Demonstration of Broadband Non-Resonant Time-Crystal Amplification in Microwaves

Alexander V. Kildishev; Dimitrios Peroulis; Ludmila J. Prokopeva; Mordechai Segev; Thomas R. Jones

arxiv: 2605.21014 · v1 · pith:NLSG65OMnew · submitted 2026-05-20 · ⚛️ physics.optics · physics.app-ph

Demonstration of Broadband Non-Resonant Time-Crystal Amplification in Microwaves

Thomas R. Jones , Ludmila J. Prokopeva , Alexander V. Kildishev , Mordechai Segev , Dimitrios Peroulis This is my paper

Pith reviewed 2026-05-21 02:10 UTC · model grok-4.3

classification ⚛️ physics.optics physics.app-ph

keywords photonic time crystaltime-modulated capacitormomentum band gapbroadband amplificationmicrowave circuitFloquet modesnon-resonant gainparametric resonance

0 comments

The pith

A time-modulated capacitor microwave circuit produces stable broadband gain from a photonic time crystal momentum band gap.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper demonstrates the first experimental realization of a photonic time crystal in the microwave regime through a purely time-modulated capacitor circuit on a microstrip line. Optical modulation of photodiodes creates 94.5 percent temporal variation in effective capacitance at 200 MHz. The resulting exponential growth overcomes losses and finite-size effects to deliver positive terminal gain across a continuous 65 MHz band, with a peak of 3.8 dB. A narrow central resonance reaches 4.8 dB but is traced to spatial inhomogeneities, while the broadband feature matches the momentum band gap expected from an ideal distributed photonic time crystal.

Core claim

The PTC exponential growth can overcome losses and finite-size constraints of a practical spatio-temporal system and yield stable positive terminal gain over a continuous broadband frequency range. Broadband amplification consistent with a momentum band gap is observed, with a peak gain of 3.8 dB over a 65 MHz bandwidth, while finite-size and loss mechanisms transform the ideal semicircular PTC gain profile into a continuous asymmetric non-Lorentzian gain band characterized by a Pearson type IV distribution.

What carries the argument

The momentum band gap created by periodic temporal modulation of capacitance, which supports phase-invariant non-resonant amplification and slow-light behavior in the Floquet-mode structure of the time crystal.

If this is right

The finite microwave circuit inherits defining PTC features including phase-invariant non-resonant amplification.
Slow-light behavior appears inside the momentum band gap.
Losses and finite size convert the ideal semicircular gain profile into a continuous asymmetric gain band following a Pearson type IV distribution.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

The separation of broadband momentum-band-gap gain from narrow parametric peaks offers a route to design time-modulated systems that favor one mechanism over the other.
Similar lumped-to-distributed mappings could guide fabrication of time-crystal amplifiers at higher frequencies or in integrated platforms.
The demonstrated robustness against losses suggests time-crystal gain could be combined with other modulation schemes for tunable broadband response.

Load-bearing premise

The broadband gain specifically arises from the momentum band gap of the photonic time crystal rather than from ordinary parametric amplification or circuit parasitics.

What would settle it

A direct measurement showing that the broadband gain profile fails to match the predicted asymmetric non-Lorentzian shape or lacks the expected slow-light dispersion inside the band gap would indicate the amplification is not due to photonic time crystal physics.

read the original abstract

We report an optically modulated experimental realization of a photonic time crystal (PTC) in the microwave regime, demonstrating for the first time that the PTC exponential growth can overcome losses and finite-size constraints of a practical spatio-temporal system and yield stable positive terminal gain over a continuous broadband frequency range. The developed experimental platform is a purely time-modulated capacitor (TMC) microwave circuit based on a microstrip transmission line, in which synchronized optical modulation of reverse-biased photodiodes generates strong (94.5 %) temporal modulation of the effective capacitance at 200 MHz. Broadband amplification consistent with a momentum band gap (MBG), a defining signature of photonic time-crystal physics, is observed, with a peak gain of 3.8 dB over a 65 MHz bandwidth. In addition, a narrow parametric resonance appears at the center of the band gap, reaching 4.8 dB. This sharp peak is associated with the spatial inhomogeneities of the lumped-element realization, while the corresponding homogeneous distributed system retains the Floquet-mode structure of a photonic time crystal. We show that finite microwave TMC implementations inherit the defining physics of PTCs, including phase-invariant non-resonant amplification and slow-light behavior inside the momentum band gap, while finite-size and loss mechanisms transform the ideal semicircular PTC gain profile into a continuous asymmetric non-Lorentzian gain band characterized by a Pearson type IV distribution.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Desk Editor's Note private letter to a colleague

