Examples of using Wave functions in English and their translations into Portuguese
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Bosons, such as the photon,have symmetric wave functions instead.
Wave functions corresponding to a state are accordingly not unique.
As the spacing between the two atoms becomes smaller, the electron wave functions begin to overlap.
Each set of wave functions with the same value of n is called a Landau level.
The method is based on the partial-wave expansion(pwe) andthe translational addition theorem for spherical wave functions.
The term encompass both the wave functions of the electrons and the energies associated with them.
Comparing the quantum dots size to the Bohr radius of the electron and hole wave functions, 3 regimes can be defined.
Exact wave functions, however, cannot generally be expressed as single determinants.
The starting point for the Hartree-Fock method is a set of approximate one-electron wave functions known as spin-orbitals.
Particles with wave functions symmetric under exchange are called bosons.
The description of these states, however,represent a great challenge since they require wave functions which are difficult to obtain and high energies sources.
Particles with wave functions antisymmetric under exchange are called fermions.
For a molecular orbital or crystalline calculation, the initial approximate one-electron wave functions are typically a linear combination of atomic orbitals LCAO.
For the wave functions, recall that p^ y{\displaystyle{\hat{p}}_{y}} commutes with the Hamiltonian.
In this formulation, the incident plane wave, as well as the scattering field, is expanded into radiating spherical vector wave functions.
To determine the entropy,we utilize the wave functions and probability densities for both the atomic models.
Each energy eigenfunction is assumed to be describable by a single Slater determinant,an antisymmetrized product of one-electron wave functions i.e..
Solutions of this equation are wave functions which can be used to describe the probability density of a particle.
Parallel worlds are generated in a manner similar to quantum superposition and decoherence,with all states of the wave functions being realized in separate worlds.
A correlation between their wave functions remained, as they were once part of the same wave-function that was not disturbed before one of the child particles was measured.
What results is, in e¨ect,that the only interactions which occur in the theoretical context under consideration involve strictly proca¿elds and wave functions for grávitons.
Typically, in modern Hartree-Fock calculations, the one-electron wave functions are approximated by a linear combination of atomic orbitals.
Edward Witten published a paper in response to Lee Smolin's,arguing that the Kodama state is unphysical, due to an analogy to a state in Chern-Simons theory wave functions, resulting in negative energies.
The basic point is the coincidence of the initial and final state many-body wave functions in the two types of processes and the formal similarity of the transition operators.
The wave functions were expanded in terms of plane waves with a cutoff energy of 25 ry, 400 a.u. f ictitious mass and a cutoff energy of 100 ry for the charge density expansion.
In 1927, D. R. Hartree introduced a procedure, which he called the self-consistent field method,to calculate approximate wave functions and energies for atoms and ions.
It follows from general symmetry principles that the wave functions can be characterized by their symmetry behavior with respect to space inversion r formula_13-r.
Abstract Quantum cosmology driven by minisuperespace models allows for the construction andanalysis of the behavior of the wave functions(of the Universe) obtained from the Wheeler-DeWitt formulation WDW.
It follows from general symmetry principles that the wave functions can be characterized by their symmetry behavior with respect to the point group inversion operation i r↦-r.
This was the first attempt to describe many-electron systems on the basis of electronic density instead of wave functions, although it was not very successful in the treatment of entire molecules.