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The use of quantum mechanics was problematic in this regard, because the necessary mathematical calculations for describing the probability states (wave functions) of individual electrons in molecular systems are so complex.
The capability of the method to reproduce the non-stationary and non-Gaussian features of random phenomena is illustrated by applications to earthquakes (seismic ground motion) and sea states (wave heights).
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The latter option includes Dirac bound state wave functions.
Superimposed on the same graph is the ground state wave function calculated with N = 150.
Obviously, the ground-state wave function is maximized in CdTe layers compared to ZnSe.
A reliable and tractable technique for constructing the ground-state wave function by the superposition of nonorthogonal SDs is described.
The comparison includes scattering state, wave packet, and transient scattering state simulations in one and two space dimensions.
With a modest extension, the solver also allows for a linear stability analysis of the steady-state wave fields.
For the stationary state, invariance under time reversal implies that if u z) is a stationary-state wave function, then u∗ z) is also one.
The equation E1 can be interpreted in the following two different ways depending on the superpotential W x) or the ground state wave function.
where ψ n j B ( q j, t ) represent number state wave functions for each component of the decoupled systems described by Ĥ Bj.
Write better and faster with AI suggestions while staying true to your unique style.
Since I tried Ludwig back in 2017, I have been constantly using it in both editing and translation. Ever since, I suggest it to my translators at ProSciEditing.

Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com