In network science, the activity-driven model is a temporal network model in which each node has a randomly-assigned "activity potential",[1] which governs how it links to other nodes over time.
Each node j {\displaystyle j} (out of N {\displaystyle N} total) has its activity potential x i {\displaystyle x_{i}} drawn from a given distribution F ( x ) {\displaystyle F(x)} . A sequence of timesteps unfolds, and in each timestep each node j {\displaystyle j} forms ties to m {\displaystyle m} random other nodes at rate a i = η x i {\displaystyle a_{i}=\eta x_{i}} (more precisely, it does so with probability a i Δ t {\displaystyle a_{i}\,\Delta t} per timestep). All links are then deleted after each timestep.
Properties of time-aggregated network snapshots are able to be studied in terms of F ( x ) {\displaystyle F(x)} . For example, since each node j {\displaystyle j} after T {\displaystyle T} timesteps will have on average m η x i T {\displaystyle m\eta x_{i}T} outgoing links, the degree distribution after T {\displaystyle T} timesteps in the time-aggregated network will be related to the activity-potential distribution by
Spreading behavior according to the SIS epidemic model was investigated on activity-driven networks, and the following condition was derived for large-scale outbreaks to be possible:
where β {\displaystyle \beta } is the per-contact transmission probability, λ {\displaystyle \lambda } is the per-timestep recovery probability, and ( ⟨ a ⟩ {\displaystyle \langle a\rangle } , ⟨ a 2 ⟩ {\displaystyle \langle a^{2}\rangle } ) are the first and second moments of the random activity-rate a j {\displaystyle a_{j}} .
A variety of extensions to the activity-driven model have been studied. One example is activity-driven networks with attractiveness,[2] in which the links that a given node forms do not attach to other nodes at random, but rather with a probability proportional to a variable encoding nodewise attractiveness. Another example is activity-driven networks with memory,[3] in which activity-levels change according to a self-excitation mechanism.