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4th Workshop on Fractional Calculus, Probability and Non-Local Operators: Applications and Recent Developments November, Wednesday 23rd - Friday 25th, 2016 Wednesday 23rd and Thursday 24th, 9:30-13:00 / 15:00-18:00 and Friday 25th, 9:30-15:00 BCAM-Basque Center for Applied Mathematics Mazzarredo 14, Bilbao, Basque Country, Spain www.bcamath.org

Book of Abstracts

List of participants Adrian Baule Queen Mary University of London, UK email: a.baule@qmul.ac.uk Nicole Cusimano, Bilbao, Spain email: ncusimano@bcamath.org José Luís da Silva University of Madeira, Funchal, Portugal email: luis@uma.pt Félix del Teso, Bilbao, Spain email: fdelteso@bcamath.org Nicos Georgiou University of Sussex, Brighton, UK email: n.georgiou@sussex.ac.uk Martin Grothaus University of Kaiserslautern, Germany email: grothaus@mathematik.uni-kl.de Rainer Klages Queen Mary University of London, UK email: r.klages@qmul.ac.uk József Lőrinczi Loughborough University, UK email: J.Lorinczi@lboro.ac.uk Eulalia Nualart Universitat Pompeu Fabra, Barcelona, Spain email: eulalia@nualart.es Gianni Pagnini, Bilbao, Spain email: gpagnini@bcamath.org Lukasz P lociniczak Wroc law University of Science and Technology, Poland email: lukasz.plociniczak@pwr.edu.pl Nikola Sandrić University of Zagreb, Croatia email: nsandric@grad.hr Mladen Savov Institute of Mathematics and Informatics, Bulgarian Academy of Sciences, Sofia, Bulgaria email: mladensavov@math.bas.bg Enrico Scalas University of Sussex, Brighton, UK email: e.scalas@sussex.ac.uk Stjepan Šebek University of Zagreb, Croatia email: stjepan.sebek@gmail.com Renato Spigler Roma Tre University, Italy email: spigler@mat.uniroma3.it Diana Stan, Bilbao, Spain email: dstan@bcamath.org Bruno Toaldo University of Rome La Sapienza, Italy email: bruno.toaldo@uniroma1.it Mailan Trinh University of Sussex, Brighton, UK email: M.Trinh@sussex.ac.uk Silvia Vitali University of Bologna, Italy email: silvia.vitali4@unibo.it

4 th FCPNLO - Fractional Calculus, Probability and Non-Local Operators 23-25 November 2016 BCAM Basque Center for Applied Mathematics, Bilbao, Spain Time 23 November 24 November 25 November 9:30-10:30 M. Grothaus R. Klages R. Spigler (9:30-10:15) 10:30 11:00 M. Trinh S. Vitali N. Cusimano (10:15-11:00) 11:00 11:30 Coffee Break Coffee Break Coffee Break 11:30 12:15 N. Sandrić Ł. Płociniczak E. Nualart 11:30-12:30 (closing talk) 12:15 13:00 M. Savov D. Stan 13:00 15:00 Lunch Lunch 15:00 16:00 B. Toaldo A. Baule 16:00 16:30 Coffee Break Coffee Break 16:30 17:15 J.L. da Silva N. Georgiou 17:15 18:00 F. del Teso J. Lörinczi 20:30 Social Dinner

Weakly Galilean invariant fractional di usion operators Andrea Cairoli, Rainer Klages, and Adrian Baule School of Mathematical Sciences, Queen Mary University of London, London E1 4NS a.baule@qmul.ac.uk Di usion of a tracer in a heat bath originates from its complex interaction with the thermal environment. When modelling such fluctuating dynamics on a microscopic level, Galilean invariance of the equations of motion holds, which describes the invariance with respect to a coordinate transformation to a reference frame that moves with a constant velocity. However, when modelling di usion on a mesoscopic level, such as with a Langevin equation, Galilean invariance breaks down. Here, we show that Galilean invariance in the context of stochastic systems has to be replaced by a so-called weak Galilean invariance of the probability density function (PDF) with respect to coordinate transformations. For anomalous di usive systems, imposing a weakly Galilean invariant PDF requires the use of a fractional substantial derivative [1, 2] already on the level of overdamped dynamics due to the spatiotemporal coupling. Moreover, we show that a weakly Galilean invariant Langevin equation for anomalous di usive systems relies on a noise term that can be expressed in terms of the subordination of a Gaussian white noise with an inverse Lévy-stable subordinator [3]. References [1] R. Friedrich, F. Jenko, A. Baule, and S. Eule, Physical Review Letters 96, 230601 (2006) [2] A. Cairoli and A. Baule, Physical Review Letters 115, 110601 (2015) [3] A. Cairoli and A. Baule, Physical Review E 92, 012102 (2015)

