PDF
... the third-order nonlinearity (χ(3) ) of the material (silica glass in the case of optical fibers) to generate two daughter photons, called signal and idler photons, respectively. The frequencies of the daughter photons are symmetrically displaced from the pump frequency, satisfying the energy conser ...
... the third-order nonlinearity (χ(3) ) of the material (silica glass in the case of optical fibers) to generate two daughter photons, called signal and idler photons, respectively. The frequencies of the daughter photons are symmetrically displaced from the pump frequency, satisfying the energy conser ...
arXiv:1504.04012v1 [cond-mat.quant
... tunneling, and can provide another mechanism to break the boson-parity symmetry, while the quantum dimension in Eq. (13) will not be a↵ected. Preparation and detection.—There is some evidence that a ⌫ = 1/2 fractional Chern insulator has a continuous transition to a BEC, which allows for quasi-adiab ...
... tunneling, and can provide another mechanism to break the boson-parity symmetry, while the quantum dimension in Eq. (13) will not be a↵ected. Preparation and detection.—There is some evidence that a ⌫ = 1/2 fractional Chern insulator has a continuous transition to a BEC, which allows for quasi-adiab ...
Formal Theory of Green Functions
... is an eigenstate of H or is commutab le medium. Since the state I with H, the function V(x) is independe nt of time. On the other hand V(x) is naturally reduced to a constant independe nt of x if G is uniform in space, in other words, if the medium is in an eigenstate of the total momentum operator ...
... is an eigenstate of H or is commutab le medium. Since the state I with H, the function V(x) is independe nt of time. On the other hand V(x) is naturally reduced to a constant independe nt of x if G is uniform in space, in other words, if the medium is in an eigenstate of the total momentum operator ...
ppt - Quark Matter 2005
... We explicitly treat the mass-change of pions (e.g., due to chiralsymmetry breaking) as they pass from the hot, dense collision medium [m(p)0]) to the outside vacuum [m(p)140 MeV]. This is accomplished by solving the Klein-Gordon equation with an optical potential, the real part of which is a deep, ...
... We explicitly treat the mass-change of pions (e.g., due to chiralsymmetry breaking) as they pass from the hot, dense collision medium [m(p)0]) to the outside vacuum [m(p)140 MeV]. This is accomplished by solving the Klein-Gordon equation with an optical potential, the real part of which is a deep, ...
Topological Phases of Matter classification and application
... ground state manifold is an analogue of the configuration space and the “first” excited states are the phase space. (excitations form an analogue of the tangent bundle) • In 2D, to first approximation, long ranged entanglement pattern is encoded by a unitary modular category: D,S,T,… ...
... ground state manifold is an analogue of the configuration space and the “first” excited states are the phase space. (excitations form an analogue of the tangent bundle) • In 2D, to first approximation, long ranged entanglement pattern is encoded by a unitary modular category: D,S,T,… ...
PDF only - at www.arxiv.org.
... scale, we apply his approach to the polarizability and the VdW force though expressed by the exact wavefunctions to calculate 2D dipoles and eigenenergies. This is expected to bring in improvements to the symbolistics, though still retaining the typical uncertainties characteristic of the 2nd order ...
... scale, we apply his approach to the polarizability and the VdW force though expressed by the exact wavefunctions to calculate 2D dipoles and eigenenergies. This is expected to bring in improvements to the symbolistics, though still retaining the typical uncertainties characteristic of the 2nd order ...
Strong coupling: Infrared limit of integrable quantum system MRL of
... In collinear limit only single particle excitations w. X = F± contribute ...
... In collinear limit only single particle excitations w. X = F± contribute ...
Particle Creation in Inflationary Spacetime
... From here on the Lagrangian density L will be called Lagrangian. An equation of motion can be determined by the principle of least action: δS = 0. ...
... From here on the Lagrangian density L will be called Lagrangian. An equation of motion can be determined by the principle of least action: δS = 0. ...
Equivalence between free quantum particles and those in harmonic
... are one and the same. This knowledge helps us to understand either from the viewpoint of the other. Here we show that all general time-dependent solutions of the free-particle Schrödinger equation can be mapped to solutions of the Schrödinger equation for harmonic potentials, both the trapping osc ...
... are one and the same. This knowledge helps us to understand either from the viewpoint of the other. Here we show that all general time-dependent solutions of the free-particle Schrödinger equation can be mapped to solutions of the Schrödinger equation for harmonic potentials, both the trapping osc ...
presentation pdf - EMERGENT QUANTUM MECHANICS
... These are the LOCAL expressions for the energy-momentum of the particle. Conservation of energy is maintained through the quantum Hamilton-Jacobi equation. Similar relations hold for the Pauli and Dirac particles. ...
... These are the LOCAL expressions for the energy-momentum of the particle. Conservation of energy is maintained through the quantum Hamilton-Jacobi equation. Similar relations hold for the Pauli and Dirac particles. ...
SELECTED TOPICS IN QUANTUM MECHANICS Pietro Menotti
... 1. Two states of the same physical system, produced by two different preparing apparatus will be considered the same state if they give rise to the same statistical distributions of results when measuring any measurable quantity. 2. We assume that it is meaningful to consider linear superposition of ...
... 1. Two states of the same physical system, produced by two different preparing apparatus will be considered the same state if they give rise to the same statistical distributions of results when measuring any measurable quantity. 2. We assume that it is meaningful to consider linear superposition of ...
Full text in PDF form
... κ by the relation κ ∼ T ∼ (GM )−1 , where M is the mass of the black hole [2]. Such a result has been obtained also for Rindler space-time [3, 4, 5, 6, 7], corresponding to an accelerating observer, with the difference that the surface gravity is replaced by the acceleration a of the observers (κ → ...
... κ by the relation κ ∼ T ∼ (GM )−1 , where M is the mass of the black hole [2]. Such a result has been obtained also for Rindler space-time [3, 4, 5, 6, 7], corresponding to an accelerating observer, with the difference that the surface gravity is replaced by the acceleration a of the observers (κ → ...
Stability of Complex Biomolecular Structures: van der Waals
... HB angles to lower values in the quantum case. It is hard to observe any other very pronounced effect except perhaps for a small shift to shorter O···H distances in the quantum case. Compared to Figure 3c middle and lower panels (AIMD and AI-TRPMD), this means that we would either need much more samp ...
... HB angles to lower values in the quantum case. It is hard to observe any other very pronounced effect except perhaps for a small shift to shorter O···H distances in the quantum case. Compared to Figure 3c middle and lower panels (AIMD and AI-TRPMD), this means that we would either need much more samp ...
Parton model from bi-local solitonic picture of the baryon in two-dimensions
... scattering; QCD; Structure functions ...
... scattering; QCD; Structure functions ...
Spectral Analysis of Nonrelativistic Quantum Electrodynamics
... In this lecture I review the progress achieved during the past decade on the mathematical description of quantum mechanical matter interacting with the quantized radiation field. My main focus will be on the results I have obtained in collaboration with Jürg Fröhlich and Israel Michael Sigal [8, 9 ...
... In this lecture I review the progress achieved during the past decade on the mathematical description of quantum mechanical matter interacting with the quantized radiation field. My main focus will be on the results I have obtained in collaboration with Jürg Fröhlich and Israel Michael Sigal [8, 9 ...