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arxiv: 2412.20686 · v3 · submitted 2024-12-30 · ⚛️ physics.optics · cond-mat.mes-hall· physics.app-ph

Surface Plasmon Polaritons: Creation Dynamics and Interference of Slow and Fast Propagating SPPs at a Temporal Boundary

Pith reviewed 2026-05-23 07:21 UTC · model grok-4.3

classification ⚛️ physics.optics cond-mat.mes-hallphysics.app-ph
keywords surface plasmon polaritonstemporal boundaryGreen's functionLaplace transformSPP interferencedynamic formationdipole excitation
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The pith

A sudden change in media at a temporal boundary creates dynamic SPPs and induces interference between their slow and fast propagating modes.

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

The paper establishes a theoretical framework for surface plasmon polaritons excited by a dipole source in a system whose media configuration changes abruptly at a temporal boundary. It uses three-dimensional Green's function analysis in the Laplace transform domain to model the scenario. This framework demonstrates how SPPs form dynamically over time and how slow and fast modes interfere due to the temporal boundary. A reader would care because the work shows how time boundaries affect wave behavior at material interfaces.

Core claim

The authors establish that three-dimensional Green's function analysis performed in the Laplace transform domain captures both the dynamic formation of surface plasmon polaritons and the interference between slow and fast propagating SPPs that arises when the media configuration changes suddenly at a temporal boundary.

What carries the argument

Three-dimensional Green's function analysis in the Laplace transform domain, which models dipole-excited SPPs under an abrupt temporal change in the surrounding media.

If this is right

  • SPPs form dynamically in time following the temporal boundary.
  • Interference occurs specifically between slow and fast propagating SPPs due to the time boundary.
  • The analysis supplies insight into the temporal formation process and the resulting interference.
  • The framework applies to a dipole-excited material system that supports SPPs.

Where Pith is reading between the lines

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

  • The same Green's function approach in the Laplace domain could be adapted to study other wave types such as acoustic or electromagnetic waves at temporal interfaces.
  • Time-varying plasmonic structures might be designed to exploit or suppress the slow-fast mode interference.
  • Experimental setups with ultrafast media switching could test the predicted interference patterns directly.

Load-bearing premise

The sudden change in media configuration at a temporal boundary can be accurately captured by three-dimensional Green's function analysis performed in the Laplace transform domain.

What would settle it

Time-domain simulations or measurements that show no interference between slow and fast SPP modes after an abrupt media change at a temporal boundary would falsify the claim.

Figures

Figures reproduced from arXiv: 2412.20686 by George W. Hanson, Jay A. Berres, S. Ali Hassani Gangaraj.

Figure 1
Figure 1. Figure 1: Model for the general case of a single interface between [PITH_FULL_IMAGE:figures/full_fig_p002_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: Real part of the z-component of each component of [PITH_FULL_IMAGE:figures/full_fig_p007_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: Real part of the z-component of each respective [PITH_FULL_IMAGE:figures/full_fig_p008_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: Real part of the electric field versus time for the [PITH_FULL_IMAGE:figures/full_fig_p009_4.png] view at source ↗
Figure 6
Figure 6. Figure 6: Real part of the electric field versus time plots regarding [PITH_FULL_IMAGE:figures/full_fig_p010_6.png] view at source ↗
Figure 4
Figure 4. Figure 4: Based on these results we can see that it is possible [PITH_FULL_IMAGE:figures/full_fig_p011_4.png] view at source ↗
read the original abstract

We establish the theoretical framework for a material system that supports surface plasmon polaritions (SPPs) excited by a dipole excitation, where the media configuration suddenly changes at a temporal boundary. We employ three-dimensional Green's function analysis in the Laplace transform domain. We use this framework to demonstrate dynamic SPP formation and time-boundary-induced interference of slow and fast propagating SPPs. This analysis provides insight into how SPPs are formed in time and how they interfere at a temporal boundary.

