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(This so-called degeneracy, the possession of the same energy by different wavefunctions, is also associated with the coincidental numerical agreement of Bohr's model with experiment).
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Also, the core idea that you can do quantum mechanics without wavefunctions is very different from other interpretations.
As a simple example we can consider a single particle whose wavefunction is different from zero only in two small and far apart regions h and t.
Spectacular images of multiparticle wavefunctions are obtained by purely optical means.
33 Electron density values, ρbcp, are computed at the BCP, and the corresponding HB energies EHB are estimated from the potential energy densities Vb. 34 In addition, NCI 35 analyses of the same wavefunctions were also performed by using the NCIPLOT 3.0 program, 36 to detect additional secondary interactions and to estimate their contributions.
However, for a larger value of the wavevector, the wavefunctions are only weakly affected by the field, due to the strong localization of the states.
The superposition principle states that linear combinations of wavefunctions are also valid wavefunctions.
Such macroscopic wavefunctions are the stuff which superconductors are made on.
With self-consistency established, the wavefunctions are available for detailed scrutiny.
In addition, the use of "fireball" wavefunctions, where the wavefunctions are explicitly zero beyond some cutoff, allows for pre-generating all integrals describing two- and three-center interactions.
Wavefunctions are highly localized in the dots.
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