Operators#
We have already seen examples of operators. For short, they consist of mathematical operations that can be carried out on functions. For example, the quantum mechanical momentum operator is:
When this operates on a function, it does the following: (1) differentiate the function with respect to
and then (2) multiply the result from (1) by .Another example of an operator is the position operator given just by coordinate
. This would operate on a given wavefunction just by multiplying it by . We denote operators with ^{} sign (``hat’’) above them.
Linearity of operators#
Operators in quantum mechanics are linear, which means that they fulfill the following rules:
and
Example Apply the following operators on the given functions:
Operator
and function .\Operator
and function .\Operator
and function .Operator
and function .Operator
and function .
Solution
. . . Note that is a constant. . .
Eigenvalue problem#
This is an eigenvalue problem where one needs to determine the eigenfunctions
and the eigenvalues . If is an eigenfunction of , operating with on it must yield a constant times .
Example What are the eigenfunctions and eigenvalues of operator
Solution Start with the eigenvalue equation:
Exepctation#
The eigenfunctions are
The last ``Bra - Ket’’ form is called the dirac notation. Note that the Bra part always contains the complex conjugation.
If
Note that operators and eigenfunctions may be complex valued; however, eigenvalues of quantum mechanical operators must be real because they correspond to values obtained from measurements. By allowing wavefunctions to be complex, it is merely possible to store more information in it (i.e., both the real and imaginary parts or ``density and velocity’’).
Hermitian property#
Operators that yield real eigenvalues are called hermitian . Operator
Note that this implies that the eigenvalues are real: Let
Example Prove that the momentum operator (in one dimension) is Hermitian.
Solution
Note that the wavefunctions approach zero at infinity and thus the boundary term in the integration by parts does not contribute. In 3-D, one would have to use the Green identities.
The Hermitian property can also be used to show that the eigenfunctions (
Here Hermiticity requires LHS = RHS. If
Note that if
The product
In practice, this means that we first operate with
If the commutator of
Example Prove that operators
Solution Let