This paper gives the first microwave experiment claiming stable broadband gain from a photonic time-crystal momentum band gap in a time-modulated capacitor circuit, but the link to PTC physics over ordinary parametric effects stays model-dependent.

read the letter

The main takeaway is an experimental microwave circuit that uses optical modulation of photodiodes on a microstrip line to create 94.5% capacitance variation at 200 MHz and produces 3.8 dB gain across 65 MHz plus a sharper central peak of 4.8 dB. They tie the broad band to the momentum band gap of an underlying photonic time crystal while blaming the narrow peak on spatial inhomogeneities in the lumped realization. That is the new piece: a hardware bridge from ideal PTC theory to a lossy finite system that still shows positive terminal gain over a continuous band rather than just at isolated resonances. The setup itself is straightforward and the numbers are concrete, which is useful for anyone trying to move time-crystal ideas out of theory and into RF hardware. They also note that the finite system turns the ideal semicircular gain profile into an asymmetric Pearson-type distribution, which matches what one would expect once losses and boundaries are included. The soft spot is the attribution step. The broadband gain is said to come from the homogeneous PTC Floquet structure, yet all data are taken on the inhomogeneous lumped circuit. Standard time-varying capacitance in a transmission line can generate parametric gain with similar bandwidth and shape once finite length and parasitics are folded in. The paper distinguishes the two by appealing to the distributed limit recovering ideal PTC dispersion, but without spatially resolved fields, phase-sensitive measurements, or a direct baseline comparison that isolates the homogeneous contribution, the separation rests on the model rather than a decisive control. The central claim therefore holds only if that mapping is accepted. Readers working on time-varying media or parametric amplifiers in microwaves will get the most from it, because it supplies a concrete platform and measured gain values even if the interpretation needs tightening. The experimental core is solid enough that a serious referee should see it, with the main request being clearer evidence that rules out conventional mechanisms for the broad component.

Referee Report

2 major / 2 minor

Summary. The manuscript reports an optically modulated experimental realization of a photonic time crystal (PTC) in the microwave regime using a microstrip transmission line with synchronized optical modulation of reverse-biased photodiodes to achieve 94.5% temporal modulation of effective capacitance at 200 MHz. It claims observation of broadband amplification of 3.8 dB over a 65 MHz bandwidth consistent with a momentum band gap (MBG), plus a narrow central parametric resonance of 4.8 dB attributed to spatial inhomogeneities of the lumped-element circuit, while arguing that finite TMC implementations retain PTC Floquet-mode structure, phase-invariant non-resonant amplification, and slow-light behavior, with losses and finite size yielding an asymmetric non-Lorentzian (Pearson type IV) gain profile.

Significance. If the attribution of the observed broadband gain specifically to PTC momentum band gap physics holds, the result would be significant for demonstrating that PTC exponential growth can overcome losses and finite-size constraints in a practical spatio-temporal system to produce stable positive terminal gain over a continuous broadband frequency range, extending time-crystal concepts into microwave engineering with potential implications for non-resonant amplification.

major comments (2)

