Fish Schools See Each Other Through Glass and Start Swimming in Sync ✛

Original: "Phase synchronization of fish schools through spatial gaps"
arXiv:2609.01754v1 · 2026-09-01 · CC BY 4.0 · 1 min
Two groups of fish separated by a transparent wall synchronize their turns, and this connection works surprisingly far.

In an aquarium, two schools of fish swim in adjacent compartments separated by a transparent wall. They cannot touch each other, but they see every movement. When one school decides to turn left, the other does the same a moment later. It is as if two pendulums hanging behind glass begin to swing in time.

Fish in a school constantly change direction, but not randomly. Their collective motion settles into one of two stable states: either all swim in one direction or in the opposite. This is like a swing that can rock left or right but does not linger in the middle. Switches between states occur spontaneously, driven by the random movements of individual fish. When schools see each other, these switches begin to coincide.

Black neon tetras have a body length of only 2.5 cm, but in the experiment their schools synchronized over distances up to 40 cm, which is 16 times the length of a single fish.

The scientists measured how the strength of this synchronization depends on the width of the gap between compartments. It turned out that the connection decays with distance more slowly than one might expect. This means that fish respond to a distant group not as individuals but as an averaged movement of the whole school. At short distances, details matter; at long distances, the overall rhythm does. This result helps understand how groups of animals remain connected even when there is a physical gap between them.

Black neon tetras (Hyphessobrycon herbertaxelrodi) have an average body length of only 2.5 cm, yet in the experiment their schools synchronized over distances up to 40 cm, which is 16 times the length of an individual fish.

P(\varphi) = \frac{1}{Z_2} e^{\lambda \cos \varphi} I_0(2\kappa \cos \varphi)
Probability of observing a phase difference φ between the directions of two schools, where λ is the visual coupling strength, κ is the depth of the bistable potential, and I0 is the modified Bessel function
\lambda(d) = \lambda_0 \exp[-(d/\ell)^\beta]
The coupling strength λ decreases with distance d as a stretched exponential with characteristic length ℓ and exponent β<1
R = \langle \cos(\theta_r - \theta_l) \rangle
Mean cosine of the phase difference between the orientations of the right and left schools; R=1 means perfect synchronization, R=0 means independent switching
Concepts
phase locking synchronization brain oscillation phase amplitude coupling ocean-atmosphere coupling synapse quantum synchronization ion channel dynamics bistability mixed mode oscillations microbial collective motion standing wave brain computer interface microorganism swimming dynamics spatial coherence cellular neural interface stochastic dynamical system biological rhythm modeling ecosystem crosstalk optical switch