Write , setting unused coefficients to zero. Split the Adler trace into its fixed leading part and variable parts:
Cyclicity from part (i) gives
Thus this Hamiltonian trace functional on monic differential operators has the required form
To make each coefficient explicit, expand by the Leibniz rule. A term with derivatives of contributes to the residue exactly when . Consequently,
These are smooth functions depending on , not on the variable coefficients of . In particular and . The coefficient must be included: it appears in the displayed sum even though the printed coefficient list starts at .
The monic operators form an affine space, not a vector space. Accordingly is affine in the coordinates , with constant , and its differential is linear in variations. Its variational derivatives are . It is the restriction of a linear trace pairing on the full operator space, which explains the terminology without discarding the constant term.

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