As in the one-dimensional case, the element indices may be changed by changing the base address 'B'.

Therefore, the rest of the article focuses on the one-dimensional case.

It is also the completion of the Borel measure, as in the one-dimensional case.

The results above can be used to show that, contrary to the one-dimensional case, there is not always a bound state in a spherical cavity.

This is the stress-strain relationship in the one-dimensional case.

This definition includes the usual one-dimensional case, when the domain is taken to be the positive halfline.

For the one-dimensional case this number was given by a binomial distribution.

As in the one-dimensional case, the energy is quantized.

There is one further difference: in the one-dimensional case, each energy level corresponds to a unique quantum state.

For simplicity, we will consider the one-dimensional case.