We study absorbing phase transitions in the one-dimensional branching annihilating random walk with long-range repulsion. The repulsion is implemented as hopping bias in such a way that a particle is more likely to hop away from its closest particle. The bias strength due to long-range interaction has the form εx −σ , where x is the distance from a particle to its closest particle, 0 ≤ σ ≤ 1, and the sign of ε determines whether the interaction is repulsive (positive ε) or attractive (negative ε). A state without particles is the absorbing state. We find a threshold εs such that the absorbing state is dynamically stable for small branching rate q if ε < εs. The threshold differs significantly, depending on parity of the number ℓ of offspring. When ε > εs, the system with odd ℓ can exhibit reentrant phase transitions from the active phase with nonzero steady-state density to the absorbing phase, and back to the active phase. On the other hand, the system with even ℓ is in the active phase for nonzero q if ε > εs. Still, there are reentrant phase transitions for ℓ = 2. Unlike the case of odd ℓ, however, the reentrant phase transitions can occur only for σ = 1 and 0 < ε < εs. We also study the crossover behavior for ℓ = 2 when the interaction is attractive (negative ε), to find the crossover exponent φ = 1.123(13) for σ = 0.