Colloquium
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準定常状態にあるハミルトン平均場モデルの外力に対する線形応答
小川駿
7月1日(金)13:30
It is a common view that Hamiltonian systems with long-range
interaction are trapped in non-equilibrium states called
quasi-stationary states. A way to analyze such a Hamiltonian system is
to use the Vlasov equation or collision-less Boltzmann equation, and
quasi-stationary states are recognized as stable stationary solutions
to the Vlasov equation[1].
In this talk, we use one of the simplest models with long-range
interaction, the Hamiltonian mean-filed (HMF) model. We apply the
linear response theory[2] to this system in spatially homogeneous
quasi-stationary states. As a result, we can obtain the asymptotic
forms of magnetization and susceptibility exactly. Moreover, it should
be noted that the critical behavior of the susceptibility like the
Curie-Weiss law is shown from this result straightforwardly by using
the result exhibited in the article [3].
[1] A. Campa, T. Dauxois and S. Ruffo, Phys. Rep. 480, 57 (2009).
[2] D.J.Evans and P.J.Morriss, "Statistical mechanics of
nonequilibrium liquids,"
(Cambridge University Press,2008) and R. Kubo, M. Toda and N.
Hashitsume, “Statistical physics II. Nonequilibrium statistical
mechanics,” (Springer, 1985).
[3] S. Ogawa and Y.Y.Yamaguchi, submitted.
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