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arxiv: 2605.22839 · v1 · pith:JUTB3BUInew · submitted 2026-05-11 · ⚛️ physics.optics · cond-mat.mtrl-sci

Propagation Maps, Maradona Exceptional Points, and Pele Singularities in Anisotropic, Tellegen, Chiral, Moving-Medium, Omega and Other Isotropy-Broken Materials

Pith reviewed 2026-05-25 00:50 UTC · model grok-4.3

classification ⚛️ physics.optics cond-mat.mtrl-sci
keywords propagation mapsexceptional pointsisotropy-broken materialsFresnel wave surfacesnon-Hermitian mediamomentum-resolved density of stateschiral materialsanisotropic media
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The pith

In Hermitian isotropy-broken media the boundary between forward and backward propagation is a continuous locus of Maradona exceptional points where the index operator becomes defective.

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

The paper converts Fresnel wave surfaces into propagation maps for anisotropic, Tellegen, chiral, moving-medium, omega, gyrotropic, hyperbolic and multi-hyperbolic materials. These maps organize positive- and negative-phase-velocity propagation along with attenuation and amplification. In Hermitian media the boundary between forward and backward waves forms the Michelangelo silhouette separatrix. This separatrix is also a continuous locus of Maradona exceptional points where the index-of-refraction operator becomes defective even though the medium remains Hermitian. In non-Hermitian media the attenuation-amplification boundary forms the Caravaggio chiaroscuro separatrix, and Pele singularities appear where handedness stays continuous while gain-loss character reverses, causing linewidth collapse in the momentum-resolved density of states.

Core claim

Fresnel wave surfaces convert into propagation maps that organize positive- and negative-phase-velocity propagation together with attenuation and amplification across isotropy-broken materials. In Hermitian media the boundary between forward and backward propagation forms the Michelangelo silhouette separatrix, which is also a continuous locus of Maradona exceptional points where the index-of-refraction operator becomes defective even though the material medium remains Hermitian. In non-Hermitian media the attenuation-amplification boundary forms the Caravaggio chiaroscuro separatrix. The associated Pele singularities occur where handedness remains continuous while the gain-loss character is

What carries the argument

Propagation maps obtained by converting Fresnel wave surfaces, which organize phase-velocity direction, attenuation, amplification, and separate Hermitian and non-Hermitian regimes through separatrices and singularities.

If this is right

  • The separatrix in Hermitian media marks a continuous line of points where the index-of-refraction operator is defective.
  • Pele singularities produce sharp peaks in the momentum-resolved density of states whose sign reverses across the separatrix.
  • The maps supply a geometric language that organizes handedness, degeneracy, loss, gain, and momentum-resolved DOS in isotropy-broken electromagnetic materials.
  • Pele singularities act as threshold-like gain-loss singularities generated by non-Hermitian linewidth collapse.

Where Pith is reading between the lines

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

  • The same conversion procedure could be tested on additional classes of media not listed in the paper to check whether new separatrix types appear.
  • Experimental observation of linewidth collapse at Pele points would require momentum-resolved spectroscopy on a non-Hermitian anisotropic sample.
  • The framework may link to other defectiveness conditions in wave operators beyond electromagnetism.

Load-bearing premise

Fresnel wave surfaces can be systematically converted into propagation maps that correctly organize positive- and negative-phase-velocity propagation together with attenuation and amplification across the listed classes of isotropy-broken materials.

What would settle it

A direct calculation or measurement at the forward-backward boundary in a Hermitian anisotropic medium showing that the index-of-refraction operator remains non-defective rather than becoming defective.

Figures

Figures reproduced from arXiv: 2605.22839 by Maxim Durach.

