Gauge Matters More Than Curvature
Abstract
Recent orthodoxy, which we call Curvature Fundamentalism, posits that the field strength F on spacetime exhausts the physically significant content of electromagnetism, at least on prosaic (contractible) spacetimes. We argue that it is gauge invariance that constrains physical significance. As a result, there are physically significant quantities that F does not capture, even on contractible spacetimes. We show that this result is robust: in the presence of charged matter fields, there are interference experiments whose outcome cannot be predicted by F or any other point-local gauge invariant quantities on the basis of initial Cauchy data. We prove this using the example of relative phase of a Klein-Gordon-Maxwell field, and use it to identify a context in which the widely-claimed equivalence between the Maxwell-Faraday formulation EM1 and the gauge formulation EM2 of electromagnetism is untenable, and that new strategies may be needed for the reductionist project.
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BibTeX
@misc{gomes2026gauge,
title = {{Gauge Matters More Than Curvature}},
author = {Henrique Gomes and Bryan W Roberts},
howpublished = {arXiv},
year = {2026},
month = sep,
doi = {10.48550/arxiv.2609.13017},
eprint = {2609.13017},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2609.13017},
note = {CC BY-NC-SA 4.0},
}
RIS
TY - UNPB
TI - Gauge Matters More Than Curvature
AU - Henrique Gomes
AU - Bryan W Roberts
PY - 2026
DA - 2026/09/11
PB - arXiv
DO - 10.48550/arxiv.2609.13017
UR - https://arxiv.org/abs/2609.13017
AB - Recent orthodoxy, which we call Curvature Fundamentalism, posits that the field strength F on spacetime exhausts the physically significant content of electromagnetism, at least on prosaic (contractible) spacetimes. We argue that it is gauge invariance that constrains physical significance. As a result, there are physically significant quantities that F does not capture, even on contractible spacetimes. We show that this result is robust: in the presence of charged matter fields, there are interference experiments whose outcome cannot be predicted by F or any other point-local gauge invariant quantities on the basis of initial Cauchy data. We prove this using the example of relative phase of a Klein-Gordon-Maxwell field, and use it to identify a context in which the widely-claimed equivalence between the Maxwell-Faraday formulation EM_1 and the gauge formulation EM_2 of electromagnetism is untenable, and that new strategies may be needed for the reductionist project.
ER -