First of all, “closed” and “infinite” are not synonymous in cosmology. A closed universe is one with a positive curvature, and is guaranteed to be finite. But you can also have a flat or open (negatively curved) universe which, due to various topological identifications, still wraps around.
If I remember correctly, there are 19 different flat 3-dimensional topologies. The simplest, of course, is just R[sup]3[/sup], a space infinite in all dimensions. For any of the others, the simplest way to describe them is by defining the basis cell and which of the faces are identified.
The next possibility is an infinite but finite-thickness slab, with the opposite faces identified. The slab may be rotated by an arbitrary angle on iteration, but we would not expect this in the actual Universe, since such a space would have a well-defined center. Each iteration might also be inverted, but we also wouldn’t expect this, since that would make the space non-orientable (like a Moebius strip), and certain properties of the weak nuclear force seem to imply that our Universe is orientable.
The next step after that is a “chimney”, which is infinite in one direction, but has a finite parallelogram cross section in the other two directions, and opposite faces identified with each other. Again, you could mathematically have an inversion in the identification, but it’s probably unphysical. You can also have a “chimney” shape which is hexagonal in cross section, rather than quadrilateral.
Of course, once you have those chimney spaces, you can chop up the infinite dimension, too, leaving your unit cells as prisms of the cross section shape (so a parallelopiped, or a hexagonal prism). And again, you can have rotations in your identifications, so long as the shapes match up. In the simplest case, here, your unit cell is a right rectangular prism (a box), with the opposite faces directly identified, in which case it’s referred to as the three-torus (since it’s analogous to the two-torus, topologically the surface of donut).
Finally, what I consider to be the most elegant one, your basis cell can be a rhombic dodecahedron, with opposite faces directly identified (no rotations are possible, on this one).
There are also a number of possible topologies for curved spaces, but I’m not too familiar with those. The only specific examples I know of are in a positively-curved space: You can have a basis cell shaped like a regular dodecahedron, with opposite faces identified with rotations of various angles.