Figure 1
Figure 1. Figure 1: Fresnel wave surface propagation map and constitutive-parameter decomposition. (a) A Fresnel wave surface divided into four propagation sectors according to the signs of 𝑠 and 𝜅𝑠 distinguishing PPV/NPV propagation and loss/gain behavior. The purple curve shows the OPV condition 𝒌 ⋅ 𝑺 = 0 forming the Michelangelo silhouette separatrix between PPV and NPV domains as a continuous locus of Maradona exceptional… view at source ↗
Figure 2
Figure 2. Figure 2: Michelangelo silhouette separatrices and Maradona exceptional points. (a) Bare Fresnel wave surface for the Hermitian reciprocal material 𝜖̂= diag(−2, −1,1) 𝜇̂= diag(1,2, −1) . The colored regions indicate PPV (green) and NPV (light blue) domains while the purple curves show the Michelangelo silhouette separatrices defined by 𝒌 ⋅ 𝑺 = 0. Diabolical point and Maradona EP discussed in the text are indicated b… view at source ↗
Figure 3
Figure 3. Figure 3: Caravaggio chiaroscuro separatrices and momentum-resolved density of states in a non￾Hermitian Fresnel wave surface map. (a) Momentum-resolved density of states 𝜌 in the 𝑘𝑧 = 0 cross￾section of the non-Hermitian Fresnel wave surface. The orange and dashed curves show the real and imaginary dispersion conditions Re {det ℒ̂ ′ } = 0 and Im {det ℒ̂ ′ } = 0 . Their intersections marked by numbered arrows define… view at source ↗
read the original abstract

Anisotropic, Tellegen, chiral, moving-medium-type, omega, gyrotropic, hyperbolic, and multi-hyperbolic materials form an important class of isotropy-broken photonic media in which wave propagation can no longer be characterized by the Fresnel wave surface alone. Here we show that Fresnel wave surfaces can be converted into propagation maps that organize positive- and negative-phase-velocity propagation together with attenuation and amplification. In Hermitian media, the boundary between forward and backward propagation forms the Michelangelo silhouette separatrix. This separatrix is also a continuous locus of Maradona exceptional points, where the index-of-refraction operator becomes defective even though the material medium remains Hermitian. In non-Hermitian media, the attenuation-amplification boundary forms the Caravaggio chiaroscuro separatrix. The associated Pele singularities occur where the handedness remains continuous while the gain-loss character changes sign. Their physical importance is revealed by the momentum-resolved density of states: at these points, the Lorentzian linewidth of the non-Hermitian momentum-resolved density of states (DOS) collapses, producing sharp DOS peaks whose sign reverses across the separatrix. Thus, Pele singularities are threshold-like gain-loss singularities of the Fresnel wave-surface propagation map, generated by non-Hermitian linewidth collapse. The result is a compact geometric language for describing how handedness, degeneracy, loss, gain, and momentum-resolved DOS are organized in isotropy-broken electromagnetic materials.

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

3 major / 0 minor

Summary. The manuscript claims that Fresnel wave surfaces in anisotropic, Tellegen, chiral, moving-medium, omega, gyrotropic, hyperbolic and multi-hyperbolic media can be systematically converted into propagation maps that organize forward/backward propagation, attenuation/amplification, handedness and momentum-resolved density of states. In Hermitian media the forward/backward boundary is identified as the Michelangelo silhouette separatrix, which is asserted to be a continuous locus of Maradona exceptional points at which the index-of-refraction operator is defective despite the medium remaining Hermitian. In non-Hermitian media the attenuation-amplification boundary is the Caravaggio chiaroscuro separatrix, with Pele singularities where handedness is continuous but gain-loss character reverses; these points are said to produce sharp, sign-reversing peaks in the momentum-resolved DOS via Lorentzian linewidth collapse.

Significance. If the conversion procedure and the spectral properties of the named separatrices are rigorously established, the work would supply a compact geometric language for classifying propagation features across a broad family of isotropy-broken media. The explicit linkage between separatrix geometry and momentum-resolved DOS peaks would be a concrete, falsifiable prediction with potential utility in photonic-material design. The manuscript does not, however, supply machine-checked proofs, reproducible code or parameter-free derivations that would strengthen this assessment.

