= Chiral phase of the round-sphere Dirac operator
{title2=$V=D^+(D^-D^+)^{-1/2}$}
For the oriented round unit two-sphere, positive and negative <spinor bundles> have degrees $-1,+1$. Its <Dirac operator> has $D^2=C+1/4$ on their homogeneous sections, where $C$ is the angular-momentum <Casimir operator>; the <eigenvalues> of $D$ are the nonzero integers. Therefore the chiral phase is a unitary between the two L2 chiral spaces, commuting with $SU(2)$. For a smooth function $f$, $[D,f]=c(df)$ is bounded. The sign-operator resolvent integral expresses its phase commutator as a norm-convergent integral of compact resolvent products bounded by a constant times $(1+t^2)^{-1}$. Thus it intertwines multiplication by every continuous function modulo compacts. Its full graded phase is self-adjoint; the chiral phase is the component relevant to nonzero compressed indices.
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