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.

Referee Report

1 major / 2 minor

Summary. The manuscript establishes a theoretical framework for SPPs excited by a dipole source in a system whose media configuration undergoes an abrupt change at a temporal boundary. It employs three-dimensional Green's function analysis performed in the Laplace-transform domain to demonstrate dynamic SPP formation and the interference between slow and fast propagating SPP modes induced by the time boundary, providing insight into the temporal evolution and interference of SPPs.

Significance. If the Laplace-domain treatment correctly recovers the physical jump conditions, the work supplies a concrete analytic route to time-domain SPP dynamics at temporal interfaces, a topic of growing interest in time-varying plasmonics and metamaterials. The explicit demonstration of slow/fast mode interference constitutes a falsifiable prediction that could be tested experimentally.

major comments (1)
  1. [Abstract and §2] The central claim that the Laplace-domain 3D Green's function fully encodes the instantaneous media discontinuity (and therefore the correct amplitudes and interference of the slow and fast SPPs) is load-bearing. The manuscript must show explicitly, either by deriving the time-domain jump conditions on the tangential fields or by direct comparison with a time-domain solution at the switching instant, that the inverse Laplace transform reproduces the required discontinuities; otherwise the reported interference pattern risks being an artifact of the transform rather than a physical result. (Abstract and §2)
minor comments (2)
  1. [§2] Notation for the Laplace variable and the inverse transform should be stated once at the beginning of §2 and used consistently; the current alternation between s and p is confusing.
  2. [Figure captions] Figure captions should indicate the value of the temporal switching time t0 and the observation plane so that the interference fringes can be reproduced.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for the constructive feedback. Below we provide a point-by-point response to the major comment.

read point-by-point responses
  1. Referee: [Abstract and §2] The central claim that the Laplace-domain 3D Green's function fully encodes the instantaneous media discontinuity (and therefore the correct amplitudes and interference of the slow and fast SPPs) is load-bearing. The manuscript must show explicitly, either by deriving the time-domain jump conditions on the tangential fields or by direct comparison with a time-domain solution at the switching instant, that the inverse Laplace transform reproduces the required discontinuities; otherwise the reported interference pattern risks being an artifact of the transform rather than a physical result. (Abstract and §2)

    Authors: We agree with the referee that explicit validation is required. The current version of the manuscript does not provide this derivation or comparison. We will revise the manuscript to include an explicit derivation of the time-domain jump conditions from the Laplace-domain solution in section 2. This will involve showing that the inverse Laplace transform yields the correct discontinuities in the tangential fields at the temporal boundary. We will also add a direct comparison with a time-domain numerical simulation to confirm the interference between slow and fast SPPs. revision: yes

Circularity Check

0 steps flagged

No circularity: derivation uses standard Green's function methods in Laplace domain without reduction to inputs or self-citation chains

full rationale

The abstract outlines a theoretical framework employing three-dimensional Green's function analysis in the Laplace transform domain to model sudden media changes at a temporal boundary and demonstrate SPP formation and interference. No equations, fitted parameters, or self-citations are quoted that reduce the central claims to their own inputs by construction. The approach is presented as an application of established electromagnetic methods, remaining self-contained against external benchmarks such as standard Green's function techniques in time-domain electromagnetics. The skeptic concern addresses potential validity of the Laplace representation for instantaneous discontinuities but does not identify any definitional or fitted-input circularity.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Abstract provides no information on free parameters, axioms, or invented entities; full text required for assessment.