major comments (3)
  1. [Abstract] Abstract: the central claim that the index-of-refraction operator becomes defective (i.e., non-diagonalizable) at Maradona exceptional points while the material medium remains Hermitian is internally inconsistent with the standard spectral theorem for Hermitian operators. The manuscript must define the index operator explicitly and demonstrate whether it is constructed to be non-normal even when the constitutive tensors are Hermitian; otherwise the defectiveness assertion cannot hold.
  2. [Abstract] Abstract: the physical importance of Pele singularities is asserted to follow from linewidth collapse in the momentum-resolved DOS, yet no derivation or explicit mapping from the Fresnel surface to the DOS is supplied. Without this step the claim that the singularities are threshold-like gain-loss features remains unsupported.
  3. [Abstract] Abstract: the Fresnel-to-propagation-map conversion is presented as systematic for all listed classes of isotropy-broken media, but the abstract gives no indication of the algebraic or geometric steps required to preserve positive/negative phase velocity together with attenuation/amplification. This conversion is load-bearing for every subsequent geometric object and must be shown to be well-defined.

Simulated Author's Rebuttal

3 responses · 0 unresolved

We thank the referee for their thorough review and insightful comments. Below we provide point-by-point responses to the major comments. We will revise the manuscript accordingly to address the concerns raised.

read point-by-point responses
  1. Referee: [Abstract] Abstract: the central claim that the index-of-refraction operator becomes defective (i.e., non-diagonalizable) at Maradona exceptional points while the material medium remains Hermitian is internally inconsistent with the standard spectral theorem for Hermitian operators. The manuscript must define the index operator explicitly and demonstrate whether it is constructed to be non-normal even when the constitutive tensors are Hermitian; otherwise the defectiveness assertion cannot hold.

    Authors: The index-of-refraction operator is not the Hermitian constitutive operator of the medium but a derived operator from the Fresnel equation that incorporates the direction-dependent wave propagation. It is non-normal due to the isotropy-breaking terms. We will add an explicit definition of this operator and a demonstration of its non-normality in the revised manuscript, clarifying that the spectral theorem applies to the constitutive tensors, not to this derived operator. revision: yes

  2. Referee: [Abstract] Abstract: the physical importance of Pele singularities is asserted to follow from linewidth collapse in the momentum-resolved DOS, yet no derivation or explicit mapping from the Fresnel surface to the DOS is supplied. Without this step the claim that the singularities are threshold-like gain-loss features remains unsupported.

    Authors: An explicit mapping from the Fresnel wave surface to the momentum-resolved DOS is provided in the main text through the resolvent of the index operator. The Lorentzian linewidth collapse at Pele singularities follows directly from this. To strengthen the presentation, we will include a dedicated derivation in an appendix of the revised manuscript. revision: yes

  3. Referee: [Abstract] Abstract: the Fresnel-to-propagation-map conversion is presented as systematic for all listed classes of isotropy-broken media, but the abstract gives no indication of the algebraic or geometric steps required to preserve positive/negative phase velocity together with attenuation/amplification. This conversion is load-bearing for every subsequent geometric object and must be shown to be well-defined.

    Authors: The algebraic and geometric steps for the Fresnel-to-propagation-map conversion are described in detail in Section 3 of the manuscript, including how phase velocity signs and attenuation are determined from the surface normals and imaginary components. We will revise the abstract to include a brief indication of these steps to make the conversion procedure more apparent from the outset. revision: partial

Circularity Check

0 steps flagged

No significant circularity; derivation presents geometric consequences of standard constitutive relations without reduction to fitted inputs or self-citation chains.

full rationale

The paper converts Fresnel wave surfaces into propagation maps for isotropy-broken media and defines separatrices (Michelangelo silhouette, Caravaggio chiaroscuro) and singularities (Maradona EPs, Pele singularities) as loci within those maps. The abstract and reader's summary give no indication that these objects are defined in terms of fitted parameters, prior self-citations, or ansatzes smuggled from the authors' own work. The central claims are presented as direct geometric consequences of the electromagnetic constitutive relations rather than statistical fits or self-referential definitions. No load-bearing step reduces by construction to its own inputs.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 2 invented entities

The central claims rest on the unproven assertion that Fresnel surfaces convert directly into the described propagation maps and that the named separatrices coincide with defective operators or linewidth collapse; no independent evidence or derivations are supplied in the abstract.

