  We propose a paradigm for realizing the SYK model within string theory. Using
the large $N$ matrix description of $c<1$ string theory, we show that the
effective theory on a large number $Q$ of FZZT D-branes in $(p,1)$ minimal
string theory takes the form of the disorder averaged SYK model with $J
\psi^{p}$ interaction. The SYK fermions represent open strings between the FZZT
branes and the ZZ branes that underly the matrix model. The continuum SYK
dynamics arises upon taking the large $Q$ limit. We observe several qualitative
and quantitative links between the SYK model and $(p,q)$ minimal string theory
and propose that the two describe different phases of a single system. We
comment on the dual string interpretation of double scaled SYK and on the
relevance of our results to the recent discussion of the role of ensemble
averaging in holography.
