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Basic Properties of Operators
Most of the properties of operators are obvious, but they are summarized
below for completeness.
- The sum and difference of two operators
and
are given by
- The product of two operators is defined by
![\begin{displaymath}\hat{A} \hat{B} f \equiv \hat{A} [ \hat{B} f ]
\end{displaymath}](/Quantum%20Mechanics/Tutorial/notes/quantum_doc/img58.png) |
(35) |
- Two operators are equal if
 |
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for all functions f.
- The identity operator
does nothing (or multiplies by 1)
 |
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A common mathematical trick is to write this operator as a sum over a
complete set of states (more on this later).
 |
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- The associative law holds for operators
 |
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- The commutative law does not generally hold for operators.
In general,
.
It is convenient to
define the quantity
![\begin{displaymath}[\hat{A}, \hat{B}]\equiv \hat{A} \hat{B} - \hat{B} \hat{A}
\end{displaymath}](/Quantum%20Mechanics/Tutorial/notes/quantum_doc/img65.png) |
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which is called the commutator of
and
.
Note
that the order matters, so that
.
If
and
happen to commute, then
.
- The n-th power of an operator
is defined as nsuccessive applications of the operator, e.g.
 |
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- The exponential of an operator
is defined via
the power series
 |
(42) |
Next: Linear Operators
Up: Operators
Previous: Operators and Quantum Mechanics