[Results section (gain spectra and discussion of homogeneous vs. inhomogeneous limits)] Results section (gain spectra and discussion of homogeneous vs. inhomogeneous limits): The central claim that the 65 MHz broadband 3.8 dB gain arises from the MBG of an underlying homogeneous PTC Floquet structure (while the narrow 4.8 dB peak is due to spatial inhomogeneities) is model-dependent. The experimental data are taken on the inhomogeneous lumped circuit; no direct measurement (e.g., spatially resolved field or phase-sensitive gain) is described that would falsify a purely parametric or parasitic origin for the broadband component, as standard time-varying capacitance in a microstrip can produce similar asymmetric profiles once losses and finite length are included.
[Theoretical modeling / mapping to ideal PTC (near Eq. describing Floquet dispersion or TMC to distributed limit)] Theoretical modeling / mapping to ideal PTC (near Eq. describing Floquet dispersion or TMC to distributed limit): The full derivation of how the lumped-element circuit with 94.5% modulation maps onto the ideal PTC dispersion relation and recovers the MBG without additional fitted parameters is not visible; post-hoc attribution of the narrow peak to inhomogeneities while claiming the broad band matches the homogeneous limit requires explicit comparison (e.g., simulated dispersion or parameter-free prediction of the Pearson type IV shape) to confirm the distinction is forced by the data.

minor comments (2)

[Figure captions] Figure captions and text: clarify the exact definition of 'terminal gain' and how it is extracted from S-parameters to avoid ambiguity with internal field growth.
[References] References: ensure all prior work on time-modulated capacitors and parametric amplification in microstrip lines is cited for context on distinguishing mechanisms.

Simulated Author's Rebuttal

2 responses · 1 unresolved

We thank the referee for the thorough review and constructive feedback on our manuscript demonstrating broadband non-resonant amplification in a microwave photonic time crystal. We address the major comments below, clarifying the theoretical mapping and the distinction between the momentum band gap and parametric features. Where appropriate, we indicate revisions to strengthen the presentation.

read point-by-point responses

Referee: Results section (gain spectra and discussion of homogeneous vs. inhomogeneous limits): The central claim that the 65 MHz broadband 3.8 dB gain arises from the MBG of an underlying homogeneous PTC Floquet structure (while the narrow 4.8 dB peak is due to spatial inhomogeneities) is model-dependent. The experimental data are taken on the inhomogeneous lumped circuit; no direct measurement (e.g., spatially resolved field or phase-sensitive gain) is described that would falsify a purely parametric or parasitic origin for the broadband component, as standard time-varying capacitance in a microstrip can produce similar asymmetric profiles once losses and finite length are included.

Authors: We agree that direct spatially resolved measurements would provide stronger falsification of alternative origins. Our current setup uses a lumped photodiode array on a microstrip line, precluding easy spatial probing. However, the broadband gain is not reproduced by a purely parametric model of the inhomogeneous circuit; it requires the Floquet dispersion of the homogeneous limit. We will add in revision a direct comparison of the measured spectrum to a parameter-free simulation of the lossy finite-length homogeneous PTC, which yields the observed asymmetric Pearson type IV profile and the 65 MHz bandwidth. The narrow central peak remains outside this prediction and is reproduced only when spatial modulation inhomogeneity is introduced, consistent with the known photodiode variations. This supports the attribution without post-hoc fitting. revision: partial
Referee: Theoretical modeling / mapping to ideal PTC (near Eq. describing Floquet dispersion or TMC to distributed limit): The full derivation of how the lumped-element circuit with 94.5% modulation maps onto the ideal PTC dispersion relation and recovers the MBG without additional fitted parameters is not visible; post-hoc attribution of the narrow peak to inhomogeneities while claiming the broad band matches the homogeneous limit requires explicit comparison (e.g., simulated dispersion or parameter-free prediction of the Pearson type IV shape) to confirm the distinction is forced by the data.

Authors: The mapping from the measured 94.5% temporal capacitance modulation to the distributed PTC limit is derived in the supplementary material via the time-periodic transmission-line equations and Floquet-Bloch analysis, but we acknowledge it is not sufficiently explicit in the main text. In revision we will expand the theoretical section to include the step-by-step reduction to the ideal PTC dispersion, showing that the momentum band gap opens at the measured modulation frequency and depth without additional parameters. We will add a figure comparing the homogeneous Floquet-mode gain spectrum (including finite-size and loss effects) directly to the data; this reproduces the broadband component and the Pearson type IV asymmetry as a natural consequence of the model. The narrow peak is absent from this homogeneous prediction and appears only with added spatial inhomogeneity, confirming the distinction is data-driven rather than post-hoc. revision: yes

standing simulated objections not resolved

Direct spatially resolved field or phase-sensitive measurements to independently falsify parametric versus PTC origins, as these require a substantially modified experimental apparatus beyond the scope of the present work.

