  When layers of graphene are rotationally misaligned by the magic angle, the
moir\'e superlattice features extremely flat bands. Due to the enhanced density
of states, the Coulomb interaction induces a variety of instabilities. The most
prominent occur at integer filling and are therefore commonly attributed to
spontaneous polarization of the moir\'e unit cell's `flavor' degrees of freedom
-- spin, valley, and the flat-band degeneracy. As the dominant member of the
hierarchy, these correlated states are thought to crucially determine further
instabilities at lower energy scales, such as superconductivity and weaker
incompressible states at fractional filling. In this work, we examine the
behavior of twisted trilayer graphene in a window of twist angle around
$1.3^{\circ}$, well below the expected magic angle of $1.55^{\circ}$. In this
small twist angle regime, we find surprisingly narrow bands, which are
populated with both an abundance of correlation-driven states at fractional
filling as well as robust superconductivity. The absence of linear-in-$T$
resistivity without significant reduction of the superconducting transition
temperature, provides insights into the origin of both phenomena. Most
remarkably, the hierarchy between integer and fractional filling is absent,
indicating that flavor polarization does not play a governing role. The
prominence of fractional filling in the small twist angle regime also points
towards a longer-range effective Coulomb interaction. Combined, our results
shed new light on outstanding questions in the field, while establishing the
small twist angle regime as a new paradigm for exploring novel flavors of
moir\'e physics.
