Short answer: probably not. Nobody really knows. Does a ball accelerating down a hill gain energy? [yes, kinetic, no total.] But the 'total energy' of the universe lies outside conservation of energy rules and regulations.
For one thing dark energy constitutes almost 3/4 of the mass-energy in the universe and we know darn little about it. For example, I don't think there is a consensus about the relationship between dark energy, the cosmological constant, vacuum energy and scalar fields.
As the universe expands, it also 'cools'...otherwise we'd still be at the approximate 3,000 degres Kelvin that the cosmic microwave was emitted at about 13.7B years ago. [The CMBR is now a lot longer wavelength than it used to be and continues to get longer.] And the universe has expanded and acclerated a lot faster in the past than it is now. So it seems things are cooling, but of course that is only one component of 'total energy'.
Another 'clue' is that most scientists believe we'll end up in a cold dark empty universe many billions of years from now. But that will be a state of maximum entropy not necessarily a different total energy. A further clue is that none of the 'cosmological calculators' available online provide a way to calculate the 'total energy' of the universe. One more technical answer, indicating 'we do not have a good answer', comes from PeterDonis of these forums:
QUOTE]... energy "conservation" is more complicated:
* In a stationary spacetime (i.e., one with a time translation symmetry), one can define a conserved "total energy" using the time translation symmetry and Noether's theorem.
* In an asymptotically flat spacetime (i.e., one in which the metric approaches the Minkowski metric at large "distances" from some central region), one can define a conserved "total energy" by finding an effective 4-momentum vector for the system in the asymptotically flat metric. Since this basically amounts to finding an asymptotic time translation symmetry, it ends up being basically equivalent to the stationary case above.
* In a spacetime that is neither stationary nor asymptotically flat, such as in the FRW spacetimes used to describe our expanding universe, neither of the above applies, so there is no good way to define a conserved "total energy".[/QUOTE]
My notes don't indicate the source for this..maybe also Peter:
In *all* of the above cases, there are various ways to define "energy stored in the gravitational field", and with at least some of them, you can often come up with a "conservation law" that includes energy being "exchanged between matter and the gravitational field". However, none of these "conservation laws" are relativistically covariant; they all require picking a particular coordinate chart and treating it as "special" somehow. [This last sentence refers to the 'frame' of reference in post #2.]