I'll try to give an answer, because I was thinking about this myself.
The answer lies in Riemannian geometry, but the question is, what is it trying to tell us? I'll talk about curved space (Riemannian geometry), and then curved spacetime (pseudo-Riemannian geometry).
I define space to be the set of locations (mathematically, all locations are conceptualized as points). Now the thing is, I have to specify relationships between these locations.
For example, some locations are closer to each other than others, the set of locations is $3$-dimensional, etc. These are all real properties of the set.
This entire process of mathematically characterizing all the properties of what we know of as space comes in "three layers."
- The first is the topological: for each location, this specifies a set of locations that are "near" the original location. This is basically the "closeness" relations between points. Actually, a more accurate word summarizing this layer is probably "continuity."
- The second is differential: we need a way to discriminate between zig-zag lines and smooth curves (because we know objects in outer-space take smooth trajectories). This is the layer that makes it possible to do calculus (which physics is based on).
- The third is Riemannian: even though we specified continuity and smoothness in the above layers, there is still something missing. We need to specify length scales and perpendicularity. Essentially, we need to define relationships between different directions at a point (which two directions are perpendicular, etc.). All of the relevant info is summarized in the metric tensor $g_{\mu\nu}$.
Now a change in the metric means a change in the relationships between points and directions.
For example, beginning with Bernhard Riemann in the mid-19th century, mathematicians realized that we can modify the Pythagorean theorem in certain ways and still get self-consistent mathematics (for example, if $dx$ and $dy$ are the legs of a right triangle and $ds$ is the hypotenuse, then instead of writing $dx^{2} + dy^{2} = ds^{2}$ maybe we can write $2dx^{2} + dx\,dy + 3dy^{2} = ds^{2}$), but this is because all they're doing is changing the metric tensor on a manifold.
So, in short, the idea of intrinsic curvature of space is just the idea that relationships between locations and directions are changed in some non-standard way.
Of course, the question is about spacetime. I define spacetime to be the set of events, and I define an event to be a location with a specified time.
We go through the same process of defining relationships between different events, except the third layer is pseudo-Riemannian geometry (this is done to account for time).
Einstein's proposal was that gravity is the result of changes in relationships between events and directions.
Why these changes happen or how they happen is a question that is currently unanswered, and it is thought that quantum gravity might provide an answer.
What I want to emphasize is that at no point was space or spacetime conceptualized as a fabric or an aether. There is a lot of confusion regarding this point, and it is the reason why I was interested in this question in the first place.
Some people might think that if spacetime is not a fabric, then it is nothing. But that's not correct, because it is defined as the set of events, and we can identify real properties about this set. It is a concept, and concepts are neither material things nor are they nothing.
Spacetime is just an abstract set of events with relationships between these events, and curvature refers to how these relationships are altered.