DESY 97-254 ANL-HEP-PR-97-99 MZ-TH/97-38 A Closed Formula for the Riemann Normal Coordinate Expansion Uwe M¨uller Institut f¨ur Physik, Johannes-Gutenberg-Universit¨at Mainz, Staudingerweg 7, D-55099 Mainz, Germany e-mail:
[email protected] Christian Schubert High Energy Physics Division, Argonne National Laboratory, Argonne, IL 60439-4815, USA and Institut f¨ur Physik, Humboldt Universit¨at zu Berlin, Invalidenstr. 110, D-10115 Berlin, Germany e-mail:
[email protected] Anton E. M. van de Ven II Institut f¨ur Theoretische Physik, Universit¨at Hamburg, Luruper Chaussee 149, D-22761 Hamburg, Germany e-mail:
[email protected] arXiv:gr-qc/9712092v2 20 Dec 1999 Abstract We derive an integral representation which encodes all coeffi- cients of the Riemann normal coordinate expansion and also a closed formula for those coefficients. In gauge theory, one often uses Fock-Schwinger gauge [1, 2] to achieve manifest covari- ance in the calculation of effective actions, anomaly densities, or other quantities. Fock- Schwinger gauge “centered at 0” can be defined by the condition µ y Aµ(y) = 0. (1) Locally in some neighbourhood of 0, this condition can be solved in terms of the following integral representation connecting the gauge potential and the field strength tensor [3, 4], 1 ρ Aµ(y)= y dvvFρµ(vy) (2) Z0 (see our eqs. (9-13)). More explicitly, in this gauge one can express the coefficients of the Taylor expansion of A at x = 0 in terms of the covariant derivatives of F , ∞ n ∞ n (y · ∂x) ρ (y · Dx) ρ Aµ(y)= y Fρµ(0) = y Fρµ(0).