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  "slug": "levy-qsd-exponential-moments-restart",
  "title": "Exact exponential moments of interval quasi-stationary laws for Lévy processes, and the saturation of idealised QSD restart",
  "shortTitle": "Restart from a quasi-stationary law: the exact constant and the real budget scale",
  "url": "https://evidencepress.org/releases/levy-qsd-exponential-moments-restart/",
  "oneLine": "A conjecture of Garcia, Bermolen, Jonckheere and Shneer on restart-based rare-event simulation holds up to a constant, but the constant is not one (0.850 in their own example), and idealised quasi-stationary restart saturates at budgets of order exp(ηL), far below the range stated in their restart theorem.",
  "abstract": "Restarting a simulation from a quasi-stationary distribution (QSD) is a simple way to look for a rare high level L of a process that drifts away from it, for example in rare-event simulation or in exploration for model-free simulation and reinforcement learning. Its efficiency is governed by an exponential moment of the QSD on the interval (0, L), and Garcia, Bermolen, Jonckheere and Shneer (Stochastic Systems, 2026) conjectured that this moment grows like exp((λ*−η)L), noting that this is exact for Brownian motion. For Lévy processes with a Gaussian component and jumps of either sign, this candidate proves that every exponential moment of the interval QSD has an exact limit after normalisation, with constants written through the ladder-height exponents of the Esscher-centred process; the core input is an exact L⁻² asymptotic for the two boundary layers of the centred QSD. The conjecture therefore holds on the logarithmic scale and up to constants, but its ratio-one reading fails: the constant is below one for every spectrally negative process with jumps, above one for every spectrally positive one, and 0.85014864899… in the source's own example (certified by interval arithmetic). For idealised QSD restart the success rate is asymptotic to R* exp(−ηL) with explicit R*, and the curve 1 − exp(−R* B exp(−ηL)) is accurate uniformly in the budget B in relative error, so the linear budget regime of the source's restart theorem is B = O(exp(ηL)), not B = o(exp(λ*L)). The moment theorem is extended to spectrally negative processes without a Gaussian part, and the first-order finite-L corrections are identified in the source model. AI-assisted, unrefereed candidate; no external peer review, independent reproduction or formal verification is claimed.",
  "datePublished": "2026-10-21",
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    "Anonymous"
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  "keywords": [
    "quasi-stationary distribution",
    "Lévy processes",
    "rare-event simulation",
    "restart",
    "Esscher transform",
    "Wiener–Hopf factorisation",
    "ladder heights",
    "Fleming–Viot"
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  "keyResults": [
    "Exact moments (Theorem 2.2, proof): for a Lévy process with a Gaussian component, jumps of either sign and a Cramér root λ*, every exponential moment M_L(θ) of the QSD on (0, L) has an exact normalised limit: bounded for θ < η (recovering Kyprianou and Palmowski's half-line formula), of order L² at θ = η, and ∼ C(θ) exp((θ−η)L) for θ > η, with C(θ) given by ladder-height exponents of the Esscher-centred process.",
    "The engine (Theorem 2.3, proof): the centred QSD is a sine-shaped bulk with two thin boundary layers whose masses are exactly of order L⁻²; the left layer follows the ascending ladder renewal function, the right one the descending ladder. The conjecture's constant is C* = K_r(λ*−η)/K_ℓ(η) = G₊(λ*−η)/G₋(η).",
    "The ratio-one reading fails (Proposition 2.9, proof; certified enclosure): C* = 1 for Brownian motion, C* < 1 for every spectrally negative process with jumps, C* > 1 for every spectrally positive one, and C* = 0.85014864899… in the source's own example.",
    "Restart saturates at exp(ηL) (Theorem 2.6 and Corollary 2.7, proof): the success rate of idealised QSD restart is r_L ∼ R* exp(−ηL), the curve 1 − exp(−R* B exp(−ηL)) has relative error at most |a_L − 1| at every budget, and the linear regime of the source's restart theorem is B = O(exp(ηL)), not B = o(exp(λ*L)); an exact Brownian example refutes the wider range.",
    "Extensions: spectrally negative processes without a Gaussian part, C* = η²ψ″(η)/(2κ∞) ≤ 1 (Theorem 8.1, proof under a scale-function positivity condition); in the source model the killing rate sees an effective length L + δ₊ + δ₋ and both constants carry relative error π²(δ₋ − δ₊)/(2L) ≈ 0.497/L (Theorems 9.1–9.2, proof given standard QSD-density regularity)."
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    {
      "citation": "Garcia, Bermolen, Jonckheere and Shneer (2026), Efficiency of parallel and restart exploration strategies in model-free stochastic simulations. Stochastic Systems 16(3), 264–288 (arXiv:2503.03565).",
      "url": "https://doi.org/10.1287/stsy.2025.0108",
      "doi": "10.1287/stsy.2025.0108"
    },
    {
      "citation": "Kyprianou and Palmowski (2006), Quasi-stationary distributions for Lévy processes. Bernoulli 12(4), 571–581.",
      "url": "https://doi.org/10.3150/bj/1155735927",
      "doi": "10.3150/bj/1155735927"
    },
    {
      "citation": "Lambert (2000), Completely asymmetric Lévy processes confined in a finite interval. Annales de l'Institut Henri Poincaré, Probabilités et Statistiques 36(2), 251–274.",
      "url": "https://doi.org/10.1016/S0246-0203(00)00126-6",
      "doi": "10.1016/S0246-0203(00)00126-6"
    },
    {
      "citation": "Kolb and Savov (2014), Exponential ergodicity of killed Lévy processes in a finite interval. Electronic Communications in Probability 19, paper 31.",
      "url": "https://doi.org/10.1214/ECP.v19-3006",
      "doi": "10.1214/ECP.v19-3006"
    },
    {
      "citation": "Bertoin and Doney (1994), Cramér's estimate for Lévy processes. Statistics & Probability Letters 21(5), 363–365.",
      "url": "https://doi.org/10.1016/0167-7152(94)00032-8",
      "doi": "10.1016/0167-7152(94)00032-8"
    },
    {
      "citation": "Villemonais (2014), General approximation method for the distribution of Markov processes conditioned not to be killed. ESAIM: Probability and Statistics 18, 441–467.",
      "url": "https://doi.org/10.1051/ps/2013045",
      "doi": "10.1051/ps/2013045"
    },
    {
      "citation": "Cérou and Guyader (2007), Adaptive multilevel splitting for rare event analysis. Stochastic Analysis and Applications 25(2), 417–443.",
      "url": "https://doi.org/10.1080/07362990601139628",
      "doi": "10.1080/07362990601139628"
    },
    {
      "citation": "Glasserman, Heidelberger, Shahabuddin and Zajic (1999), Multilevel splitting for estimating rare event probabilities. Operations Research 47(4), 585–600.",
      "url": "https://doi.org/10.1287/opre.47.4.585",
      "doi": "10.1287/opre.47.4.585"
    },
    {
      "citation": "Ecoffet, Huizinga, Lehman, Stanley and Clune (2021), First return, then explore. Nature 590, 580–586.",
      "url": "https://doi.org/10.1038/s41586-020-03157-9",
      "doi": "10.1038/s41586-020-03157-9"
    }
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