Thinning-invariant partition structures from stationary random measures

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Let ρ\trimmed\rho\trimmed be a stationary random measure on R\mathbb{R} with intensity-one asymptotic density, let K\mathscr{K} be the disjoint union of M+,1(R)×(0,1)\mathcal{M}_{+,1}(\mathbb{R})\times(0,1) and 11, and let Mst(K)\mathcal{M}_{\mathrm{st}}(\mathscr{K}) be the measures invariant under shifts of the ρ\rho coordinate. For Q\trimmed\thisQ\trimmed\this in Mst(K)\mathcal{M}_{\mathrm{st}}(\mathscr{K}), define NQ\mathcal{N}_Q by mixing the Poisson--Kingman structures ν(Λρ,m,0)\nu_{(\Lambda_{\rho,m},0)} and the structure ν(0,1)\nu_{(0,1)}. The thinning-invariant partition-structure conjecture. For any Q,QMst(K)Q,Q'\in\mathcal{M}_{\mathrm{st}}(\mathscr{K}), if NQ=NQ\mathcal{N}_Q=\mathcal{N}_{Q'} then Q=QQ=Q', and the set of thinning-invariant μM(Δ)\mu\in\mathcal{M}(\Delta_\infty) is precisely {NQ:QMst(K)}\{\mathcal{N}_Q:Q\in\mathcal{M}_{\mathrm{st}}(\mathscr{K})\}. This claims both uniqueness of the mixing measure and a complete classification of thinning-invariant partition structures; the supplied text gives no resolution status.

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Primary source

Shannon Starr, Brigitta Vermesi and Ang Wei, “About Thinning Invariant Partition Structures”, arXiv:1106.0267 (2012).

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