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Reference graph

Works this paper leans on

54 extracted references · 54 canonical work pages

  1. [1]

    Velocity modulation of electromagnetic waves,

    F. R. Morgenthaler, “Velocity modulation of electromagnetic waves,” IEEE Transactions on Microwave Theory and Techniques , vol. 6, no. 2, pp. 167–172, Apr. 1958

  2. [2]

    Wave propagation in time-varying media,

    L. Felsen and G. Whitman, “Wave propagation in time-varying media,” IEEE Transactions on Antennas and Propagation , vol. 18, no. 2, pp. 242–253, Mar. 1970

  3. [3]

    Transmission of electromagnetic waves into time-varying media,

    R. Fante, “Transmission of electromagnetic waves into time-varying media,” IEEE Transactions on Antennas and Propagation, vol. 19, no. 3, pp. 417–424, May 1971

  4. [4]

    Characteristics of electromagnetic waves propagating in time varying media,

    T. Ruiz, C. Wright, and J. Smith, “Characteristics of electromagnetic waves propagating in time varying media,” IEEE Transactions on Antennas and Propagation , vol. 26, no. 2, pp. 358–361, Mar. 1978

  5. [5]

    Wave propagation and dipole radiation in a suddenly created plasma,

    C.-L. Jiang, “Wave propagation and dipole radiation in a suddenly created plasma,” IEEE Transactions on Antennas and Propagation , vol. 23, no. 1, pp. 83–90, Jan. 1975

  6. [6]

    Reflection and transmission of electromagnetic waves at a temporal boundary,

    Y . Xiao, D. N. Maywar, and G. P. Agrawal, “Reflection and transmission of electromagnetic waves at a temporal boundary,” Optics Letters , vol. 39, no. 3, p. 574, Jan. 2014

  7. [7]

    Reflection and transmission of elec- tromagnetic waves at a temporal boundary: comment,

    M. I. Bakunov and A. V . Maslov, “Reflection and transmission of elec- tromagnetic waves at a temporal boundary: comment,” Optics Letters , vol. 39, no. 20, p. 6029, Oct. 2014

  8. [8]

    Spacetime metamaterials— part I: General concepts,

    C. Caloz and Z.-L. Deck-Leger, “Spacetime metamaterials— part I: General concepts,” IEEE Transactions on Antennas and Propagation , vol. 68, no. 3, pp. 1569–1582, Mar. 2020

  9. [9]

    Spacetime metamaterials— part II: Theory and applications,

    C. Caloz and Z.-L. Deck-Leger, “Spacetime metamaterials— part II: Theory and applications,” IEEE Transactions on Antennas and Propa- gation, vol. 68, no. 3, pp. 1583–1598, Mar. 2020

  10. [10]

    Time-varying materials in the presence of dispersion: plane-wave propagation in a Lorentzian medium with temporal discontinuity,

    D. M. Sol ´ıs, R. Kastner, and N. Engheta, “Time-varying materials in the presence of dispersion: plane-wave propagation in a Lorentzian medium with temporal discontinuity,” Photonics Research, vol. 9, no. 9, p. 1842, Aug. 2021

  11. [11]

    Temporal boundaries in electromagnetic materials,

    J. Gratus, R. Seviour, P. Kinsler, and D. A. Jaroszynski, “Temporal boundaries in electromagnetic materials,” New Journal of Physics , vol. 23, no. 8, p. 083032, Aug. 2021

  12. [12]

    Photonics of time- varying media,

    E. Galiffi, R. Tirole, S. Yin, H. Li, S. Vezzoli, P. A. Huidobro, M. G. Silveirinha, R. Sapienza, A. Al `u, and J. B. Pendry, “Photonics of time- varying media,” Advanced Photonics, vol. 4, no. 01, Feb. 2022

  13. [13]

    Feature issue introduction: temporal and spatiotemporal metamaterials,

    P. A. Huidobro, M. Z. Alam, N. Engheta, and V . Pacheco-Pe˜na, “Feature issue introduction: temporal and spatiotemporal metamaterials,” Optics Express, vol. 31, no. 11, p. 18072, May 2023

  14. [14]

    Time rever- sal and holography with spacetime transformations,

    V . Bacot, M. Labousse, A. Eddi, M. Fink, and E. Fort, “Time rever- sal and holography with spacetime transformations,” Nature Physics , vol. 12, no. 10, pp. 972–977, Jul. 2016