Circularity Check

0 steps flagged

No significant circularity in experimental claims or modeling

full rationale

The paper presents an experimental demonstration of broadband gain in a time-modulated microwave circuit, attributing the 65 MHz band to the momentum band gap of a photonic time crystal while ascribing the narrow central peak to spatial inhomogeneities in the lumped-element realization. This distinction is drawn from standard Floquet analysis of homogeneous vs. inhomogeneous systems and direct comparison to measured terminal gain data, without any derivation that reduces by construction to fitted inputs or self-referential definitions. No load-bearing self-citations, ansatz smuggling, or renaming of known results appear in the reported chain; the central result is an observation of positive gain overcoming losses, supported by independent circuit measurements rather than a closed mathematical loop.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The central claim rests on standard electromagnetic theory for time-varying media plus the assumption that the observed gain profile matches the ideal PTC momentum band gap after accounting for losses and finite size. No new particles or forces are postulated. The modulation depth and frequency are experimental controls rather than fitted free parameters for the gain result.

axioms (2)

standard math Maxwell's equations hold for time-periodically modulated media and produce Floquet modes with momentum band gaps
Invoked implicitly when the paper equates the measured broadband gain to the defining signature of a photonic time crystal.
domain assumption The lumped-element TMC circuit sufficiently approximates the homogeneous distributed PTC for the broadband gain component
Stated when the authors note that the homogeneous distributed system retains the Floquet-mode structure while the actual realization shows an asymmetric gain band.

pith-pipeline@v0.9.0 · 5805 in / 1618 out tokens · 38482 ms · 2026-05-21T02:10:17.895943+00:00 · methodology

discussion (0)

Lean theorems connected to this paper

Citations machine-checked in the Pith Canon. Every link opens the source theorem in the public Lean library.

IndisputableMonolith/Cost/FunctionalEquation.lean washburn_uniqueness_aczel echoes

?

echoes
ECHOES: this paper passage has the same mathematical shape or conceptual pattern as the Recognition theorem, but is not a direct formal dependency.

Im(Ω)p = cosh^{-1}(2/(1−(Cm_sq)^2) sin²(kd/2)−1); finite TMC inherits MBG Floquet instability with Pearson type IV terminal gain
IndisputableMonolith/Foundation/RealityFromDistinction.lean reality_from_one_distinction unclear

?

unclear
Relation between the paper passage and the cited Recognition theorem.

N=5 cell lumped TMC, 200 MHz trapezoidal modulation, 65 MHz broadband 3.8 dB gain from MBG

What do these tags mean?

matches: The paper's claim is directly supported by a theorem in the formal canon.
supports: The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
extends: The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
uses: The paper appears to rely on the theorem as machinery.
contradicts: The paper's claim conflicts with a theorem or certificate in the canon.
unclear: Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.

Reference graph

Works this paper leans on

22 extracted references · 22 canonical work pages

[1]

Amplified emission and lasing in photonic time crystals

Lyubarov, M.; Lumer, Y .; Dikopoltsev, A.; Lustig, E.; Sharabi, Y .; Segev, M. Amplified emission and lasing in photonic time crystals. Science 2022, 377, 425–428

work page 2022
[2]

M.; Boltasseva, A.; Segev, M

Lustig, E.; Segal, O.; Saha, S.; Fruhling, C.; Shalaev, V . M.; Boltasseva, A.; Segev, M. Photonic time-crystals – fundamental concepts. Opt. Express 2023, 31, 9165–9170

work page 2023
[3]

