Discontinuity at the Pole
Abstract
The exchange of a particle whose mass is taken to zero need not reproduce the exchange of a particle that is strictly massless from the outset. We derive a general on-shell diagnostic of the well-known discontinuity between the exchange of a massless particle and the massless limit of a massive-particle exchange, valid for a mediator of arbitrary integer spin S. Our main observation is that this discontinuity can be identified directly at the level of the pole residue. We find that, in four dimensions, the residue is governed by a Chebyshev polynomial in the massless case and by a Legendre polynomial in the massless limit of the massive case. For S = 2, this reproduces the van Dam-Veltman-Zakharov discontinuity. For general S, it provides a simple and compact higher-spin analogue from on-shell factorisation. The discontinuity is probed, in principle, by the leading post-Newtonian correction to the non-relativistic potential between two massive scalar bodies.
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BibTeX
@misc{haslehner2026discontinuity,
title = {{Discontinuity at the Pole}},
author = {Dominik Haslehner and Elena Kaiser and Javi Serra and Andreas Weiler},
howpublished = {arXiv},
year = {2026},
month = oct,
doi = {10.48550/arxiv.2610.31759},
eprint = {2610.31759},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2610.31759},
}
RIS
TY - UNPB
TI - Discontinuity at the Pole
AU - Dominik Haslehner
AU - Elena Kaiser
AU - Javi Serra
AU - Andreas Weiler
PY - 2026
DA - 2026/10/22
PB - arXiv
DO - 10.48550/arxiv.2610.31759
UR - https://arxiv.org/abs/2610.31759
AB - The exchange of a particle whose mass is taken to zero need not reproduce the exchange of a particle that is strictly massless from the outset. We derive a general on-shell diagnostic of the well-known discontinuity between the exchange of a massless particle and the massless limit of a massive-particle exchange, valid for a mediator of arbitrary integer spin S. Our main observation is that this discontinuity can be identified directly at the level of the pole residue. We find that, in four dimensions, the residue is governed by a Chebyshev polynomial in the massless case and by a Legendre polynomial in the massless limit of the massive case. For S = 2, this reproduces the van Dam-Veltman-Zakharov discontinuity. For general S, it provides a simple and compact higher-spin analogue from on-shell factorisation. The discontinuity is probed, in principle, by the leading post-Newtonian correction to the non-relativistic potential between two massive scalar bodies.
ER -