  15. [15]

    Non-reciprocal electromagnetics in time- varying systems,

    D. L. Sounas and A. Al `u, “Non-reciprocal electromagnetics in time- varying systems,” in 2017 IEEE International Symposium on Antennas and Propagation & USNC/URSI National Radio Science Meeting . IEEE, Jul. 2017

  16. [16]

    Temporal scattering of a graphene plasmon by a rapid carrier density decrease,

    A. V . Maslov and M. I. Bakunov, “Temporal scattering of a graphene plasmon by a rapid carrier density decrease,” Optica, vol. 5, no. 12, p. 1508, Nov. 2018

  17. [17]

    Topological aspects of photonic time crystals,

    E. Lustig, Y . Sharabi, and M. Segev, “Topological aspects of photonic time crystals,” Optica, vol. 5, no. 11, p. 1390, Oct. 2018

  18. [18]

    Scattering of surface plasmons on graphene by abrupt free-carrier generation,

    A. V . Shirokova, A. V . Maslov, and M. I. Bakunov, “Scattering of surface plasmons on graphene by abrupt free-carrier generation,” Physical Review B, vol. 100, no. 4, p. 045424, Jul. 2019

  19. [19]

    Broadband frequency translation through time refraction in an epsilon-near-zero material,

    Y . Zhou, M. Z. Alam, M. Karimi, J. Upham, O. Reshef, C. Liu, A. E. Willner, and R. W. Boyd, “Broadband frequency translation through time refraction in an epsilon-near-zero material,” Nature Communications , vol. 11, no. 1, May 2020

  20. [20]

    Antireflection temporal coatings,

    V . Pacheco-Pe ˜na and N. Engheta, “Antireflection temporal coatings,” Optica, vol. 7, no. 4, p. 323, Apr. 2020

  21. [21]

    Temporal aiming,

    V . Pacheco-Pe ˜na and N. Engheta, “Temporal aiming,” Light: Science & Applications, vol. 9, no. 1, Jul. 2020

  22. [22]

    Adiabatic invariants for surface plasmons on temporally dynamic graphene,

    M. I. Bakunov, A. V . Shirokova, and A. V . Maslov, “Adiabatic invariants for surface plasmons on temporally dynamic graphene,” Journal of Optics, vol. 22, no. 9, p. 095005, Aug. 2020

  23. [23]

    Light propagation through metamaterial temporal slabs: reflection, refraction, and special cases,

    D. Ramaccia, A. Toscano, and F. Bilotti, “Light propagation through metamaterial temporal slabs: reflection, refraction, and special cases,” Optics Letters, vol. 45, no. 20, p. 5836, Oct. 2020

  24. [24]

    Temporal multilayer structures for designing higher-order transfer functions using time- varying metamaterials,

    D. Ramaccia, A. Al `u, A. Toscano, and F. Bilotti, “Temporal multilayer structures for designing higher-order transfer functions using time- varying metamaterials,” Applied Physics Letters , vol. 118, no. 10, Mar. 2021

  25. [25]

    Complete polarization conversion using anisotropic temporal slabs,

    J. Xu, W. Mai, and D. H. Werner, “Complete polarization conversion using anisotropic temporal slabs,” Optics Letters, vol. 46, no. 6, p. 1373, Mar. 2021

  26. [26]

    Disordered photonic time crystals,

    Y . Sharabi, E. Lustig, and M. Segev, “Disordered photonic time crystals,” Physical Review Letters , vol. 126, no. 16, p. 163902, Apr. 2021

  27. [27]

    Universal statistics of waves in a random time-varying medium,

    R. Carminati, H. Chen, R. Pierrat, and B. Shapiro, “Universal statistics of waves in a random time-varying medium,” Physical Review Letters , vol. 127, no. 9, p. 094101, Aug. 2021

