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[3. Schrödinger equations.]
Quantum operators.
An operator is a rule that transcripts (that is transforms) a given function
in another function. Quantum mechanics makes use of operator for translating
classical mechanical equations in quantum mechanical equations.
Let u be a classical mechanical quantity. Every classical mechanical
quantity is defined by position and momentum, so u is a function of
q and p :
u = u (q1 , q2 , q3 , p1 , p2 , p3)
In quantum mechanics, an operator uop corresponding to u is
defined by means of the following two rules acting on the equation
u = u (q1 , q2 , q3 , p1 , p2 , p3).
- Substitute every occurrences of qk with the operator
"multiplication by qk" and every occurrences of f (qk) with
the operator "multiplication by f (qk)".
- Substitute every occurrences of pkn with the operator
.
For example, let u be the mechanical energy E given by (3.3).
The operator Eop associated to E is:
.
Note that in (3.4) the expression U(q1 , q2 , q3) means
"multiply by U(q1 , q2 , q3) ".
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