axioms (1)
  • domain assumption Fresnel wave surfaces can be converted into propagation maps that organize positive- and negative-phase-velocity propagation together with attenuation and amplification
    This conversion is the foundational step stated in the abstract.
invented entities (2)
  • Maradona exceptional points no independent evidence
    purpose: Continuous locus on the forward-backward separatrix where the index-of-refraction operator becomes defective in Hermitian media
    Newly introduced concept with no independent evidence supplied
  • Pele singularities no independent evidence
    purpose: Threshold-like gain-loss singularities where Lorentzian linewidth collapses in the momentum-resolved DOS
    Newly introduced concept with no independent evidence supplied

pith-pipeline@v0.9.0 · 5808 in / 1346 out tokens · 21747 ms · 2026-05-25T00:50:43.144818+00:00 · methodology

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Works this paper leans on

55 extracted references · 55 canonical work pages

  1. [1]

    Why Everyone Must Get Ready For The 4th Industrial Revolution ,

    Marr, Bernard, “Why Everyone Must Get Ready For The 4th Industrial Revolution ,” Forbes (2016)

  2. [2]

    R. P. Feynman, R. B. Leighton, and M. Sands, The Feynman Lectures on Physics, V ol. II, Ch. 1, California Institute of Technology, 1964

  3. [3]

    National Research Council, Optics and Photonics: Essential Technologies for Our Nation , National Academies Press, Washington, DC, 2013

  4. [4]

    Measuring the balance of the world’s largest machine,

    W. H. Baird, “Measuring the balance of the world’s largest machine,” American Journal of Physics 89, 1086–1093 (2021)

  5. [5]

    Electromagnetic metamaterials for biomedical applications: short review and trends,

    D. C. Tzarouchis, “Electromagnetic metamaterials for biomedical applications: short review and trends,” EPJ Applied Metamaterials 11, 2 (2024)

  6. [6]

    Directly wireless communication of human minds via non-invasive brain-computer-metasurface platform,

    Q. Ma, W. Gao, Q. Xiao, L. Ding, T. Gao, Y . Zhou, X. Gao, T. Yan, C. Liu, Z. Gu, X. Kong, Q. H. Abbasi, L. Li, C. -W. Qiu, Y . Li, and T. J. Cui, “Directly wireless communication of human minds via non-invasive brain-computer-metasurface platform,” eLight 2, 11 (2022)

  7. [7]

    Secure wireless communication of brain–computer interface enabled by space-time- coding digital metasurface,

    Q. Xiao, W. Gao, Q. Ma, Y . Zhou, C. Liu, Z. Gu, Z. A. Huang, X. Wan, L. Li, Y . Li, C.-W. Qiu, and T. J. Cui, “Secure wireless communication of brain–computer interface enabled by space-time- coding digital metasurface,” Nature Communications 16, 7693 (2025)

  8. [8]

    Metasurface -assisted bioelectronics: bridging photonic innovation with biomedical implants,

    M. M . Aria, S. B. Srivastava, “Metasurface -assisted bioelectronics: bridging photonic innovation with biomedical implants,” Light: Science & Applications 14, 386 (2025)

  9. [9]

    Smart radio environments empowered by reconfigurable intelligent surfaces: how it works, state of research, and the road ahead,

    M. Di Renzo, A. Zappone, M. Debbah, M.-S. Alouini, C. Yuen, J. de Rosny, and S. Tretyakov, “Smart radio environments empowered by reconfigurable intelligent surfaces: how it works, state of research, and the road ahead,” IEEE Journal on Selected Areas in Communications 38, 2450– 2525 (2020)

  10. [10]

    Coding metamaterials, digital metamaterials and programmable metamaterials,

    T. J. Cui, M. Q. Qi, X. Wan, J. Zhao, and Q. Cheng, “Coding metamaterials, digital metamaterials and programmable metamaterials,” Light: Science & Applications 3, e218 (2014)

  11. [11]

    Flexible Metamaterial Wrap for Improved Head Imaging at 3 T MRI With Low-Cost and Easy Fabrication Method ,

