Examples of using Wavefunctions in English and their translations into French
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Colloquial
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Official
The second step consists in assuming that the wavefunction of the system can be written as a Slater determinant of one-particle spin-orbitals.
beyond that of exchange energy resulting from the anti-symmetrization of the wavefunction, are completely neglected.
The intensity at the Raman resonance peaks is modulated by an envelope function which is related to the overlap integral of the electron and the hole wavefunction.
The ground state wavefunction for H2 at the equilibrium geometry is dominated by the configuration(φ1)2,
For energy eigenstates of the Schrödinger equation, the wavefunction is wavelike wherever the particle's energy is greater than the local potential, and exponential-like(evanescent)
These include Hartree-Fock theory, where the wavefunction is a single determinant,
the collapse of the wavefunction does not happen at any specific point in time,
If I wanted to use a computer to mathematically represent the electron wavefunction for a minuscule, nanometre-sized chunk of dust,
of configuration state functions(CSF) or configuration determinants to approximate the exact electronic wavefunction of an atom or molecule.
the same total wavefunction, total energy,
determinants and the basis functions in the molecular orbitals are varied to obtain the total electronic wavefunction with the lowest possible energy.
can separate via the wavefunction into three quasiparticles holon, spinon, orbiton.
this means that any evanescent portions of the wavefunction would be associated with a local negative mass-energy.
that every possibility at every interaction which is not forbidden by such a conservation law will actually happen in some branch of the wavefunction.
correlated wavefunction methods such as Coupled Clusters
identify the subtle signatures of a phase of matter, using the imperfect snapshots of the wavefunction.
These transformations leave the sum of the absolute square of the wavefunction components invariant, while they take states which are multiples of each other(including states which are imaginary multiples of each other)
Atomic wavefunctions and Hartree-Fock parameters of XeL and XeII atoms.
The theory is based on Bloch wavefunctions and is therefore only applicable to crystalline systems.
Thus we determine the Fourier components of the hole wavefunction in terms of the conduction band wavefunctions.