Integrability classification conjecture for the minimally coupled scalar-field system

Let

H=12(p12+1q12p22)kq12+Λq14+m2q22q14,H = \frac12 \left(-p_1^2 + \frac{1}{q_1^2}p_2^2 \right) - k q_1^2 + \Lambda q_1^4 + m^2q_2^2 q_1^4,

be the Hamiltonian of the minimally coupled scalar-field system. Assume Λ0\Lambda\ne0, let nn be an integer satisfying

94m2Λ=(2n+1)2,9-\frac{4m^2}{\Lambda}=(2n+1)^2,

and consider a generic energy level E0E\ne0. Integrability classification conjecture. If the system is integrable, then one of the following holds: n=1n=1 or n=2n=-2, with m=0m=0 in both cases; k=0k=0 and 94m2/Λ=(2l)29-4m^2/\Lambda=(2l)^2 for an odd integer ll; or k=0k=0 and

n+1213Z14Z15ZZ.n+\frac12\in \frac13\mathbb Z\cup\frac14\mathbb Z\cup\frac15\mathbb Z\setminus\mathbb Z.

This statement appears in the conclusions as a classification of the remaining potentially integrable parameter values on generic nonzero energy levels, complementing the necessary conditions proved earlier. Its resolution is not supplied in the paper.

Sources & referencesView supporting material

Primary source

Andrzej J. Maciejewski, Maria Przybylska, Tomasz Stachowiak and Marek Szydlowski, “Global integrability of cosmological scalar fields”, arXiv:0803.2318 (2008).

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