    S. L. Sokol, et al, “Flexible Metamaterial Wrap for Improved Head Imaging at 3 T MRI With Low-Cost and Easy Fabrication Method ,” IEEE Antennas and Wireless Propagation Letters 21, 2075–2079 (2022)

  12. [12]

    Electromagnetic brain–computer–metasurface holography,

    Q. Xiao, W. Gao, Q. Ma, Z. Gu, Y . Zhou, C. Liu, Z. A. Huang, X. Wan, L. Li, Y . Li, and T. J. Cui, “Electromagnetic brain–computer–metasurface holography,” ACS Photonics 10, 2249–2256 (2023)

  13. [13]

    Metasurfaces for quantitative biosciences of molecules, cells, and tissues: sensing and diagnostics,

    A. Barulin, D. D. Nguyen, Y . Kim, C. Ko, and I. Kim, “Metasurfaces for quantitative biosciences of molecules, cells, and tissues: sensing and diagnostics,” ACS Photonics 11, 904–916 (2024). -21-

  14. [14]

    Plasmonic metamaterials for nanochemistry and sensing,

    P. Wang, M. E. Nasir, A. V . Krasavin, W. Dickson, Y . Jiang, and A. V . Zayats, “Plasmonic metamaterials for nanochemistry and sensing,” Accounts of Chemical Research 52, 3018–3028 (2019)

  15. [15]

    Metasurfaces for sensing applications: gas, bio and chemical,

    S. Tabassum, S. K. Nayemuzzaman, M. Kala, A. K. Mishra, and S. K. Mishra, “Metasurfaces for sensing applications: gas, bio and chemical,” Sensors 22, 6896 (2022)

  16. [16]

    Thermal camouflage based on the phase - changing material GST,

    Y . Qu, Q. Li, K. Du, L. Cai, J. Lu, and M. Qiu, “Thermal camouflage based on the phase - changing material GST,” Light: Science & Applications 7, 26 (2018)

  17. [17]

    United Nations General Assembly, Transforming Our World: The 2030 Agenda for Sustainable Development, Resolution A/RES/70/1, United Nations, New York, 2015

  18. [18]

    J. A. Kong, Electromagnetic Wave Theory, EMW Publishing, Cambridge, MA, 2008

  19. [19]

    F. W. Hehl and Y . N. Obukhov, Foundations of Classical Electrodynamics: Charge Flux and Metric, Birkhäuser, Boston, 2003

  20. [20]

    Lakhtakia, Beltrami Fields in Chiral Media, World Scientific, Singapore, 1994

    A. Lakhtakia, Beltrami Fields in Chiral Media, World Scientific, Singapore, 1994

  21. [21]

    I. V . Lindell, A. H. Sihvola, S. A. Tretyakov, and A. J. Viitanen, Electromagnetic Waves in Chiral and Bi-Isotropic Media, Artech House, Boston, 1994

  22. [22]

    Serdyukov, I

    A. Serdyukov, I. Semchenko, S. Tretyakov, and A. Sihvola, Electromagnetics of Bi - Anisotropic Materials: Theory and Applications, Gordon and Breach, Amsterdam, 2001

  23. [23]

    T. G. Mackay and A. Lakhtakia, Electromagnetic Anisotropy and Bianisotropy: A Field Guide, 2nd ed., World Scientific, Singapore, 2019

  24. [24]

    Eroglu, Wave Propagation and Radiation in Gyrotropic and Anisotropic Media, Springer, New York, 2010

    A. Eroglu, Wave Propagation and Radiation in Gyrotropic and Anisotropic Media, Springer, New York, 2010

  25. [25]

    Hyperbolic metamaterials,

    A. Poddubny, I. Iorsh, P. Belov, and Y . Kivshar, “Hyperbolic metamaterials,” Nature Photonics 7, 948–957 (2013)

  26. [26]

    Tri- and tetrahyperbolic isofrequency topologies complete classifications of bianisotropic materials,

