case

[see also: event, possibility]

We first do the case $n=1$.

This argument also settles the case of $K= \Gamma$.

We finish by mentioning that, suitably modified, the results of Section 2 apply to the $AP$ case.

Note that (4) covers the other cases.

There are several cases to consider: ......

We close this article by addressing, in part, the case of what happens if we replace the map $T$ by convolution.

There are quite a number of cases, but they can be described reasonably systematically.

The general case follows by changing $x$ to $x-a$.

This abstract theory is not in any way more difficult than the special case of the real line.

Important cases are where $S=$ ......

This case arises when ......

Both cases can occur.

To deal with the zero characteristic case, let ......

Then either ......, or ...... In the latter $\langle$former$\rangle$ case, ......

In the case of finite additivity, we have ......

In the case of $n\ge 1$ $\langle$In case $n\ge 1\rangle$, ...... [ Better: If $n\geq 1$ then ......]

In the case where $A$ is commutative, as it will be in most of this paper, we have ......

We shall assume that this is the case.

It cannot be that there exists $x \in \Omega \setminus F$, for otherwise $\theta(\delta_x) = \kappa_E(\delta_x) =0$, which is not the case.

Unfortunately, this is rarely the case.

However, it need not be the case that $V> W$, as we shall see in the following example.

Such was the case in (8).

The $L^2$ theory has more symmetry than is the case in $L^1$.

Note that some of the $a_n$ may be repeated, in which case $B$ has multiple zeros at those points.

This is handled by a direct case-by-case argument.

a classic $\langle$textbook/typical/borderline/simple/extreme/rare/striking$\rangle$ case

We use upper case letters to represent inverses of generators. [= capital letters]



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