New representations of pi and Dirac delta using the nonextensive-statistical-mechanics q-exponential function

preprint2010arXivOpen access

Abstract

We present a generalization of the representation in plane waves of Dirac delta, δ(x)=(1/2π)∫−∞∞e−ikx dkδ(x)=(1/2π)\int_{-\infty}^\infty e^{-ikx}\,dk, namely δ(x)=(2−q)/(2π)∫−∞∞eq−ikx dkδ(x)=(2-q)/(2π)\int_{-\infty}^\infty e_q^{-ikx}\,dk, using the nonextensive-statistical-mechanics qq-exponential function, eqix≡[1+(1−q)ix]1/(1−q)e_q^{ix}\equiv[1+(1-q)ix]^{1/(1-q)} with e1ix≡eixe_1^{ix}\equiv e^{ix}, being xx any real number, for real values of qq within the interval [1,2[[1,2[. Concomitantly with the development of these new representations of Dirac delta, we also present two new families of representations of the transcendental number ππ. Incidentally, we remark that the qq-plane wave form which emerges, namely eqikxe_q^{ikx}, is normalizable for 1<q<31<q<3, in contrast with the standard one, eikxe^{ikx}, which is not.

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