Numerical implementation of fractional powers of the Laplacian operator on bounded domains Nicole Cusimano BCAM Alameda de Mazarredo 14, 48009 Bilbao - Spain ncusimano@bcamath.org Félix del Teso BCAM Alameda de Mazarredo 14, 48009 Bilbao - Spain fdelteso@bcamath.org Luca Gerardo-Giorda BCAM Alameda de Mazarredo 14, 48009 Bilbao - Spain lgerardo@bcamath.org The fractional Laplacian is a di erential operator of non-integer order that has been extensively studied in the last few decades and is naturally defined on the whole R n, n 1. As many other fractional order derivatives and integrals, this operator has been often used to model transport processes which generalise classical Brownian motion. However, many physical problems of interest are defined in bounded domains and the use of the fractional Laplacian as modelling tool in this context poses the challenge of providing a meaningful interpretation of the operator in these settings. Following the heat semi-group formalism, we introduce a family of operators which are boundary conditions dependent and discuss a suitable approach for their numerical discretisation by combining a quadrature rule of integration with the finite element method. This approach will not only allow for a meaningful interpretation of fractional powers of an operator in bounded settings but will also provide a flexible strategy for the computation of their value on multi-dimensional (possibly irregular) domains, and a convenient framework for the solution of the fractional Poisson equation and the corresponding parabolic problem.

The Stein characterization of Wright-type distributions Mohamed Erraoui Université Cadi Ayyad, Faculté des Sciences Semlalia, Département de Mathématiques, BP 2390, Marrakech, Maroc erraoui@uca.ma José Luís da Silva University of Madeira Campus da Penteada, 9020-205, Funchal, Portugal luis@uma.pt The M-Wright function M,0< < 1, was introduced by F. Mainardi in order to study time-fractional di usion-wave equation, see [2]. The class of random variables X with M- Wright density M is denoted by MW( ) and we say that X has M-Wright distribution. In this talk we extend the Stein method to the class MW( ), i.e., find a proper characterizing equation for the distribution and the corresponding Stein equation. So far, we succeeded to distribution from MW 1 3 [1]. References [1] M. Erraoui and J. L. da Silva. The Stein characterization of Wright-type distributions, in preparation, 2016. [2] F. Mainardi. On the initial value problem for the fractional di usion-wave equation. In S. Rionero and T. Ruggeri, editors, Waves and Stability in Continuous Media (Bologna, 1993), volume 23 of Advances in Mathematics for Applied Sciences, pages 246 251, River Edge, NJ, USA, 1994. World Scientific.

Numerical methods for distributional solutions of nonlocal equations of porous medium type Félix del Teso fdelteso@bcamath.org Jørgen Endal NTNU - Norwegian University of Science and Technology Trondheim Norway jorgen.endal@math.ntnu.no Espen R. Jakobsen NTNU - Norwegian University of Science and Technology Trondheim Norway espen.jakobsen@math.ntnu.no Recently, the group of J. L. Vázquez and some other have obtained many results concerning weak (energy) solutions for the so-called Fractional Porous Medium Equation: @ t u +( ) 2 '(u) =0, (FPME) where ( ) 2 denotes the fractional Laplacian for 2 (0, 2) and ' : R! R is a nonlinearity of power type. However, there not seem to be many works on numerics for (FPME) (no results at all in the fast di usion case: '(u) =u m with m<1). We present two set of results in this talk: 1. Very general well-posedness results: We allow general nonlocal symmetric nonnegative di usion operators, any continuous nondecreasing nonlinearity, and distributional solutions (that do not have finite energy a priori [2]) 2. A wide class of numerical schemes which are monotone, stable, consistent and convergent for both local and nonlocal problems [1, 3]. The very general framework considered make the proofs become very involved, including a priori estimates, L 1 -contraction, comparison principles, compactness and regularity arguments, Stroock-Varopoulos inequalities and Liouville type results. References [1] F. del Teso, J. Endal, E. R. Jakobsen. Uniqueness and properties of distributional solutions of nonlocal equations of porous medium type. Adv. Math. 305 (2017), 78 143. [2] F. del Teso, J. Endal, E. R. Jakobsen. On the well-posedness of solutions with finite energy for nonlocal equations of porous medium type. arxiv:1610.02221. Submitted for publication (2016). [3] F. del Teso, J. Endal, E. R. Jakobsen. Numerical methods for distributional solutions of local and nonlocal equations of porous medium type. In preparation.