    M. Durach, R. Williamson, M. Laballe, and T. Mulkey, “Tri- and tetrahyperbolic isofrequency topologies complete classifications of bianisotropic materials,” Applied Sciences 10, 763 (2020)

  27. [27]

    Dispersion peculiarities of hybrid modes in a circular waveguide filled by a composite gyroelectromagnetic medium,

    V . R. Tuz, V . I. Fesenko, I. V . Fedorin, H.-B. Sun, V . M. Shulga, and W. Han, “Dispersion peculiarities of hybrid modes in a circular waveguide filled by a composite gyroelectromagnetic medium,” Journal of Electromagnetic Waves and Applications 31, 140–154 (2017)

  28. [28]

    Magnet -free nonreciprocal bianisotropic metasurfaces,

    Y . Ra’di and A. Grbic, “Magnet -free nonreciprocal bianisotropic metasurfaces,” Physical Review B 94, 195432 (2016)

  29. [29]

    Electromagnetic wave scattering from a moving medium with stationary interfaces,

    Z.-L. Deck-Léger, X. Zheng, and C. Caloz, “Electromagnetic wave scattering from a moving medium with stationary interfaces,” Photonics 8, 202 (2021). -22-

  30. [30]

    Optical Tellegen metamaterial with spontaneous magnetization,

    S. S. Jazi, et al, “Optical Tellegen metamaterial with spontaneous magnetization,” Nature Communications 15, 1854 (2024)

  31. [31]

    Gigantic Tellegen responses in metamaterials,

    Q. Yang, X. Wen, Z. Li, O. You, and S. Zhang, “Gigantic Tellegen responses in metamaterials,” Nature Communications 16, 151 (2025)

  32. [32]

    Non -Hermitian photonics based on parity –time symmetry,

    L. Feng, R. El -Ganainy, and L. Ge, “Non -Hermitian photonics based on parity –time symmetry,” Nature Photonics 11, 752–762 (2017)

  33. [33]

    The dawn of non -Hermitian optics,

    R. El -Ganainy, M. Khajavikhan, and L. Ge, “The dawn of non -Hermitian optics,” Communications Physics 2, 37 (2019)

  34. [34]

    Lossless and loss-induced topological transitions of isofrequency surfaces in a biaxial gyroelectromagnetic medium,

    V . I. Fesenko and V . R. Tuz, “Lossless and loss-induced topological transitions of isofrequency surfaces in a biaxial gyroelectromagnetic medium,” Physical Review B 99, 094404 (2019)

  35. [35]

    Beyond Fresnel wave surfaces: theory of off-shell photonic density of states and near-fields in isotropy-broken materials with loss or gain,

    M. Durach and D. Keene, “Beyond Fresnel wave surfaces: theory of off-shell photonic density of states and near-fields in isotropy-broken materials with loss or gain,” Photonics 12, 1032 (2025)

  36. [36]

    The Fresnel wave surface,

    H. Knörrer, “The Fresnel wave surface,” in Geometry of Surfaces , Lecture Notes in Mathematics 1062, 127–132, Springer, Berlin, 1984

  37. [37]

    Line degeneracy and strong spin -orbit coupling of light with bulk bianisotropic metamaterials,

    Q. Guo, W. Gao, J. Chen, Y . Liu, and S. Zhang, “Line degeneracy and strong spin -orbit coupling of light with bulk bianisotropic metamaterials,” Physical Review Letters 115, 067402 (2015)

  38. [38]

    Light propagation in local and linear media: Fresnel -Kummer wave surfaces with 16 singular points,

    A. Favaro and F. W. Hehl, “Light propagation in local and linear media: Fresnel -Kummer wave surfaces with 16 singular points,” Physical Review A 93, 013844 (2016)

  39. [39]

    The optical singularities of bianisotropic crystals,

    M. V . Berry, “The optical singularities of bianisotropic crystals,” Proceedings of the Royal Society A: Mathematical Physical and Engineering Sciences 461, 2071–2098 (2005)

  40. [40]

    Exceptional points in optics and photonics,

    M.-A. Miri and A. Alù, “Exceptional points in optics and photonics,” Science 363, eaar7709 (2019)

  41. [41]

