The term moment of X implies that X happens at a distance as you mentioned. Additionally, there is a commonality in how they are calculated which involves the cross product of position and X. The cross product is used to extract the moment arm distance to that X.
- Moment of rotation (aka velocity) => $\boldsymbol{v} = \boldsymbol{r} \times \boldsymbol{\omega}$
- Moment of momentum (aka angular momentum) => $\boldsymbol{L} = \boldsymbol{r} \times \boldsymbol{p}$
- Moment of force (aka just moment) => $\boldsymbol{M} = \boldsymbol{r} \times \boldsymbol{F}$
So if you want to be technically correct, use the moment of X terms, and not the colloquial ones such as velocity, angular momentum and moment. I know crazy!
But you cannot do that, because you can have velocity without rotation, or moment without a force. The velocity of a purely translating rigid body is not generated from rotation, but it is the same for all parts of the body. It is a free vector because it is not associated with particular location, like the moment of rotation.
Similarly, a pure torque is not generated from a force at a distance (and hence the term moment is avoided) but something felt equally by all parts of the body. It is also a free vector because it is not associated with a particular location, like the moment of force.
A common way to generate a pure torque is by a force couple (aka just couple) which means two equal and opposite forces offset from each other arranged in such a way to generate the specific torque vector needed. This is mostly a result of the fact the mechanics primarily deals with contacts between bodies which only forces at the contact points, and there is no good way to apply a pure torque to a body without applied some kind of force combination also.
In practice, torque is meant to be used when the result is known (a moment along a specified axis) but the means of generating this torque aren't important. But a moment is used when the details of how it is generated are important.
Consider the following example
A rotating shaft with an asymmetric mass attached to it is cantilevered off one end of the shaft with a bearing, and a torque is applied on the shaft. Find the reaction forces and moments on the bearing.
Here there is a distinction between the shaft torque whose details are unimportant to the problem other than the moment is along the shaft axis and the reaction moments of the bearing whose details are important and act along an unknown arbitrary direction.