Mixing times and relaxation to equilibrium for fractional time-changed semi-markov processes Enrico Scalas University of Sussex Brighton, United Kingdom e.scalas@sussex.ac.uk Nicos Georgiou University of Sussex Brighton, United Kingdom n.georgiou@sussex.ac.uk Of interest in the theory of finite state Markov processes is the relaxation to equilibrium, particularly 1. the estimation of convergence rates to the invariant measure 2. the mixing time for the chain (usually associated with reversible chains) which estimates the necessary time so that the transition probabilities and the invariant measure are close in the total variation distance. The answer to these questions are also important when performing Monte Carlo simulations. We are concerned with the answers to these questions when we have time-changed, continuous time semi Markov process where the inter-event times are arbitrary positive random variables with a special focus (and sharper results) on heavy-tailed (e.g. Mittag-Le er) waiting times. Examples include semi-markov processes on a finite, countable and continuous compact state space.

Mittag Le er Analysis: Construction and Applications Florian Jahnert University of Kaiserslautern P.O. Box 3049, 67653 Kaiserslautern, Germany jahnert@mathematik.uni-kl.de José Luís da Silva Universidade da Madeira Edifício da Penteada, Caminho da Penteada, 9020-105, Funchal, Madeira, Portugal luis@uma.pt Martin Grothaus and Felix Riemann University of Kaiserslautern P.O. Box 3049, 67653 Kaiserslautern, Germany grothaus@mathematik.uni-kl.de, riemann@mathematik.uni-kl.de Motivated by the results of infinite dimensional Gaussian analysis and especially white noise analysis, we construct a Mittag Le er analysis. This is an infinite dimensional analysis with respect to non-gaussian measures of Mittag Le er type which we call Mittag-Le er measures. Our results indicate that the Wick ordered polynomials, which play a key role in Gaussian analysis, cannot be generalized to this non-gaussian case. We provide evidence that a system of biorthogonal polynomials, called generalized Appell system, is applicable to the Mittag Le er measures, instead of using Wick ordered polynomials. With the help of an Appell system, we introduce a test function and a distribution space. Furthermore we give characterizations of the distribution space and we characterize the weak integrable functions and the convergent sequences within the distribution space. We construct Donsker s delta in a non-gaussian setting as an application. In the second part, we develop a grey noise analysis. This is a special application of the Mittag Le er analysis. In this framework, we introduce generalized grey Brownian motion and prove di erentiability in a distributional sense and the existence of generalized grey Brownian motion local times. Grey noise analysis is then applied to the time-fractional heat equation and the time-fractional Schrödinger equation. We prove a generalization of the fractional Feynman Kac formula for distributional initial values. In this way, we find a Green s function for the time-fractional heat equation which coincides with the solutions given in the literature. The results presented in this talk are published in the references below. References [1] M. Grothaus; F. Jahnert; F. Riemann; J. L. da Silva. Mittag Le er analysis I: Construction and characterization. Journal of Functional Analysis. 268(7), 1876 1903, 2015. [2] M. Grothaus; F. Jahnert. Mittag Le er analysis II: Application to the fractional heat equation. Journal of Functional Analysis, 270(7), 2732 2768, 2016.

