In the modern physics, there are several anomaly.
Gauge anomaly : this terminology is used to describe the situation that classical theory has some gauge symmetry but it becomes anomalous in quantum theory. If gauge symmetry has an anomaly, a theory does not hold an unitality or renormalizability, so Gauge anomaly must be cancelled. (See anomaly cancellation.)
Global anomaly by a dynamical gauge field: this type of anomaly is known as ABJ anomaly. It describes the situation that classical theory has some global symmetry $G$ but it becomes anomalous in quantum theory by some dynamical gauge field. Here, we note that this dynamical gauge field is not necessarily the gauge field for the classical symmetry $G$ that we are now considering. This is main deference compared to the ‘t Hooft anomaly that we consider at the third pert. Also, this anomaly does not make a serious problem like a breaking of unitality. In this sense, it simply tells that classical symmetry is not necessarily a symmetry of quantum theory.
Global anomaly by a background gauge field: this type of anomaly is called as the ‘t Hooft anomaly. It describes the situation that classical theory has some global symmetry $G$ but it becomes anomalous in quantum theory by a background gauge field about $G$. This anomaly is RG invariant. Thus it is used to check a consistency of the theory. (See Anonaly matching)
There are other anomalies that should be separately mentioned, such as Witten anomaly or conformal anomaly(trace anomaly), but broadly speaking, these three anomalies are the ones you should know at least to understand modern field theories. I guess your text basically only refer to the first two types of anomaly.
We here note that we can consider the ‘t Hooft anomaly not only for continuous symmetry but discrete symmetry. (e.g. this article)
In this context, mixed ‘t Hooft anomaly about C, P and T symmetry is discussed. (e.g. this article) It is a little bit different context from your original text, but we should know about this type of anomaly so I mentioned.
About Poincaré symmetry, this forum already has one post for it, so please look that post.
Anyway, my main point is that if we take anomaly in a broad sense, discrete symmetry can also have anomaly. Of course, CPT symmetry, etc., can also be anomalous in principle.