Classification conjecture for codimension-four \mathfrak{bms}_3 Poisson pairs

Let bms3\mathfrak{bms}_3^* be the dual of the centrally extended bms3\mathfrak{bms}_3 algebra, let c1c_1 be its first central charge, and let {,}LPbms3\{,\}_\mathrm{LP}^{\mathfrak{bms}_3^*} and {,}0bms3\{,\}_0^{\mathfrak{bms}_3^*} denote the Lie–Poisson and frozen Poisson brackets. For non-vanishing c1c_1, consider Poisson pairs of codimension 44 on bms3\mathfrak{bms}_3^*, classified by the type of their frozen point. Classification conjecture. All such Poisson pairs are classified into the following fifteen classes:

(dx22,0;dx22,0),(dx2,0;dx22,0),(dx22,1;dx22,0),(dx2,1;dx22,0);(0,1;0,1),(dx22,1;0,1),(0,2;0,1),(dx22,2;0,1);(dx22,1;dx22,1),(dx2,1;dx22,1),(dx22,2;dx22,1),(dx2,2;dx22,1);(dx22,0;0,0),(0,1;0,0),(dx22,1;0,0).\begin{gathered} \left(\frac{dx^2}{2},0;\frac{dx^2}{2},0\right),\quad\left(dx^2,0;\frac{dx^2}{2},0\right),\quad\left(\frac{dx^2}{2},1;\frac{dx^2}{2},0\right),\quad\left(dx^2,1;\frac{dx^2}{2},0\right);\\ (0,1;0,1),\quad\left(\frac{dx^2}{2},1;0,1\right),\quad(0,2;0,1),\quad\left(\frac{dx^2}{2},2;0,1\right);\\ \left(\frac{dx^2}{2},1;\frac{dx^2}{2},1\right),\quad\left(dx^2,1;\frac{dx^2}{2},1\right),\quad\left(\frac{dx^2}{2},2;\frac{dx^2}{2},1\right),\quad\left(dx^2,2;\frac{dx^2}{2},1\right);\\ \left(\frac{dx^2}{2},0;0,0\right),\quad(0,1;0,0),\quad\left(\frac{dx^2}{2},1;0,0\right). \end{gathered}

The source presents this classification as an argument based on the relation between frozen points and codimension-four coadjoint orbits; it gives no resolution status beyond the stated claim.

Sources & referencesView supporting material

Primary source

Corentin Vitel, “Integrability in Asymptotic Symmetries of Spacetime: the BMS_3 scenario”, arXiv:2607.28454 (2026).

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