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Solvable model of the collective motion of heterogeneous particles interacting on a sphere
Adaptation and Self-Organizing Systems · Submitted 14 Jan 2014
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim I show that the motion of the centre of mass of an infinite number of heterogeneous particles whose natural-frequency matrices are obtained from a class of multivariate Lorentz distribution is given by an M-dimensional ordinary differential equation in closed form.
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The abstract, sentence by sentence
I propose a model of mutually interacting particles on an M-dimensional unit sphere. I derive the dynamics of the particles by extending the dynamics of the Kuramoto-Sakaguchi model. The dynamics include a natural-frequency matrix, which determines the motion of a particle with no external force, and an external force vector. The position (state variable) of a particle at a given time is obtained by the projection transformation of the initial position of the particle. The same projection transformation gives the position of the particles with the same natural-frequency matrix. I show that the motion of the centre of mass of an infinite number of heterogeneous particles whose natural-frequency matrices are obtained from a class of multivariate Lorentz distribution is given by an M-dimensional ordinary differential equation in closed form. This result is an extension of the Ott-Antonsen theory.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | I propose a model of mutually interacting particles on an M-dimensional unit sphere. | contribution 0.92 | 0.91 | 0.04 | asserted 0.97 |
| s1 | I derive the dynamics of the particles by extending the dynamics of the Kuramoto-Sakaguchi model. | method 0.94 | 0.94 | 0.04 | asserted 1.00 |
| s2 | The dynamics include a natural-frequency matrix, which determines the motion of a particle with no external force, and an external force vector. | method 0.93 | 0.74 | 0.04 | asserted 1.00 |
| s3 | The position (state variable) of a particle at a given time is obtained by the projection transformation of the initial position of the particle. | result 0.75 | 0.85 | 0.06 | asserted 1.00 |
| s4 | The same projection transformation gives the position of the particles with the same natural-frequency matrix. | result 0.80 | 0.83 | 0.06 | asserted 1.00 |
| s5 | I show that the motion of the centre of mass of an infinite number of heterogeneous particles whose natural-frequency matrices are obtained from a class of multivariate Lorentz distribution is given by an M-dimensional ordinary differential equation in closed form. | result 0.99 | 0.94 | 0.82 | asserted 1.00 |
| s6 | This result is an extension of the Ott-Antonsen theory. | interpretation 0.85 | 0.51 | 0.12 | asserted 1.00 |
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The paper
Original abstract
I propose a model of mutually interacting particles on an M-dimensional unit sphere. I derive the dynamics of the particles by extending the dynamics of the Kuramoto-Sakaguchi model. The dynamics include a natural-frequency matrix, which determines the motion of a particle with no external force, and an external force vector. The position (state variable) of a particle at a given time is obtained by the projection transformation of the initial position of the particle. The same projection transformation gives the position of the particles with the same natural-frequency matrix. I show that the motion of the centre of mass of an infinite number of heterogeneous particles whose natural-frequency matrices are obtained from a class of multivariate Lorentz distribution is given by an M-dimensional ordinary differential equation in closed form. This result is an extension of the Ott-Antonsen theory.
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