“…= e z ) (and its associated q-Gaussian [78]) has already emerged in a considerable amount of nonextensive and similar systems (see [6,38,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104] among others), as the appropriate generalization of the exponential one (and its associated Gaussian) (with regard to the nonlinear quantum equations introduced in [103], see also [105,106,107,108,109,110,111,112,113,114,115]). Therefore, it appears as rather natural to conjecture that, in some sense that remains to be precisely defined, the LDT expression e −r 1 N becomes generalized into something close to e −rqN q (q ∈ R), where the generalized rate function r q should be some generalized entropic quantity per particle.…”