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Requirements for an Acceptable Wave Function

In solving the particle in a box, we required ij/ to be continuous. We now discuss other requirements the wave function must satisfy. [Pg.57]

Since i/ p dr is a probability, we want to be able to normalize the wave function by choosing a suitable normalization constant N as multiplier of the wave function. If (// is unnormalized and Ntft is normalized, the normalization condition (3.59) gives [Pg.57]

In addition to demanding that tp be continuous, we usually also require that all the partial derivatives dtp/dx, dtp/dy, and so on, be continuous. (See Fig. 3.4.) Referring back to Section 2.2, however, we note that for the particle in a box dtp/dx is discontinuous at the walls of the box tp and dtp/dx are zero everywhere outside the box, but from Eq. (2.23) we see that dtp/dx does not become zero at the walls. The discontinuity in tp  [Pg.57]

FIGURE 3.4 Function (a) is continuous and its first derivative is continuous. Function (b) is continuous, but its first derivative has a discontinuity. Function (c) is discontinuous. [Pg.58]

We require that the eigenfunctions of any operator representing a physical quantity meet the above requirements. A function meeting these requirements is said to be well-behaved. [Pg.58]


See other pages where Requirements for an Acceptable Wave Function is mentioned: [Pg.57]    [Pg.57]    [Pg.54]   


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