Abstract: We study the decay Bˉ<sup>0→Λc<sup>+pˉπ<sup>+π<sup>−, reconstructing the \Lambda_{c}{+} baryon in the pK<sup>−π<sup>+ mode, using a data sample of 467×10<sup>6 BBˉ pairs collected with the BaBar detector at the PEP-2 storage rings at SLAC. We measure branching fractions for decays with intermediate Σc baryons to be B[Bˉ<sup>0→Σc(2455)<sup>++pˉπ<sup>−]=(21.3</sup></sup></sup>±1.0±1.0±5.5)×10<sup>−5, B[Bˉ<sup>0→Σc(2520)<sup>++pˉπ<sup>−]=(11.5±</sup></sup></sup>1.0±0.5±3.0)×10<sup>−5, B[Bˉ<sup>0→Σc(2455)<sup>0pˉπ<sup>+]=(9.1</sup></sup></sup>±0.7±0.4±2.4)×10<sup>−5, and B[Bˉ<sup>0→Σc(2520)<sup>0pˉπ<sup>+]=</sup></sup></sup>(2.2±0.7±0.1±0.6)×10<sup>−5, where the uncertainties are statistical, systematic, and due to the uncertainty on the $\Lambda_{c}<sup>{+}\rightarrow\proton\Km\pi<sup>{+}$ branching fraction, respectively. For decays without Σc(2455) or Σc(2520) resonances, we measure B[Bˉ<sup>0→Λc<sup>+pˉπ<sup>+π<sup>−]<em>non−Σ</em>c=(79</sup></sup></sup></sup>±4±4±20)×10<sup>−5. The total branching fraction is determined to be B[Bˉ<sup>0→Λc<sup>+pˉπ<sup>+π<sup>−]total=(123</sup></sup></sup></sup>±5±7±32)×10<sup>−5. We examine multibody mass combinations in the resonant three-particle Σcpˉπ final states and in the four-particle Λc<sup>+pˉπ<sup>+π<sup>− final state, and observe different characteristics for the pˉπ combination in neutral versus doubly-charged Σc decays.