the face of uncertainty and disruptions, which can propagate in time and space throughout the system and
lead to heavy congestion, make the system fragile.
The main goal of this study is to introduce the application of antifragile control to traffic control and
optimization under uncertainty, volatility, and variability. As coined in the book of Taleb Taleb (2012),
antifragility is a property of a system to gain from uncertainty, randomness, and volatility, opposite to
what fragility would incur. An antifragile system’s response to external perturbations is beyond robust,
such that small stressors can strengthen the future response of the system by adding a strong anticipation
component. For the closed-loop system we employ the model introduced by Axenie et al. (2021) that uses
oscillator-based dynamics modelling. Such an approach has the advantage of capturing both the periodicity
in daily/seasonal traffic patterns and the periodicity of the local signal timings, and as shown in Axenie
et al. (2021) is robust and efficient at scale. We now propose an alternative control mechanism, based on
the antifragile control framework introduced by Axenie et al. (2022) and built on top of the principles in
the seminal work of Taleb & Douady (2013).
1.2. Oscillator-based network modelling and interaction dynamics
Oscillator-based modelling and control is an approach emerging from physics that proves to be a plausi-
ble application in traffic control. In a very good review and perspective, the study of Chedjou & Kyamakya
(2018) introduced the formalism of oscillator-based traffic modelling and control. Despite the strong math-
ematical grounding, the proposed approach was static, in that it removed all convergence and dynamics
of the oscillator-based model by replacing it with the steady-state solution. Such an approach proves its
benefits at the single cross level, as the authors claim, but will fail in large-scale heterogeneous road networks
(i.e. non-uniform road geometry, disrupted traffic patterns, volatility of traffic load, uncertainty of weather
conditions). The approach we take in the current study is to design a closed-loop antifragile control system
in which a novel variable structure sliding mode controller (see Utkin (2008)) is designed for a nonlinearly-
coupled oscillators model based on the model of Strogatz (2000). We demonstrate through our experiments
that the oscillator-based model with antifragile control can stabilize in a plausible solution of signal timing
under dynamical demand changes based on measurement of local traffic data. A similar oscillator-based
model approach was used in the work of Nishikawa & Kuroe (2004) and later in the work of Fang et al.
(2013) as area-wide signal control of an urban traffic network. Yet, due to their complex-valued dynamics
and optimization, the systems could not capture both the spatial and temporal correlations under a realistic
computational cost for real-world deployment.
1.3. Fragility-robustness-antifragility continuum in traffic control
Traffic dynamics is highly nonlinear and sensitive to multiple sources of uncertainty. Here we go beyond
uncertainty in capturing the real dynamics of traffic through a model (i.e. structured/parametric uncertain-
ties) and consider the changes that disruptions, such as weather, accidents, social events, and infrastructure
availability (i.e. unstructured uncertainties, or un-modelled dynamics), induce in the overall flow of cars.
The uncertainty, volatility, and variability inherent in such disruptions are described by a stochastic evo-
lution in the space-time-intensity reference system. The compound effect of such disruptions (typically
additive in nature) reflects itself in computed measures of quality of traffic, for instance travel time for
cars over a certain itinerary. Such unstructured uncertainties determine traffic signal re-computations that,
subsequently, alter the shape of the travel time distribution and, hence, the overall travel time distribution
– as depicted in Figure 2.
Going further with our travel time example, the change in the shape of the distribution of the travel time
can be described through the actual type of response (i.e. the shape) to the space-time-intensity character-
istics of the uncertainty. We can then describe the distribution of such responses to uncertainty-triggered
signal re-computation with respect to the travel time itself, as shown in Figure 3. As also show in the excel-
lent work of Taleb & West (2022), if we combine the reaction to uncertainties, or the uncertainty response
(i.e. signal re-computation) S(T ravelT ime), with the distribution of the travel time P(T ravelT ime), we
can describe the probability distribution of the signal re-computation P(S(T ravelT ime)). The core idea
is that we can vary the parameters of the signal re-computation such that the shape of S(T ravelT ime)
changes to handle the changes in P(T ravelT ime) given uncertainty.
3