I think the answer must be yes, in the standard, mainstream interpretation of general relativity, and its application to big bang cosmology. Just look at Einstein's equations. Despite all my efforts, I cannot make Greek letters, even following the
instructions given. So just pretend that the mn subscripts are Greek
mu &
nu and the L is an upper case
lambda. Or look at the
Wikipedia article, which looks OK to me.
R
mn - (1/2)Rg
mn + Lg
mn = 8(pi)T
mn
Written this way, everything on the left side of the equation is
spacetime, and everything on the right side of the equation is all of the matter & energy. So to create a toy universe with nothing in it, just set the right side to zero. But the left side, spacetime, is still there. So if there are any dynamic properties on the left side, then space expands (which is in fact the case for mainstream big bang cosmology, where the expansion is expressed as a change in the scalar curvature
R).
Note that the cosmological constant is on the left side, since it is proportional to the metric tensor. This means that if
dark energy, driving the accelerated expansion of the universe, is interpreted as a cosmological constant, then it is not actually "energy" at all, and "dark energy" becomes a poor choice of words to describe it. On the other hand,
quintessence,
quartessence,
Cardassian Expansion,
Phantom cosmology, and who knows what else, are all examples of expansion driven by fields found in the stress-energy tensor (
Tmn). In those cases we can identify expansion with something identifiable as energy.