By Lefschetz S.
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Extra info for [Article] On the Real Folds of Abelian Varieties
And = Q of canonical of canonical dimension 1 and of the Weyl spinor super"elds = " A@? @? A" dimension 3/2. 2i( ? ) @Q . 20) We then proceed in the order of increasing canonical dimension. At dimension 1/2, all the torsion coe$cients vanish whereas at dimension 1 the above-mentioned super"elds R, RR and G are ? GA , @A? A@ A@? R, ¹A "! ( )A GA . @ @ @? 2 A @ ? 22) Plrep=1020=EM=VVC P. Bine& truy et al. "0 . 23) A@ At dimension 3/2, the super-covariant Rarita}Schwinger (super)"eld strengths ¹ ?
I[a , a ])#e L ( ? L @ @? @ ? L K K L L K @ L ? 42) @ L ? ?
W P [K (T )I#K M ( M T )IM ] , ? 50) receives additional terms due to the Yang}Mills couplings. 35) are replaced by D D I"E + R D I! 51) ? + ? P P ? GH ? M M M M M M n D D? M I"E + R D? M I! DP M I#A P (D? M T )I#A D? M I# I n M D M D? 45). 32). 3. 5. 3. Superxeld actions and equations of motion Invariant actions in superspace supergravity are obtained upon integrating superspace densities over the commuting and anticommuting directions of superspace. Densities, in this case, are constructed with the help of E, the superdeterminant of E .
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