The E = 0 octet of bilayer graphene in the filling factor range of -4 < < 4 is a fertile playground for many-body phenomena, yet a Landau level diagram is missing due to strong interactions and competing quantum degrees of freedom. We combine measurements and modeling to construct an empirical and quantitative spectrum. The single-particlelike diagram incorporates interaction effects effectively and provides a unified framework to understand the occupation sequence, gap energies and phase transitions observed in the octet. It serves as a new starting point for more sophisticated calculations and experiments.2 Bilayer graphene provides a fascinating platform to explore potentially new phenomena in the quantum Hall regime of a two-dimensional electron gas (2DEG). The existence of two spins, two valley indices K and Kʹ, and two isospins corresponding to the n = 0 and 1 orbital wave functions results in an eight-fold degeneracy of the singleparticle E = 0 Landau level (LL) in a perpendicular magnetic field B [1,2]. This SU (8) phase space provides ample opportunities for the emergence of broken-symmetry manybody ground states [3][4][5][6][7][8][9][10][11][12][13][14][15]. The application of a transverse electric field E drives valley polarization through their respective occupancy of the two constituent layers [1,2]. Coulomb exchange interactions, on the other hand, enhance spin ordering and promote isospin doublets [11,15,16]. As a result of these intricate competitions, the E = 0 octet of bilayer graphene (integer filling factor range -4 < < 4) exhibits a far richer phase diagram than their semiconductor counterparts. Experiments have uncovered 4, 3, 2, 1 coincidence points for filing factors = 0, ±1, ±2 and ±3 respectively, where the crossing of two LLs leads to the closing of the gap and signals the phase transition of the ground state from one order to another [13,[15][16][17][18]. Their appearance provides key information to the energetics of the LLs and the nature of the ground states involved. Indeed, coincidence studies on semiconducting 2DEGs are used to probe the magnetization of quantum Hall states [19] and measure the many-body enhanced spin susceptibility [20]. In bilayer graphene, the valley and isospin degrees of freedom increase the number of potential many-body coherent ground states. Furthermore, the impact of actively controlling these degrees of freedom became evident in the recent observations of fractional and even-denominator fractional quantum Hall effects [17,[21][22][23][24][25].A good starting point of exploring this rich landscape would be a single-particle, or single-particlelike LL diagram, upon which interaction effects can be elucidated perturbatively. Indeed, even in the inherently strongly interacting fractional quantum Hall effect, effective single-particle models, e.g. the composite fermion model [26], can capture the bulk of the interaction effects and provide conceptually simple and elegant ways to understand complex many-body phenomena. In bilayer graphene, a LL ...