Abstract
A basic postulate of wave mechanics is that the wave function of a microscopic system develops in time according to the equation iℏ∂ψ/∂
t
=
H
ψ, where
H
, the Hamiltonian, is an operator which in general depends upon the time. If, and only if, the Hamiltonian is time-independent, then the solutions of this equation take the form ψ(
q, t
) = ∑
n
c
n
Ѱ
n
(
q
)e
-1
E
n
t
/ℏ
, (2) where the individual terms
Ѱ
n
(
q
) are functions of the co-ordinates alone and the
E
n
are the corresponding eigenvalues of the Hamiltonian, satisfying
HѰ
n
=
E
n
Ѱ
n
. (3)
Cited by
9 articles.
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