Mittag-Leffler analysis is an infinite dimensional analysis with respect to non-Gaussian measures of Mittag-Leffler type which generalizes the powerful theory of Gaussian analysis and in particular white noise analysis. In this paper we further develop the Mittag-Leffler analysis by characterizing the convergent sequences in the distribution space. Moreover we provide an approximation of Donsker's delta by square integrable functions. Then we apply the structures and techniques from Mittag-Leffler analysis in order to show that a Green's function to the time-fractional heat equation can be constructed using generalized grey Brownian motion (ggBm) by extending the fractional Feynman-Kac formula [Sch92]. Moreover we analyse ggBm, show its differentiability in a distributional sense and the existence of corresponding local times. (2010): Primary: 46F25, 60G22. Secondary: 26A33, 33E12.
Mathematics Subject ClassificationRemark 2.1. N is a perfect space, i.e. every bounded and closed set in N is compact. As a consequence strong and weak convergence coincide in both N and N ′ , see page 73 in [GV64] and Section I.6.3 and I.6.4 in [GS68].Example 2.2. Consider the white noise setting, where N = S(R) is the space of Schwartz test functions, H = L 2 (R, dx) and N ′ = S ′ (R) are the tempered distributions. S(R) is dense in L 2 (R, dx) and can be represented as the projective limit of certain Hilbert spaces H p , p > 0, with norms denoted by |·| p , see e.g. [Kuo96]. Thus the white noise setting is an example for the nuclear triple described above.
The Mittag-Leffler measureAs Mittag-Leffler measures µ β , 0 < β < 1, we denote the probability measures on N ′ whose characteristic functions are given via Mittag-Leffler functions. The Mittag-Leffler function was introduced by Gösta Mittag-Leffler in [ML05] and we also consider a generalization first appeared in [Wim05]. Definition 2.3. For 0 < β < ∞ the Mittag-Leffler function is an entire function defined by its power series E β (z) := ∞ n=0 z n Γ(βn + 1), z ∈ C.