    Parity–time symmetry and exceptional points in photonics,

    Ş. K. Özdemir, S. Rotter, F. Nori, and L. Yang, “Parity–time symmetry and exceptional points in photonics,” Nature Materials 18, 783–798 (2019)

  42. [42]

    Exceptional topology of non -Hermitian systems,

    E. J. Bergholtz, J. C. Budich, and F. K. Kunst, “Exceptional topology of non -Hermitian systems,” Reviews of Modern Physics 93, 015005 (2021)

  43. [43]

    Positive -, negative-, and orthogonal -phase- velocity propagation of electromagnetic plane waves in a simply moving medium,

    T. G. Mackay, A. Lakhtakia, and S. Setiawan, “Positive -, negative-, and orthogonal -phase- velocity propagation of electromagnetic plane waves in a simply moving medium,” Optik 118, 195–202 (2007)

  44. [44]

    L. D. Landau and E. M. Lifshitz, Electrodynamics of Continuous Media, 2nd ed., Pergamon Press, Oxford, 1984. -23-

  45. [45]

    Robin Wilson, Four Colors Suffice: How the Map Problem Was Solved, (Princeton University Press, 2002)

  46. [46]

    (Penguin, 2003)

    Ross King, Michelangelo and the Pope’ s Ceiling. (Penguin, 2003)

  47. [47]

    The Hand of God, the Hand of the Devil: a sociological interpretation of Maradona’s hand goal ,

    Simone Magalhães Britto, Jorge V entura de Morais and Túlio V elho Barreto, “The Hand of God, the Hand of the Devil: a sociological interpretation of Maradona’s hand goal ,” in Legacies of Great Men in World Soccer, Heroes, Icons, Legends (Routledge, London, 2016)

  48. [48]

    Caravaggio and Tenebrism —Beauty of light and shadow in baroque paintings ,

    H. Xu, “ Caravaggio and Tenebrism —Beauty of light and shadow in baroque paintings ,” Journal of Arts and Humanities 9(6), pp. 1–11 (2020)

  49. [49]

    Pelé Gives Uruguay the Runaround,

    FIFA, “Pelé Gives Uruguay the Runaround,” FIF A (2016). https://inside.fifa.com/news/pele- gives-uruguay-the-runaround-2764887

  50. [50]

    The optical singularities of bianisotropic crystals,

    M. V . Berry, “The optical singularities of bianisotropic crystals,” Proc. R. Soc. A 461, 2071– 2098, 2005

  51. [51]

    Beyond Green’s Functions: Inverse Helmholtz and ‘Om’ ॐ-Potential Methods for Macroscopic Electromagnetism in Isotropy-Broken Media,

    M. Durach, “Beyond Green’s Functions: Inverse Helmholtz and ‘Om’ ॐ-Potential Methods for Macroscopic Electromagnetism in Isotropy-Broken Media,” Photonics 12(7), 660, 2025

  52. [52]

    M. Durach, “Tetra-hyperbolic and tri-hyperbolic optical phases in anisotropic metamaterials without magnetoelectric coupling due to hybridization of plasmonic and magnetic Bloch high -𝑘 polaritons,” Optics Communications 476, 126349 (2020)

  53. [53]

    On the anatomy of V oigt plane waves,

    T. G. Mackay and A. Lakhtakia, “On the anatomy of V oigt plane waves,” in Adventures in Contemporary Electromagnetic Theory, pp. 61–91 (Springer, 2023)

  54. [54]

    Inverse problem of quartic photonics,

    T. Mulkey, J. Dillies, and M. Durach, “Inverse problem of quartic photonics,” Optics Letters 43, 1226–1229, (2018)

  55. [55]

    -Y .; Park, H.-C.; Ryu, J

    Park, J.; Lee, K.; Zhang, R. -Y .; Park, H.-C.; Ryu, J. -W.; Cho, G.Y .; Lee, M.Y .; Zhang, Z.; Park, N.; Jeon, W.; et al. Spontaneous emission decay and excitation in photonic time crystals. Phys. Rev. Lett., 135, 133801 (2025)