A.; Silveirinha, M

Galiffi, E.; Tirole, R.; Yin, S.; Li, H.; Vezzoli, S.; Huidobro, P. A.; Silveirinha, M. G.; Sapienza, R.; Alù, A.; Pendry, J. B. Photonics of time-varying media. Adv. Photonics 2022, 4, 014002

work page 2022
[4]

Four-dimensional optics using time-varying metamaterials

Engheta, N. Four-dimensional optics using time-varying metamaterials. Science 2023, 379, 1190– 1191

work page 2023
[5]

M.; Engheta, N

Pacheco-Peña, V .; Solís, D. M.; Engheta, N. Time -varying electromagnetic media: opinion. Opt. Mater. Express 2022, 12, 3829–3840

work page 2022
[6]

Spacetime metamaterials— Part II: Theory and applications

Caloz, C.; Deck- Léger, Z.-L. Spacetime metamaterials— Part II: Theory and applications. IEEE Trans. Antennas Propag. 2020, 68, 1583–1612

work page 2020
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M.; Kastner, R.; Engheta, N

Solís, D. M.; Kastner, R.; Engheta, N. Time-varying materials in the presence of dispersion: plane- wave propagation in a Lorentzian medium with temporal discontinuity. Photonics Res. 2021, 9, 1842– 1853

work page 2021
[8]

Electrodynamics of photonic temporal interfaces

Galiffi, E.; Martínez Solís, D.; Yin, S.; Engheta, N.; Alù, A. Electrodynamics of photonic temporal interfaces. Light Sci. Appl. 2025, 14, 338

work page 2025
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Space-time Fresnel prism

Li, Z.; Ma, X.; Bahrami, A.; Deck -Léger, Z.-L.; Caloz, C. Space-time Fresnel prism. Phys. Rev. Applied 2023, 20, 054029

work page 2023
[10]

Spatiotemporal cascading of dielectric waveguides

Pacheco-Peña, V .; Engheta, N. Spatiotemporal cascading of dielectric waveguides. Opt. Mater. Express 2024, 14, 1062–1073

work page 2024
[11]

Nonlocal effects in temporal metamaterials

Rizza, C.; Castaldi, G.; Galdi, V . Nonlocal effects in temporal metamaterials. Nanophotonics 2022, 11, 1285–1295

work page 2022
[12]

Disordered photonic time crystals

Sharabi, Y .; Lustig, E.; Segev, M. Disordered photonic time crystals. Phys. Rev. Lett. 2021, 126, 163902

work page 2021
[13]

C.; Vezzoli, S.; Tirole, R.; Alù, A.; Sapienza, R

Galiffi, E.; Harwood, A. C.; Vezzoli, S.; Tirole, R.; Alù, A.; Sapienza, R. Optical coherent perfect absorption and amplification in a time-varying medium. Nat. Photonics 2026, 20, 163–169

work page 2026
[14]

M.; Engheta, N

Solís, D. M.; Engheta, N. Functional analysis of the polarization response in linear time -varying media: A generalization of the Kramers–Kronig relations. Phys. Rev. B 2021, 103, 144303

work page 2021
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A photonic Floquet scattering matrix for wavefront-shaping in time-periodic media

Globosits, D.; Hüpfl, J.; Rotter, S. A photonic Floquet scattering matrix for wavefront-shaping in time-periodic media. arXiv 2024, arXiv:2403.19311

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G.; Rahman, S.; Stefanou, N.; Almpanis, E.; Papanikolaou, N.; Verfürth, B.; Rockstuhl, C

Garg, P.; Lamprianidis, A. G.; Rahman, S.; Stefanou, N.; Almpanis, E.; Papanikolaou, N.; Verfürth, B.; Rockstuhl, C. Two-step homogenization of spatiotemporal metasurfaces using an eigenmode-based approach. Opt. Mater. Express 2024, 14, 549–563

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W.; Min, B

Lee, K.; Kim, Y .; Kim, K. W.; Min, B. Energy transport velocity in photonic time crystals. arXiv 2026, arXiv:2602.03453

work page arXiv 2026
[18]

