Abstract
This paper considers time-evolving generalised network, intended as networks where (i)
the edges connecting the nodes are nonlinear, (ii) stochastic processes are continuously indexed
over both vertices and edges and (iii) the topology is allowed to change over time, that is: vertices
and edges can disappear at subsequent time instants and edges may change in shape and length.
Topological structures satisfying (i) and (ii) are usually represented through special classes of
graphs, termed graphs with Euclidean edges. We build a rigorous mathematical framework for
time-evolving networks. We consider both cases of linear and circular time, where, for the latter,
the generalised network exhibits a periodic structure. Our findings allow to illustrate pros and
cons of each setting. Our approach allows to build proper semi-distances for the temporallyevolving topological structures of the networks. Generalised networks become semi-distance
spaces whenever equipped with semi-distances. Our final effort is then devoted to guiding the
reader through the appropriate choice of classes of functions that allow to build random fields on
the time-evolving networks, via their kernels, that are composed with the temporally-evolving
semi-distances topological structure.
Information
| Preprint No. | SS-2024-0345 |
|---|---|
| Manuscript ID | SS-2024-0345 |
| Complete Authors | Tobia Filosi, Claudio Agostinelli, Emilio Porcu |
| Corresponding Authors | Emilio Porcu |
| Emails | georgepolya01@gmail.com |
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Acknowledgments
The authors are grateful to Havard Rue for insightful discussions during the preparation
of this manuscript. This project has also been sustained by the prompt help of Valeria
Simoncini and Valter Moretti.
Claudio Agostinelli was partially funded by BaC INF-ACT S4 - BEHAVE-MOD
PE00000007 PNRR M4C2 Inv. 1.3 - NextGenerationEU, CUP: I83C22001810007 and
by the PRIN funding scheme of the Italian Ministry of University and Research (Grant
No. P2022N5ZNP).
Supplementary Materials
. However, we stress that the semi-distance and the resulting
covariance functions remain the same for x = 0 (thus L⋆= L), as shown in Proposition