Statistical Physics and Anomalous Dynamics of Foraging Rainer Klages Queen Mary University of London, School of Mathematical Sciences Mile End Road, London E1 4NS, UK r.klages@qmul.ac.uk My talk will illustrate the application of fractional calculus and non-local operators to mathematically model the search for food by biological organisms, and problems by trying to do so. A question that attracted a lot of attention in the past two decades is whether biologically relevant search strategies can be identified by statistical data analysis and mathematical modeling [1]. A famous paradigm in this field is the Lévy Flight Hypothesis. It states that under certain mathematical conditions Lévy dynamics, which defines a key concept in the theory of anomalous stochastic processes, leads to an optimal search strategy for foraging organisms. This hypothesis is discussed very controversially in the current literature [2]. After introducing the stochastic processes of Lévy flights and Lévy walks I will review examples and counterexamples of experimental data and their analyses confirming and refuting the Lévy flight hypothesis. This debate motivated own work on deriving a fractional diffusion equation for an n- dimensional correlated Lévy walk [3], studying search reliability and search efficiency of combined Lévy-Brownian motion [4], and investigating stochastic first passage and first arrival problems [5]. References [1] see webpage by the Advanced Study Group corresponding to the title of this talk: www.mpipks-dresden.mpg.de/ asg 2015 [2] R.Klages, Search for food of birds, fish and insects, book chapter in: A.Bunde, J.Caro, J.Kaerger, G.Vogl (Eds.), Diffusive Spreading in Nature, Technology and Society. (Springer, Berlin, 2017). [3] J.P.Taylor-King, R.Klages, S.Fedotov, R.A.Van Gorder, Phys.Rev.E 94, 012104 (2016). [4] V.V.Palyulin, A.Chechkin, R.Klages, R.Metzler, J.Phys.A: Math.Theor. 49, 394002 (2016). [5] G.Blackburn, A.V.Chechkin, V.V.Palyulin, N.W.Watkins, R.Klages, tbp

Jump Processes in a Potential Landscape József Lőrinczi Department of Mathematical Sciences, Loughborough University Loughborough LE11 3TU, United Kingdom J.Lorinczi@lboro.ac.uk There is much activity recently in both pure and applied mathematics in an e ort to investigate random processes with jump discontinuities and related non-local operators. Such problems appear and rapidly multiply at the interface area of probability and functional analysis, and have a range of applications in scientific modelling. While many authors focus on Lévy processes securing stationary increments, there is interest in taking account also of the e ect of a non-uniform environment, in which paths are reinforced or penalised according to their position in space. In this talk I will survey some rigorous results on various aspects of jump processes which are assumed to have a stationary measure. References [1] Kaleta, K., Kwaśnicki, M. and Lőrinczi J. 2016 Contractivity and ground state domination properties for non-local Schrödinger operators. arxiv:1509.08319. [2] Kaleta, K. and Lőrinczi J. 2012 Fractional P ( ) 1 -processes and Gibbs measures. Stoch. Proc. Appl. 122, 3580 3617. [3] Kaleta, K. and Lőrinczi J. 2015 Pointwise estimates of the eigenfunctions and intrinsic ultracontractivity-type properties of Feynman Kac semigroups for a class of Lévy processes. Ann. Probab. 43, 1350 1398. [4] Kaleta, K. and Lőrinczi J. 2016 Fall-o of eigenfunctions of non-local Schrödinger operators with decaying potentials. Potential Anal., doi:10.1007/s11118-016-9597-3, pp. 1 42. [5] Kaleta, K. and Lőrinczi J. 2016 Typical long time behaviour of ground state transformed jump processes. Preprint. [6] Kaleta, K. and Lőrinczi J. 2016 Zero-energy bound state decay for fractional Schrödinger operators. Preprint. [7] Lőrinczi, J. and Ma lecki J. 2012 Spectral properties of the massless relativistic harmonic oscillator. J. Di. Equa. 253, 2846 2871. [8] Lőrinczi, J. and Sasaki I. 2016 Embedded eigenvalues and Neumann Wigner potentials for relativistic Schrödinger operators. arxiv:1605.00196.