Observation of temporal reflection and broadband frequency translation at photonic time interfaces

Moussa, H.; Xu, G.; Yin, S.; Galiffi, E.; Ra’di, Y .; Alù, A. Observation of temporal reflection and broadband frequency translation at photonic time interfaces. Nat. Phys. 2023, 19, 863–868

work page 2023
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R.; Kildishev, A

Jones, T. R.; Kildishev, A. V .; Segev, M.; Peroulis, D. Time -reflection of microwaves by a fast optically-controlled time-boundary. Nat. Commun. 2024, 15, 6786

work page 2024
[20]

S.; Asadchy, V

Wang, X.; Mirmoosa, M. S.; Asadchy, V . S.; Rockstuhl, C.; Fan, S.; Tretyakov, S. A. Metasurface- based realization of photonic time crystals. Sci. Adv. 2023, 9, eadg7541

work page 2023
[21]

Observation of wave amplification and temporal topological state in a non- synthetic photonic time crystal

Xiong, J.; Zhang, X.; Duan, L.; Wang, J.; Long, Y .; Hou, H.; Yu, L.; Zou, L.; Zhang, B. Observation of wave amplification and temporal topological state in a non- synthetic photonic time crystal. Nat. Commun. 2025, 16, 11182

work page 2025
[22]

F.; Zheludev, N

Liu, T.; Ou, J.- Y .; MacDonald, K. F.; Zheludev, N. I. Photonic metamaterial analogue of a continuous time crystal. Nat. Phys. 2023, 19, 986–992

work page 2023

[1] [1]

Amplified emission and lasing in photonic time crystals

Lyubarov, M.; Lumer, Y .; Dikopoltsev, A.; Lustig, E.; Sharabi, Y .; Segev, M. Amplified emission and lasing in photonic time crystals. Science 2022, 377, 425–428

work page 2022

[2] [2]

M.; Boltasseva, A.; Segev, M

Lustig, E.; Segal, O.; Saha, S.; Fruhling, C.; Shalaev, V . M.; Boltasseva, A.; Segev, M. Photonic time-crystals – fundamental concepts. Opt. Express 2023, 31, 9165–9170

work page 2023

[3] [3]

A.; Silveirinha, M

Galiffi, E.; Tirole, R.; Yin, S.; Li, H.; Vezzoli, S.; Huidobro, P. A.; Silveirinha, M. G.; Sapienza, R.; Alù, A.; Pendry, J. B. Photonics of time-varying media. Adv. Photonics 2022, 4, 014002

work page 2022

[4] [4]

Four-dimensional optics using time-varying metamaterials

Engheta, N. Four-dimensional optics using time-varying metamaterials. Science 2023, 379, 1190– 1191

work page 2023

[5] [5]

M.; Engheta, N

Pacheco-Peña, V .; Solís, D. M.; Engheta, N. Time -varying electromagnetic media: opinion. Opt. Mater. Express 2022, 12, 3829–3840

work page 2022

[6] [6]

Spacetime metamaterials— Part II: Theory and applications

Caloz, C.; Deck- Léger, Z.-L. Spacetime metamaterials— Part II: Theory and applications. IEEE Trans. Antennas Propag. 2020, 68, 1583–1612

work page 2020

[7] [7]

M.; Kastner, R.; Engheta, N

Solís, D. M.; Kastner, R.; Engheta, N. Time-varying materials in the presence of dispersion: plane- wave propagation in a Lorentzian medium with temporal discontinuity. Photonics Res. 2021, 9, 1842– 1853

work page 2021

[8] [8]

Electrodynamics of photonic temporal interfaces

Galiffi, E.; Martínez Solís, D.; Yin, S.; Engheta, N.; Alù, A. Electrodynamics of photonic temporal interfaces. Light Sci. Appl. 2025, 14, 338

work page 2025

[9] [9]

Space-time Fresnel prism

Li, Z.; Ma, X.; Bahrami, A.; Deck -Léger, Z.-L.; Caloz, C. Space-time Fresnel prism. Phys. Rev. Applied 2023, 20, 054029

work page 2023

[10] [10]

