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PreprintCC BY 4.0arXiv

Quicksilver Asymptotics and Pole Arrays for q-Painlevé II

Abstract

We construct local families of solutions of the q-difference second Painlevé equation that vanish at infinity with a common algebraic expansion, parameterised by the amplitude of an exponentially small correction. Considering an appropriate boundary region, a formal expansion that retains two independently excited exponential perturbations is developed, and subsequent transseries summation predicts the location of simple poles. Adopting a q-theta function realisation of the exponential factors, we prove an asymptotic pole-location formula for a one-parameter family of true solutions. These poles approach the aforementioned boundaries where exponential behaviour fundamentally changes, providing an analogue of pole arrays near anti-Stokes directions in classical Painlevé asymptotics.

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BibTeX
@misc{holroyd2026quicksilver,
  title = {{Quicksilver Asymptotics and Pole Arrays for $q$-Painlevé II}},
  author = {Joshua Holroyd},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.27525},
  eprint = {2610.27525},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.27525},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Quicksilver Asymptotics and Pole Arrays for q-Painlevé II
AU  - Joshua Holroyd
PY  - 2026
DA  - 2026/10/20
PB  - arXiv
DO  - 10.48550/arxiv.2610.27525
UR  - https://arxiv.org/abs/2610.27525
AB  - We construct local families of solutions of the q-difference second Painlevé equation that vanish at infinity with a common algebraic expansion, parameterised by the amplitude of an exponentially small correction. Considering an appropriate boundary region, a formal expansion that retains two independently excited exponential perturbations is developed, and subsequent transseries summation predicts the location of simple poles. Adopting a q-theta function realisation of the exponential factors, we prove an asymptotic pole-location formula for a one-parameter family of true solutions. These poles approach the aforementioned boundaries where exponential behaviour fundamentally changes, providing an analogue of pole arrays near anti-Stokes directions in classical Painlevé asymptotics.
ER  -