The finite size scaling renormalisation group (FSSRG) was introduced i
n Europhysics Letters 20 (1992) 621. Based only on the finite size sca
ling hypothesis, with no further assumptions, it differs from other re
al space renormalisation groups (RSRGs) in the following essential poi
nt: one does not need to adopt any particular recipe exp(-H(S')/T = SI
GMA(s) P(S, S') exp[-H(S)/T] relating the spin states S of the origina
l system to the spin states S' of a renormalised system. The choice of
a particular weight function P(S, S'), e.g. the so called majority ru
le, is generally based on plausibility arguments, and involves uncontr
ollable approximations. In addition to being free from these drawbacks
, FSSRG shares with RSRG some good features as, for instance, the poss
ibility of extracting qualitative informations from multi-parameter RG
flow diagrams, including crossovers, universality classes, universali
ty breakings, multicriticalities, orders of transitions, etc. Other un
pleasant consequences of particular weight functions, as the so called
proliferation of parameters, are also absent in the FSSRG. Using it i
n three-dimensions, we were able to find a semi-unstable fixed point i
n the critical frontier concentration p versus exchange coupling J, ch
aracterizing a universality class crossover when one goes from pure to
diluted Ising ferromagnets. The specific heat exponents we have obtai
ned for the pure and diluted regimes are in agreement with the Harris
criterion.