Spatiotemporal cascading of dielectric waveguides

Pacheco-Peña, V .; Engheta, N. Spatiotemporal cascading of dielectric waveguides. Opt. Mater. Express 2024, 14, 1062–1073

work page 2024

[11] [11]

Nonlocal effects in temporal metamaterials

Rizza, C.; Castaldi, G.; Galdi, V . Nonlocal effects in temporal metamaterials. Nanophotonics 2022, 11, 1285–1295

work page 2022

[12] [12]

Disordered photonic time crystals

Sharabi, Y .; Lustig, E.; Segev, M. Disordered photonic time crystals. Phys. Rev. Lett. 2021, 126, 163902

work page 2021

[13] [13]

C.; Vezzoli, S.; Tirole, R.; Alù, A.; Sapienza, R

Galiffi, E.; Harwood, A. C.; Vezzoli, S.; Tirole, R.; Alù, A.; Sapienza, R. Optical coherent perfect absorption and amplification in a time-varying medium. Nat. Photonics 2026, 20, 163–169

work page 2026

[14] [14]

M.; Engheta, N

Solís, D. M.; Engheta, N. Functional analysis of the polarization response in linear time -varying media: A generalization of the Kramers–Kronig relations. Phys. Rev. B 2021, 103, 144303

work page 2021

[15] [15]

A photonic Floquet scattering matrix for wavefront-shaping in time-periodic media

Globosits, D.; Hüpfl, J.; Rotter, S. A photonic Floquet scattering matrix for wavefront-shaping in time-periodic media. arXiv 2024, arXiv:2403.19311

work page arXiv 2024

[16] [16]

G.; Rahman, S.; Stefanou, N.; Almpanis, E.; Papanikolaou, N.; Verfürth, B.; Rockstuhl, C

Garg, P.; Lamprianidis, A. G.; Rahman, S.; Stefanou, N.; Almpanis, E.; Papanikolaou, N.; Verfürth, B.; Rockstuhl, C. Two-step homogenization of spatiotemporal metasurfaces using an eigenmode-based approach. Opt. Mater. Express 2024, 14, 549–563

work page 2024

[17] [17]

W.; Min, B

Lee, K.; Kim, Y .; Kim, K. W.; Min, B. Energy transport velocity in photonic time crystals. arXiv 2026, arXiv:2602.03453

work page arXiv 2026

[18] [18]

Observation of temporal reflection and broadband frequency translation at photonic time interfaces

Moussa, H.; Xu, G.; Yin, S.; Galiffi, E.; Ra’di, Y .; Alù, A. Observation of temporal reflection and broadband frequency translation at photonic time interfaces. Nat. Phys. 2023, 19, 863–868

work page 2023

[19] [19]

R.; Kildishev, A

Jones, T. R.; Kildishev, A. V .; Segev, M.; Peroulis, D. Time -reflection of microwaves by a fast optically-controlled time-boundary. Nat. Commun. 2024, 15, 6786

work page 2024

[20] [20]

S.; Asadchy, V

Wang, X.; Mirmoosa, M. S.; Asadchy, V . S.; Rockstuhl, C.; Fan, S.; Tretyakov, S. A. Metasurface- based realization of photonic time crystals. Sci. Adv. 2023, 9, eadg7541

work page 2023

[21] [21]

Observation of wave amplification and temporal topological state in a non- synthetic photonic time crystal

Xiong, J.; Zhang, X.; Duan, L.; Wang, J.; Long, Y .; Hou, H.; Yu, L.; Zou, L.; Zhang, B. Observation of wave amplification and temporal topological state in a non- synthetic photonic time crystal. Nat. Commun. 2025, 16, 11182

work page 2025

[22] [22]

F.; Zheludev, N

Liu, T.; Ou, J.- Y .; MacDonald, K. F.; Zheludev, N. I. Photonic metamaterial analogue of a continuous time crystal. Nat. Phys. 2023, 19, 986–992

work page 2023