Coherent Release Fronts in Krylov Chains and Thermal AdS2 Response
Abstract
We study coherent release from a finite serial Krylov sector into an exact conformal tail with asymptotically linear Lanczos coefficients. We derive the cumulative occupation up to a cut that moves to greater Krylov depth with time, tracking the probability accumulated behind the propagating front. This quantity separates the release dynamics of the finite sector from subsequent propagation through the tail. The tail sets the logarithmic transit scale, while the finite sector shapes the resulting distribution. The early edge records the number of serial steps before emission, while the late edge reflects slow resonances and interference and can also exhibit logarithmic enhancements. Thus, one- and two-site sectors can share the same leading resonance in their continued-fraction descriptions yet produce distinct cumulative occupation patterns. We illustrate this framework in thermal AdS2, where a dressed oscillator yields, in the weak-coupling limit, a two-site shallow sector coupled to the conformal tail.
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BibTeX
@misc{alishahiha2026coherent,
title = {{Coherent Release Fronts in Krylov Chains and Thermal AdS$_2$ Response}},
author = {Mohsen Alishahiha},
howpublished = {arXiv},
year = {2026},
month = oct,
doi = {10.48550/arxiv.2610.01862},
eprint = {2610.01862},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2610.01862},
note = {CC BY 4.0},
}
RIS
TY - UNPB
TI - Coherent Release Fronts in Krylov Chains and Thermal AdS_2 Response
AU - Mohsen Alishahiha
PY - 2026
DA - 2026/10/14
PB - arXiv
DO - 10.48550/arxiv.2610.01862
UR - https://arxiv.org/abs/2610.01862
AB - We study coherent release from a finite serial Krylov sector into an exact conformal tail with asymptotically linear Lanczos coefficients. We derive the cumulative occupation up to a cut that moves to greater Krylov depth with time, tracking the probability accumulated behind the propagating front. This quantity separates the release dynamics of the finite sector from subsequent propagation through the tail. The tail sets the logarithmic transit scale, while the finite sector shapes the resulting distribution. The early edge records the number of serial steps before emission, while the late edge reflects slow resonances and interference and can also exhibit logarithmic enhancements. Thus, one- and two-site sectors can share the same leading resonance in their continued-fraction descriptions yet produce distinct cumulative occupation patterns. We illustrate this framework in thermal AdS_2, where a dressed oscillator yields, in the weak-coupling limit, a two-site shallow sector coupled to the conformal tail.
ER -