In the first part of this paper we revisited the ghost-free four-derivative sector for chiral superfields in N=1 global supersymmetry as well as supergravity in superspace. This sector is captured by the operator in eq. (2.1). This term does not lea…
The contributions proportional to T2FCF,A for the gluonic massive operator matrix element at 3-loop order were calculated. These are the diagrams with two massive lines of equal mass.
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