Physica 104A (1980) 115-125 © North-Holland Publishing Co.
REAL SPACE RENORMALIZATION GROUP STUDY
OF THE RANDOM BOND ISING MODEL
Moshe SCHWARTZ
Department of Physics and Astronomy, TeI-Aviv University, Ramat-Aviv, Israel
and
Shmuel FISHMAN
Baker Laboratory, Cornell University, Ithaca, New York 14853, USA
Received II June 1980
The effects of configurational, quenched, bond randomness on the critical properties of the
nearest-neighbour Ising model are studied in two and three dimensions by a real space renor-
realization group method. Correlations between the random bonds generated by the renor-
malization group transformation are taken into account approximately. This proves necessary in
order to obtain correct scaling behaviour, i.e., crossover exponent A = a/v. The transition
temperature is calculated approximately as a function of the bond variance.
I. Introduction
The effect of quenched randomness on continuous phase transitions has
been studied extensively recently~). In the present work, we restrict ourselves
to weak, uncorrelated, quenched bond randomness. For such randomness, it
has been shown 2) that, if the specific heat exponent ot of the pure system is
negative, the critical behaviour should not be altered by the randomness. On
the other hand, if a is positive, randomness is expected to lead to new critical
behaviour. Moreover, from scaling3) and momentum space renormalization
group (RG)4) analysis, the stability exponent of the pure system fixed point is
A = a/v (where v is the correlation length exponent). Specifically, for the Ising
model in three dimensions, a >0 for the pure system, and one expects
different critical behaviour in the presence of randomness. In d =4-E
dimensions it was shown 5) that the Ising model critical behaviour is described
by a fixed point of order E~/2. According I0 experience with the E-expansion,
one is inclined to believe that this fixed point will also describe the critical
behaviour of the random Ising model in three dimensions. For the Ising
model, high temperature series expansions6) and real space RG calculations
have not been successful so far in revealing crossover to this new critical
behaviour, although distinct random critical behaviour has been obtained for a
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