Reciprocity by Design - The shape of the loss in space-time modulated media

A modulated medium whose permittivity and conductivity depend on both position and time may be invariant under an operation that reverses time and translates space at once. Two such space-time glide operations exist in one spatial dimension, and the literature gives both the same name; this paper treats the one that reverses time, and separates it from its sister at the outset. We show that invariance under a whole one-parameter family of these operations preserves reciprocity. Closure of the operation forces the spatial offset to half a unit cell and leaves the time origin free, so the family is a line rather than a point. Two conditions already in the literature — glide time-reversal on one side, symmetry of the modulation under plain time reversal on the other — are its two endpoints, and the interior is reachable from neither: a modulation is exhibited that satisfies the family condition exactly while failing the published time-reversal criterion for every choice of time origin, and it is reciprocal to the precision of the computation. The proof splits into three independent relations. The first uses the symmetry and, in a lossy medium, reverses the sign of the conductivity. The second uses only that the material functions are real, and reverses that sign back. The third uses nothing at all and holds for every medium. The split is what makes the lossy case provable rather than merely observed, and it yields a criterion on the shape of the loss rather than on its size: a spatially uniform conductivity is harmless at any strength, while a conductivity of the wrong spatial parity breaks the conclusion however small it is. Finally, the violation is priced. Where the symmetry is broken by a controlled amount, the asymmetry of the band structure is linear in that amount over a range located from the data, which turns a statement about what cannot be done into a tolerance budget for what can. Numerical verification accompanies every claim; each measuring test is paired with an input on which the claim must fail, and the scripts are deterministic and deposited with this record. The condition is sufficient, not necessary. A case is recorded in which reciprocity survives although the proof does not reach it, and a selection rule suggested by one family of profiles is shown to disappear on another that satisfies the same condition. Neither is claimed here.

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Publication Details

Journal
Zenodo (CERN European Organization for Nuclear Research)
Published
2026-09-15
DOI
https://doi.org/10.5281/zenodo.22765346
Primary Topic
Numerical methods in inverse problems
Type
preprint
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Reciprocity by Design - The shape of the loss in space-time modulated media

László Márk
Zenodo (CERN European Organization for Nuclear Research)
Numerical methods in inverse problems
preprint

Reciprocity by Design - The shape of the loss in space-time modulated media

László Márk
preprint en

Abstract

A modulated medium whose permittivity and conductivity depend on both position and time may be invariant under an operation that reverses time and translates space at once. Two such space-time glide operations exist in one spatial dimension, and the literature gives both the same name; this paper treats the one that reverses time, and separates it from its sister at the outset. We show that invariance under a whole one-parameter family of these operations preserves reciprocity. Closure of the operation forces the spatial offset to half a unit cell and leaves the time origin free, so the family is a line rather than a point. Two conditions already in the literature — glide time-reversal on one side, symmetry of the modulation under plain time reversal on the other — are its two endpoints, and the interior is reachable from neither: a modulation is exhibited that satisfies the family condition exactly while failing the published time-reversal criterion for every choice of time origin, and it is reciprocal to the precision of the computation. The proof splits into three independent relations. The first uses the symmetry and, in a lossy medium, reverses the sign of the conductivity. The second uses only that the material functions are real, and reverses that sign back. The third uses nothing at all and holds for every medium. The split is what makes the lossy case provable rather than merely observed, and it yields a criterion on the shape of the loss rather than on its size: a spatially uniform conductivity is harmless at any strength, while a conductivity of the wrong spatial parity breaks the conclusion however small it is. Finally, the violation is priced. Where the symmetry is broken by a controlled amount, the asymmetry of the band structure is linear in that amount over a range located from the data, which turns a statement about what cannot be done into a tolerance budget for what can. Numerical verification accompanies every claim; each measuring test is paired with an input on which the claim must fail, and the scripts are deterministic and deposited with this record. The condition is sufficient, not necessary. A case is recorded in which reciprocity survives although the proof does not reach it, and a selection rule suggested by one family of profiles is shown to disappear on another that satisfies the same condition. Neither is claimed here.

Zenodo (CERN European Organization for Nuclear Research)
Peace, Justice and strong institutions
Numerical methods in inverse problems
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