Intermittency of some fractional stochastic heat equations Eulalia Nualart Universitat Pompeu Fabra Ramon Trias Fargas 25-27, 08005, Barcelona eulalia@nualart.es I will present an overview talk about recent results on moments, intermittency and chaotic behaviour of some fractional stochastic heat equation. I will also discuss some open problems. References [1] Foondun, M. and Khoshnevisan, D. 2009 Intermittence and nonlinear parabolic stochastic partial di erential equations, Electronic Journal of Probability 548 568, 14. [2] Foondun, M., Khoshnevisan, D. and Nualart, E. 2011 A local time correspondence for stochastic partial di erential equations, Transactions of the American Mathematical Society 363, 2481 2515. [3] Foondun, M. and Nualart, E. 2015 On the behaviour of stochastic heat equations on bounded domains, ALEA Lat. Am. J. Probab. Math. Stat. 12, 551-571. [4] Khoshnevisan, D. and Kim, K. 2015, Non-linear noise excitation and intermittency under high disorder, Proc. AMS, 143, 4073-4083. [5] Foondun, M., Liu, W. and Omaba, M. 2016, Moment bounds for a class of fractional stochastic heat equations, to appear in Annals of Probab.

Nonlinear subdi usion in porous media Lukasz P lociniczak Faculty of Pure and Applied Mathematics, Wroc law University of Science and Technology Wyb. Wyspiańskiego 27, 50-370 Wroc law, Poland lukasz.plociniczak@pwr.edu.pl We consider a nonlocal nonlinear partial di erential equation modelling moisture distribution (denoted by u = u(x, t)) with initial-boundary conditions @ t u =(D(u)u x ) x, x > 0, t>0, 0 < < 1, u(0,t)=1, u(x, 0) = 0, x > 0, t>0. Here, the operator @ t is the Riemann-Liouville fractional derivative taken with respect to the time t. Looking for a self-similar solution u(x, t) =U(xt /2 ) leads to an ordinary integro-di erential equation apple (1 ) D(U)U 0 0 = 1 (1 ) where we have defined the Erdélyi-Kober type operator F U( ) := Z 1 0 (1 s) U 2 d d F U, 0 < < 1, s 2 ds. We will present several results concerning existence, uniqueness, approximations and inverse problems associated with the above problem. Some of them can be found in our works [1, 2]. References [1] P lociniczak, L. 2014 Approximation of the Erdélyi-Kober fractional operator with application to the time-fractional porous medium equation. SIAM Journal of Applied Mathematics 74(4), 1219 1237. [2] P lociniczak, L. 2016 Di usivity identification in a nonlinear time-fractional di usion equation. Fractional Calculus and Applied Analysis 19(4), 883 866.

Stochastic stability of Lévy-type processes Nikola Sandrić University of Zagreb Trg maršala Tita 14, 10000 Zagreb, Croatia nsandric@grad.hr In this talk, we discuss transience, recurrence, weak and strong transience, and ergodicity of Feller processes associated with pseudo-di erential operators - the so-called Lévy-type processes. First, we present Chung-Fuchs type conditions for the transience and recurrence in terms of the symbol of the corresponding pseudo-di erential operator. Next, by using these conditions we discuss the transience and recurrence with respect to the dimension of the state space and Pruitt indices, and the transience and recurrence of Feller-Dynkin di usions and stable-like processes. In the one and two-dimensional cases, we analyze perturbations of these processes which do not a ect their transience and recurrence properties, and we present su cient conditions for their transience and recurrence in terms of the corresponding Lévy measure. At the end, we introduce the notion of weak and strong transience and discuss ergodicity of Lévy-type processes. References [1] Sandrić, N. 2013 Long-time behavior of stable-like processes, Stochastic Process. Appl. 123(4):1276-1300. [2] Sandrić, N. 2016 Long-time behavior for a class of Feller processes, Trans. Am. Math. Soc. 368(3):1871-1910. [3] Sandrić, N. 2016 On recurrence and transience of two-dimensional Lévy and Lévy-type processes, Stochastic Process. Appl. 126(2):414-438. [4] Sandrić, N. 2016 Ergodicity of Lévy-type processes, ESAIM-Prob. Stat. 20:154-177. [5] Sandrić, N. 2016 On transience of Lévy-type processes, Stochastics 88(7):1012-1040. [6] Schilling, R. L. and Wang, J. 2013 Some theorems on Feller processes: transience, local times and ultracontractivity, Trans. Am. Math. Soc. 365(6):3255-3286.

