We study the ground-state properties of a spin-1 Heisenberg model on the square lattice with the first and second nearest-neighbor antiferromagnetic couplings J1, J2 and a three-spin scalar chirality term Jχ. Using the density matrix renormalization group calculation, we map out a global phase diagram including various magnetic order phases and an emergent quantum spin liquid phase. The nature of the spin liquid is identified as a bosonic non-Abelian Moore-Read state by the fingerprint of the entanglement spectra and identification of a full set of topological sectors. We further unveil a stripe magnetic order coexisting with this spin liquid. Our results not only establish a rare example of non-Abelian spin liquids in simple spin systems, but also demonstrate the coexistence of fractionalized excitations and magnetic order beyond mean-field descriptions.Introduction.-Quantum spin liquids (QSLs) are novel quantum states with long-range entanglement and emergent fractionalized excitations, which can escape from forming conventional magnetic order due to geometric frustration and quantum fluctuation [1-5]. The prominent realizations of QSLs are the chiral spin liquids (CSLs) [6], which break time-reversal symmetry (TRS) and have been established in some spin-1/2 systems [7][8][9][10][11][12][13][14][15][16][17][18]. These CSLs have fractional excitations following the Abelian anyon statistics, which are spin-analogues of the Laughlin state and bridge QSLs and fractional quantum Hall effect [19][20][21]. More interestingly, the exactly soluble models host a new class of CSLs with non-Abelian quasiparticles [22,23] that have the potential of performing topological quantum computation [24] and have stimulated extensive search of CSLs in the Kitaev materials with strong spin-orbit couplings [25]. Another natural system to search for non-Abelian CSLs is the frustrated spin-1 model [26][27][28], which could be realized in both magnetic compounds [29,30] and cold atom systems [31]. However, the identified non-Abelian CSLs in frustrated spin-1 systems are very rare so far [32].