Characterize the limiting intensity of the maximum-particle thinning

Determine whether the limiting Poisson point process obtained from the maximum-particle thinning M(θ_t^λ) has intensity measure of the form A_∞e^{-μx}dx+B_∞dx, where μ=λ+√(λ²−2) and A_∞,B_∞ are possibly random non-negative constants.

Background

The paper studies the large-time behavior of a branching Brownian motion started from a point process θ. To analyze the leading particles, it introduces the non-Markovian thinning M(θ_tλ), which retains the maximum descendant from each initial atom. The authors explain that any limiting object should be a Poisson point process, but unlike the uniformly tagged-particle thinning, M(θ_tλ) is non-Markovian, so an invariant-measure or Choquet–Deny argument is unavailable to identify its intensity.

The proposed form includes both an exponentially decaying component and a constant component. The constant term is important because its positivity would correspond to a limiting Poisson point process without a finite top particle, while the later results show that fixed-point limits of the full BBM must nevertheless have finite top particles almost surely.

References

However, resembling the case of U(θtλ), we guess and conjecture that the intensity measure in this case has to be of the form A∞ e{-μ x} dx + B_∞ dx, where μ = λ + √(λ² -2). We emphasize that B_∞ can be positive with positive probability.

Locally finite fixed points of branching Brownian motion  (2608.23202 - Chen et al., 24 Aug 2026) in Section 1, subsection “Heuristic ideas and outline of the proof”