Bernstein-gamma functions and Exponential functionals of Lévy Processes Mladen Savov Institute of Mathematics and Informatics, Bulgarian Academy of Sciences ul. Akad. Georgi Bonchev, bl. 8, Sofia 1113, Bulgaria mladensavov@math.bas.bg In this talk we consider a recurrent equation of the type f(z + 1) = ( z) f(z) on a subset of the imaginary line where is a negative definite function. This equation is solved by the Mellin transform of the exponential functional of Lévy processes, that is R 1 0 e s ds. Using the analytical Wiener-Hopf method we furnish the solution to this equation in a three term product involving the solutions to the equation W (z + 1) = (z)w (z) on {z 2 C : <(z) > 0}, where is any Bernstein function. The functions W we call the Bernstein-gamma functions and note that they have appeared earlier in some studies albeit in more restricted context. Via a couple of computable parameters depending on we provide a thorough characterization of W as a meromorphic function on an identifiable complex strip. Moreover, we establish universal Stirling type asymptotic which is explicit in terms of. This allows the thorough understanding of the decay of f(z) at least along the imaginary lines z = a + ir, a2 (0, 1), and an access to quantities important for many theoretical and applied studies in probability theory and analysis. Since exponential functionals appear in areas such as pricing of Asian options, branching processes in random environments, stable processes, etc., we will illustrate some applications of our new results in those areas. Joint work with Pierre Patie (Cornell) z

Asymptotic and numerical solution of fractional di erential equations Renato Spigler Roma Tre University Largo San Leonardo Murialdo, 1 00146 - Rome Italy spigler@mat.uniroma3.it The emerging and increasing importance of fractional di erential equations in modeling a number of phenomena and applications, call for the development of methods to construct or to approximate their solutions. These may be, e.g., numerical or asymptotic methods. In this talk, we will consider a perturbative approach to handle fractional ordinary di erential equations when regular or even singular perturbations a ect the model equations. We will also consider an asymptotic-numerical method to solve [the Cattaneo and] the fractional Cattaneo hyperbolic di erential equations, earlier proposed to go beyond the Fourier law in he field of heat transfer modeling.

Recent result on porous medium equations with nonlocal pressure Diana Stan BCAM Alameda Mazarredo 14, 48006 Bilbao Spain dstan@bcamath.org Félix del Teso BCAM Alameda Mazarredo 14, 48006 Bilbao Spain felix.delteso@uam.es Juan Luis Vázquez Universidad Autonoma de Madrid Madrid Spain juanluis.vazquez@uam.es We study the nonlinear di usion equation u t = r (u m 1 r( ) s u) that describes a flow through a porous medium which is driven by a nonlocal pressure. We consider constant parameters m>1and 0 <s<1, we assume that the solutions are non-negative and the problem is posed in the whole space. We prove existence of weak solutions for all integrable initial data u 0 0 and for all exponents m>1 by using a new approximating method. Finite speed of propagation is established for all m 2, which implies the existence of free boundaries. Infinite speed of propagation is proved for 1 <m<2. We also consider as initial data any non-negative measure µ with finite mass. In passing from bounded initial data to measure data we make strong use of an L 1 -L 1 smoothing e ect and other functional inequalities. We also discuss the relation with other nonlocal di usion models. References [1] Stan, D., del Teso, F., and Vázquez, J. L. Finite and infinite speed of propagation for porous medium equations with nonlocal pressure. J. Di erential Equations 260, 2 (2016), 1154 1199. [2] D. Stan, F. del. Teso, J. L. Vázquez, Transformations of self-similar solutions for porous medium equations of fractional type, Nonlinear Anal., 119 (2015), 62 73. [3] D. Stan, F. del Teso, J. L. Vázquez. Existence of weak solutions for a general porous medium equation with nonlocal pressure, preprint arxiv:1609.05139.

