Computer simulations were carried out for self-avoiding walk conformat
ions of randomly branched polymers on a simple cubic lattice. The numb
er of segments (N) and branching points (rn) are set constant. The max
imum N and m examined are 500 and 5, respectively. No attractive energ
y among the segments is considered. The standard success-walk number i
s 100000 for every condition. A critical exponent (upsilon) on N for t
he root of the mean square radius of gyration ([s(2)](1/2)) is found t
o be 0.598. This upsilon is the same value as those of both linear and
star-branched polymers reported in other papers. The g-values (=[s(2)
](branch)/[s(2)](linear)) Obtained are nearly equal to those of the ra
ndom walk in the rn-range of this work. Generalization of the conclusi
on is speculated. upsilon of the case where m distributes statisticall
y is estimated to be 0.35 which is smaller by about 0.1 than that of o
ther randomly-branched polymers. The difference, 0.1, might be attribu
ted to that of the distribution of branching points. The above descrip
tion assumes the polymers long and flexible.