  28. [28]

    Temporal parity-time symmetry for extreme energy transformations,

    H. Li, S. Yin, E. Galiffi, and A. Al `u, “Temporal parity-time symmetry for extreme energy transformations,” Physical Review Letters, vol. 127, no. 15, p. 153903, Oct. 2021

  29. [29]

    Nonreciprocity and faraday rotation at time interfaces,

    H. Li, S. Yin, and A. Al `u, “Nonreciprocity and faraday rotation at time interfaces,” Physical Review Letters , vol. 128, no. 17, p. 173901, Apr. 2022

  30. [30]

    Shaping the quantum vacuum with anisotropic temporal boundaries,

    J. E. V ´azquez-Lozano and I. n. Liberal, “Shaping the quantum vacuum with anisotropic temporal boundaries,” Nanophotonics, vol. 12, no. 3, pp. 539–548, Oct. 2022

  31. [31]

    Static-to- dynamic field conversion with time-varying media,

    M. J. Mencagli, D. L. Sounas, M. Fink, and N. Engheta, “Static-to- dynamic field conversion with time-varying media,” Physical Review B, vol. 105, no. 14, p. 144301, Apr. 2022. 12

  32. [32]

    Temporal interfaces by instantaneously varying boundary conditions,

    L. Stefanini, S. Yin, D. Ramaccia, A. Al `u, A. Toscano, and F. Bilotti, “Temporal interfaces by instantaneously varying boundary conditions,” Physical Review B , vol. 106, no. 9, p. 094312, Sep. 2022

  33. [33]

    Multiharmonic reso- nances of coupled time-modulated resistive metasurfaces,

    T. T. Koutserimpas and C. Valagiannopoulos, “Multiharmonic reso- nances of coupled time-modulated resistive metasurfaces,” Physical Review Applied, vol. 19, no. 6, p. 064072, Jun. 2023

  34. [34]

    Incandescent temporal meta- materials,

    J. E. V ´azquez-Lozano and I. n. Liberal, “Incandescent temporal meta- materials,” Nature Communications, vol. 14, no. 1, Aug. 2023

  35. [35]

    Nonlocal effective medium theory for phononic temporal metamaterials,

    N. Wang, F. Feng, and G. P. Wang, “Nonlocal effective medium theory for phononic temporal metamaterials,” Journal of Physics: Condensed Matter, vol. 36, no. 10, p. 105701, Dec. 2023

  36. [36]

    Time-varying media, relativity, and the arrow of time,

    M. Koivurova, C. W. Robson, and M. Ornigotti, “Time-varying media, relativity, and the arrow of time,” Optica, vol. 10, no. 10, p. 1398, Oct. 2023

  37. [37]

    Eigenpulses of dispersive time- varying media,

    S. Horsley, E. Galiffi, and Y .-T. Wang, “Eigenpulses of dispersive time- varying media,” Physical Review Letters , vol. 130, no. 20, p. 203803, May 2023

  38. [38]

    Temporal interfaces in complex electromagnetic materials: an overview [invited],

    M. H. Mostafa, M. S. Mirmoosa, M. S. Sidorenko, V . S. Asadchy, and S. A. Tretyakov, “Temporal interfaces in complex electromagnetic materials: an overview [invited],” Optical Materials Express , vol. 14, no. 5, p. 1103, Apr. 2024

  39. [39]

    Localized source above a time-modulated dielectric half-space: Green’s function theory,

    M. Kreiczer, B. Z. Steinberg, and Y . Hadad, “Localized source above a time-modulated dielectric half-space: Green’s function theory,”Physical Review Research, vol. 6, no. 1, p. 013277, Mar. 2024

  40. [40]

    Wave propagation in pure-time modu- lated step media with applications to temporal-aiming,

