We introduce a new nonextensive entropic measure S-chi that grows like N-ch
i, where N is the size of the system under consideration. This kind of none
xtensivity arises in a natural way in some N-body systems endowed with long
-range interactions described by r(-alpha) interparticle potentials. The po
wer law (weakly nonextensive) behavior exhibited by S-chi is intermediate b
etween (1) the linear (extensive) regime characterizing the standard Boltzm
ann-Gibbs entropy and (2) the exponential law (strongly nonextensive) behav
ior associated with the Tsallis generalized q-entropies. The functional S-c
hi is parametrized by the real number chi epsilon [1,2] in such a way that
the standard logarithmic entropy is recovered when chi = 1. We study the ma
thematical properties of the new entropy, showing that the basic requiremen
ts for a well behaved entropy functional are verified, i.e., S-chi possesse
s the usual properties of positivity, equiprobability, concavity and irreve
rsibility and verifies Khinchin axioms except the one related to additivity
since S-chi is nonextensive. For 1 < <chi> < 2, the entropy S-<chi> become
s superadditive in the thermodynamic limit. The present formalism is illust
rated by a numerical study of the thermodynamic scaling laws of a ferromagn
etic Ising model with long-range interactions.