activity
20022023
most citedNew Algorithm of the Finite Lattice Method for the High-temperature Expansion of the Ising Model in Three Dimensions

24 citations · 122 across the 22 of their papers we have counts for

collaborators

22 papers

math.CA2023★ 1 cited

Continuations and bifurcations of relative equilibria for the positive curved three body problem

Toshiaki Fujiwara, Ernesto Pérez-Chavela

The positive curved three body problem is a natural extension of the planar Newtonian three body problem to the sphere . In this paper we study the extensions of the…

math.CA2023

A new method to study relative equilibria on

Toshiaki Fujiwara, Ernesto Pérez-Chavela

We develop a new geometrical technique to study relative equilibria for a system of --positive masses, moving on the two dimensional sphere , under the influence o…

math.CA2022★ 1 cited

Equal masses Eulerian relative equilibria on a rotating meridian of S^2

Toshiaki Fujiwara, Ernesto Pérez-Chavela

Relative equilibria on a rotating meridian on in equal-mass three-body problem under the cotangent potential are determined. We show the existence of scalene and iso…

math.CA2022★ 1 cited

Three-body relative equilibria on II: Extended Lagrangian configurations

Toshiaki Fujiwara, Ernesto Perez-Chavela

This is a natural continuation of our first paper \cite{pre}, where we develop a new geometrical technique which allow us to study relative equilibria on the two sphere. We conside…

math.CA2022

Three-body relative equilibria on I: Euler configurations

Toshiaki Fujiwara, Ernesto Perez-Chavela

Using the properties of the angular momentum, we develop a new geometrical technique to study relative equilibria for a system of --bodies with positive masses, moving on the tw…

math-ph2020

Variational principle of action and group theory for bifurcation of figure-eight solutions

Toshiaki Fujiwara, Hiroshi Fukuda, Hiroshi Ozaki

Figure-eight solutions are solutions to planar equal mass three-body problem under homogeneous or inhomogeneous potentials. They are known to be invariant under the transformation…