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Oakfield Operator Calculus Function Reference Site

Phase Coherence Measures

For angles {θj}j=1N\{\theta_j\}_{j=1}^{N}, the mean phase coherence is

R=1Nj=1NeiθjR = \left|\frac{1}{N} \sum_{j=1}^{N} e^{i\theta_j}\right|

R[0,1]R \in [0,1] measures alignment: R=1R=1 indicates identical phases; R0R \approx 0 indicates phase dispersion.


Replacing θj\theta_j by θj+ϕ\theta_j + \phi leaves RR unchanged; only relative phase differences matter.

RR equals the magnitude of the circular mean of unit phasors: R=1NjeiθjR = \left|\frac{1}{N}\sum_j e^{i\theta_j}\right|. Larger RR indicates tighter angular concentration.


For two phases,

R=12(eiθ1+eiθ2)=1+cos(θ1θ2)2=cos ⁣(θ1θ22)R = \left|\tfrac{1}{2}(e^{i\theta_1} + e^{i\theta_2})\right| = \sqrt{\tfrac{1+\cos(\theta_1-\theta_2)}{2}} = \left|\cos\!\left(\tfrac{\theta_1-\theta_2}{2}\right)\right|

For uniformly distributed phases, RR tends to 00 as NN \to \infty.




  1. 📜 Synchronization Order Parameters

    Coherence measures of the form R=1NjeiθjR=\left|\frac{1}{N}\sum_j e^{i\theta_j}\right| are standard in circular statistics and became especially prominent through the Kuramoto model as an order parameter for collective synchronization.

  2. 🌍 Modern Perspective

    In numerical simulations, coherence is used as a compact scalar diagnostic for phase organization across space, time, or modal decompositions.


  • Kuramoto, Chemical Oscillations, Waves, and Turbulence
  • Mardia & Jupp, Directional Statistics