For any observable , the Markov jump-process generator identity gives
Set and . With , reaction 2 changes by and reaction 3 changes it by . Therefore
and, using and ,
The equation for the second moment contains the third, whose equation contains the fourth, and so on. This is an infinite moment hierarchy.
Reaction 1 eventually leaves the odd initial copy number at . Put
The stationary first-moment equation gives
The stationary second-moment equation then gives
Under the prescribed central-moment closure,
Substitution yields the requested polynomial equation
This cubic comes from the closure approximation; it is not an exact equation for the stationary mean.
Reaction 4 creates , reaction 5 removes one and one , and reaction 6 creates ; reaction 7 leaves unchanged. The exact first-moment equations are therefore
At the assumed unique stationary distribution, both left-hand sides vanish. Eliminating the common mixed moment gives
No moment closure or independence assumption is involved.

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