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We study random lattice networks consisting of resistor like and diode like bonds. For investigating the transport properties of these random resistor diode networks we introduce a field theoretic Hamiltonian amenable to renormalization group analysis. We focus on the average two-port resistance at the transition from the nonpercolating to the directed percolating phase and calculate the corresponding resistance exponent to two-loop order. Moreover, we determine the backbone dimension of directed percolation clusters to two-loop order. We obtain a scaling relation for that is in agreement with well known scaling arguments.

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