Semi-Markov processes and their Kolmogorov s equations Bruno Toaldo Sapienza - Università di Roma p.le Aldo Moro, 5 00195 - Roma Italy bruno.toaldo@uniroma1.it A process X(t), t 0, is said to be a semi-markov process in the sense of Gihman and Skorohod [1] if the couple (X(t), (t)), where (t) is the sojourn time in the current position, is a strong (homogeneous) Markov process. The Kolmogorov s equations of such processes are investigated. An evolutionary form (integro-di erential) for such equations is derived by using the construction of a semi-markov processes as time-changed Markov processes [2, 3, 4, 5, 6]. The time-fractional equation is an interesting particular case, obtained when the waiting times between the jumps are i.i.d. r.v. s with Mittag-Le er distribution. References [1] Gihman, I.I. and Skorohod A.V. 1975 The theory of stochastic processes II. Springer- Verlag, 1975. [2] Meerschaert M.M. and Toaldo B. 2016 Relaxation patterns and semi-markov dynamics. In revision. Available on the arxiv [3] Orsingher E., Ricciuti C. and Toaldo B. 2016 Time-inhompgeneous jump processes and variable order operators. Potential Analysis, 45(3): 435-461. [4] Orsingher E., Ricciuti C. and Toaldo B. 2016 On semi-markov processes and their Kolmogorov s integro-di erential equations. Work in progress. [5] Toaldo B. 2015 Convolution-type derivatives, hitting-times of subordinators and timechanged C 0 -semigroups. Potential Analysis, 42(1): 115 140 [6] Toaldo B. 2015 Lévy mixing related to distributed order calculus, subordinators and slow di usions. Journal of Mathematical Analysis and Applications, 430(2): 1009 1036.

The fractional non-homogeneous Poisson Process Nikolai Leonenko Cardi University Senghennydd Road, Cardi, CF24 4AG, UK Enrico Scalas University of Sussex Brighton, BN1 9QH, UK Mailan Trinh University of Sussex Brighton, BN1 9QH, UK M.Trinh@sussex.ac.uk We introduce a non-homogeneous fractional Poisson process by replacing the time variable in the fractional Poisson process of renewal type with an appropriate function of time. We characterize the resulting process by deriving its non-local governing equation. We further compute the first and second moments of the process. Eventually, we derive the distribution of arrival times. Constant reference is made to previous known results in the homogeneous case and to how they can be derived from the specialization of the non-homogeneous process. References [1] Leonenko N. et al., 2017, The fractional non-homogeneous Poisson process, Statistics & Probability Letters 120, 147-156

A Langevin approach to generate fractional transport in complex environment Paolo Paradisi ISTI - CNR di Pisa Via G. Moruzzi, 1 56124 - Pisa Italy paolo.paradisi@isti.cnr.it Silvia Vitali DIFA - Università degli Studi di Bologna viale Carlo Berti Pichat, 6 40127 - Bologna Italy silvia.vitali4@unibo.it Gastone Castellani DIFA - Università degli Studi di Bologna viale Carlo Berti Pichat, 6 40127 - Bologna Italy gastone.castellani@unibo.it Gianni Pagnini and Ikerbasque Alameda de Mazarredo, 14 E-48009 - Bilbao Basque Country - Spain gpagnini@bcamath.org The Langevin equation is characterized by several physical parameters, in particular the friction (equivalently, the relaxation or time correlation) and the noise intensity (equivalently the di usivity). We discuss here the extension of the classical process by means of a random modulation of these parameters. This random modulation can be interpreted as the e ect of the statistical characteristics of the non-homogeneous/complex medium in which the di usion occurs, e.g. the e ect of random conditions in the experimental observations. In particular we show a parameter modulation that, when it is pluged into the Langevin equation, leads to fractional di usion. After the results achieved on the basis of the generalized gray Brownian motion (ggbm) [1] and the Continuos Time Random Walk (CTRW) [2], the present approach is a further one based on the Langevin equation. These results support the physical idea that fractional di usion in random/complex media can emerge from Gaussian processes for particle motion and random parameters due to the medium. References [1] Mura, M. and Pagnini, G. 2008 Characterizations and simulations of a class of stochastic processes to model anomalous di usion. J. Phys. A: Math. Theor. 41, 285003. [2] Pagnini, G. 2014 Short note on the emergence of fractional kinetics. Physica A 409, 29 34.

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