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Viable choices could have been the PE of an object on
a high shelf, the KE of a moving object, the electrostatic
energy of a capacitor, ... almost any form of energy.
Obviously you can raise the energy of the earth/moon
gravitational system by raising the moon in the earth's
gravitational potential, i.e. by doing work on it by pulling
it against the gravitational force.
It is traditional and convenient from a /laboratory/ point of
view to speak of the gravitational energy "of" an object when
it is subject to an applied gravitational field ... as if the
energy "belonged" to the object. For example, we speak of
the GPE "of" a book on a high shelf. However, from the point
of view of /universal/ gravitation, this is highly
problematic. For starters, equation [1] is symmetric w.r.t
the roles of (m) and (M), and attributing the energy to just
one of the objects would break this symmetry.
Local conservation demands that any decrease in energy in any
region must correspond with a simultaneous increase in energy
in some _adjacent_ region(s).
So, unless you want to overthrow the most fundamental
principles of physics, we have to assume that there is energy
flowing in the field in Region 2. (The energy must be in the
_field_, because there isn't anything else in Region 2.)