There are three simplest forms for function operators which we shall see over and over again in this course, the constant operator, the argument multiplication operator and the differential operator. These are described in detail in the three paragraphs below.
One of the simplest function operators with which we shall deal is just multiplication of the input function by some constant, c. We would then write this operator as so that the action of is just
Note that, with the hat ``on,'' is an operator whereas with the hat ``off'' c is just a constant number which is multiplying . Two very importation constant operators are the zero operator , whose operation on any function returns the zero function, , and the unit operator whose action on any function is to ``do nothing'' or just return the input function back as output, .
We saw an example of our next more complicated operator in our first expression for Here is derived from by multiplication of by its argument x. For this new function operator, we write so that the action of on is just
We now may rewrite our expression for the average position as The same type of operation occurs in the calculation of the average momentum within the momentum representation. In this case we define so that
and . Note that we put the tilde ``'' on the p below the hat to remind us that this operator is defined for use in the momentum representation.
We also had an expression for the average position computed within the momentum representation, . Here, is derived from using the yet more complicated operation of differentiation. We now write as a differential operator so that the action of is just
and the average position computed in the momentum representation is . (Again, we put the tilde ``'' on the x to remind us that this operator is defined for use in the momentum representation.) Finally, to complete the set of average-operator correspondences, for computing the average momentum from within the position representation we define a second differential operator so that
and