapter 13 Radioactive Decay
... the remaining discussion, that Nf represents the ground state. In (13.15) we see that the energy of the γ is given by the difference in energies of the two nuclear states, less the recoil energy, Ef imparted to the daughter (resultant) nucleus. If the energy of the excited state is uncertain, we kno ...
... the remaining discussion, that Nf represents the ground state. In (13.15) we see that the energy of the γ is given by the difference in energies of the two nuclear states, less the recoil energy, Ef imparted to the daughter (resultant) nucleus. If the energy of the excited state is uncertain, we kno ...
Multiphoton localization and propagating quantum gap solitons in a
... We evaluate the dispersion relations, the effective masses, and the dissociation energies of quantum gap solitons and we show that they are stable with respect to weak perturbations. Our results demonstrate a clear distinction, at the quantum level, between fermionic gap systems (such as electronic ...
... We evaluate the dispersion relations, the effective masses, and the dissociation energies of quantum gap solitons and we show that they are stable with respect to weak perturbations. Our results demonstrate a clear distinction, at the quantum level, between fermionic gap systems (such as electronic ...
In-medium
... 1. Introduction to charm (bottom) nuclei 2. Mass formula with 1/mQ expansion 3. Anti-D (B) meson in nuclear medium - Heavy meson effective theory with 1/M corretions ...
... 1. Introduction to charm (bottom) nuclei 2. Mass formula with 1/mQ expansion 3. Anti-D (B) meson in nuclear medium - Heavy meson effective theory with 1/M corretions ...
Regular/irregular phase space structure of HCN/HNC
... Eighty vibrational levels were computed covering an energy region up to 18 500 cm - I (energies are measured from the minimum of the potential except if it is stated otherwise) the highest of these are converged to within 10 cm - I. Quantum 3D calculations have performed by Bacic and Light17 for 110 ...
... Eighty vibrational levels were computed covering an energy region up to 18 500 cm - I (energies are measured from the minimum of the potential except if it is stated otherwise) the highest of these are converged to within 10 cm - I. Quantum 3D calculations have performed by Bacic and Light17 for 110 ...
Improve The Convergence of Jarzynski Equality through Fast
... The discovery of Jarzynski equality signifies that people have a much deeper understanding on nonequilibrium statistical mechanics and thermodynamics. Its application is, however, often limited by its poor convergence. To resolve the problem, physicists have made a lot of efforts [11, 12] and have m ...
... The discovery of Jarzynski equality signifies that people have a much deeper understanding on nonequilibrium statistical mechanics and thermodynamics. Its application is, however, often limited by its poor convergence. To resolve the problem, physicists have made a lot of efforts [11, 12] and have m ...
SELECTED ANSWERS
... The Lewis structure shows the two O–H covalent bonds and the two lone pairs on the oxygen atom. The space-filling model provides the most accurate representation of the electron charge clouds for the atoms and the bonding electrons. The ball-and-stick model emphasizes the molecule’s correct molecula ...
... The Lewis structure shows the two O–H covalent bonds and the two lone pairs on the oxygen atom. The space-filling model provides the most accurate representation of the electron charge clouds for the atoms and the bonding electrons. The ball-and-stick model emphasizes the molecule’s correct molecula ...
Hexagonal Plaquette Spin-spin Interactions and Quantum
... constraints imposed by the first term in the Hamiltonian, i.e., i∈7 Szi = 0. Hence, the ground state configurations are such that each hexagon in a Kagome lattice consists of three up spins and three down spins. This is reminiscent of the ice rule in spinice models [3, 4] in which, close to each ver ...
... constraints imposed by the first term in the Hamiltonian, i.e., i∈7 Szi = 0. Hence, the ground state configurations are such that each hexagon in a Kagome lattice consists of three up spins and three down spins. This is reminiscent of the ice rule in spinice models [3, 4] in which, close to each ver ...