    M. Sini, H. Wang, and Q. Yao, “Wave propagation in pure-time modu- lated step media with applications to temporal-aiming,” Communications on Analysis and Computation , vol. 2, no. 1, pp. 48–70, 2024

  41. [41]

    Enhancing interactions among dipole excitations using surface plasmon polaritons: Quantum entanglement and classical interactions,

    J. A. Berres, “Enhancing interactions among dipole excitations using surface plasmon polaritons: Quantum entanglement and classical interactions,” Theses and Dissertations, University of Wisconsin-Milwaukee, 2024, 3554. [Online]. Available: https://dc.uwm.edu/etd/3554

  42. [42]

    Zangwill, Modern electrodynamics

    A. Zangwill, Modern electrodynamics. Cambridge: Cambridge Univer- sity Press, 2013

  43. [43]

    B. P. Lathi, Linear systems and signals , 2nd ed. New York: Oxford University Press, 2005

  44. [44]

    C. A. Balanis, Advanced engineering electromagnetics . New York [u.a.]: Wiley, 2009

  45. [45]

    Ishimaru, Electromagnetic wave propagation, radiation, and scatter- ing

    A. Ishimaru, Electromagnetic wave propagation, radiation, and scatter- ing. Englewood Cliffs, N.J.: Prentice Hall, 1991

  46. [46]

    W. C. Chew, Waves and fields in inhomogeneous media, ser. IEEE Xplore Digital Library. New York: IEEE Press, 1995

  47. [47]

    A simple model for fre- quency up-conversion in linear time-variant gaseous plasmas,

    H. Mehrpour Bernety and M. A. Cappelli, “A simple model for fre- quency up-conversion in linear time-variant gaseous plasmas,” Physics of Plasmas, vol. 31, no. 10, Oct. 2024

  48. [48]

    Enhanced laser-induced plasma channels in air,

    Y . Zuo, X. Wei, K. Zhou, X. Zeng, J. Su, Z. Jiao, N. Xie, and Z. Wu, “Enhanced laser-induced plasma channels in air,” Chinese Physics B , vol. 25, no. 3, p. 035203, Mar. 2016

  49. [49]

    Quasi-steady-state air plasma channel produced by a femtosecond laser pulse sequence,

    X. Lu, S.-Y . Chen, J.-L. Ma, L. Hou, G.-Q. Liao, J.-G. Wang, Y .-J. Han, X.-L. Liu, H. Teng, H.-N. Han, Y .-T. Li, L.-M. Chen, Z.-Y . Wei, and J. Zhang, “Quasi-steady-state air plasma channel produced by a femtosecond laser pulse sequence,” Scientific Reports, vol. 5, no. 1, Oct. 2015

  50. [50]

    Experimental study of wave propagation through a rapidly created plasma,

    S. P. Kuo and A. Ren, “Experimental study of wave propagation through a rapidly created plasma,” IEEE Transactions on Plasma Science , vol. 21, no. 1, pp. 53–56, 1993

  51. [51]

    Active magneto-plasmonics in hybrid metal- ferromagnet structures,

    V . V . Temnov, G. Armelles, U. Woggon, D. Guzatov, A. Cebollada, A. Garcia-Martin, J.-M. Garcia-Martin, T. Thomay, A. Leitenstorfer, and R. Bratschitsch, “Active magneto-plasmonics in hybrid metal- ferromagnet structures,” Nature Photonics, vol. 4, no. 2, pp. 107–111, Jan. 2010

  52. [52]

    E. J. Rothwell and M. J. Cloud, Electromagnetics, 2nd ed. CRC Press, 2010

  53. [53]

    S. A. Maier, Plasmonics: Fundamentals and applications . New York, NY: Springer, 2010

  54. [54]

    In the quest of lossless slow light at surface plasmons,

    K. Ziyatkhan, B. Orazbayev, and C. Valagiannopoulos, “In the quest of lossless slow light at surface plasmons,” Scientific Reports, vol. 14, no. 1, Nov. 2024