A recently proposed theory for diffusion-limited aggregation (DLA), wh
ich models this system as a random branched growth process, is reviewe
d. Like DLA, this process is stochastic, and ensemble averaging is nee
ded in order to define multifractal dimensions. In an earlier work by
Halsey and Leibig, annealed average dimensions were computed for this
model. In this paper, we compute the quenched average dimensions, whic
h are expected to apply to typical members of the ensemble. We develop
a perturbative expansion for the average of the logarithm of the mult
ifractal partition function; the leading and subleading divergent term
s in this expansion are then resummed to all orders. The result is tha
t in the limit where the number of particles n --> infinity, the quenc
hed and annealed dimensions are identical; however, the attainment of
this limit requires enormous values of n. At smaller, more realistic v
alues of n, the apparent quenched dimensions differ from the annealed
dimensions. We interpret these results to mean that while multifractal
ity as an ensemble property of random branched growth (and hence of DL
A) is quite robust, it subtly fails for typical members of the ensembl
e.