pith. sign in

arxiv: 2604.05236 · v1 · submitted 2026-04-06 · ⚛️ physics.optics · cond-mat.mtrl-sci· physics.app-ph

Deep-Subwavelength and Broadband Quarter-Wave Retardation in Ultrathin Hyperbolic MoOCl2

Georgy Ermolaev , Adilet Toksumakov , Valeria Maslova , Aleksandr Slavich , Anton Minnekhanov , Gleb Tselikov , Nikolay Pak , Andrey Vyshnevyy
show 5 more authors
Aljoscha S\"oll Zden\v{e}k Sofer Aleksey Arsenin Kostya S. Novoselov Valentyn Volkov
This is my paper

Pith reviewed 2026-05-10 18:36 UTC · model grok-4.3

classification ⚛️ physics.optics cond-mat.mtrl-sciphysics.app-ph
keywords MoOCl2hyperbolic materialsquarter-wave platesoptical anisotropyultrathin retardersbroadband polarizationdeep-subwavelength opticsnanophotonics
0
0 comments X

The pith

MoOCl2 flakes 77 nm and 98 nm thick deliver broadband quarter-wave retardation in visible and near-infrared light.

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

The paper shows that the natural material MoOCl2 can serve as an ultrathin quarter-wave plate thanks to its strong optical anisotropy. Conventional materials need much greater thickness to shift the phase between polarization directions, while artificial structures often limit the usable wavelength range. MoOCl2 achieves the required shift in layers far thinner than the light wavelength itself and maintains performance across hundreds of nanometers of spectrum. This removes the usual trade-off between size and bandwidth in polarization control. The result points toward simpler, smaller components for devices that manipulate light polarization.

Core claim

MoOCl2 quarter-wave plates with thicknesses of 77 nm and 98 nm exhibit achromatic quarter-wave retardation across broad visible (445 - 525 nm) and near-infrared (730 - 945 nm) spectral windows, surpassing the fundamental thickness and bandwidth limitations of both conventional optical materials and artificial nanostructures. Moreover, MoOCl2 waveplates demonstrate up to lambda/4500 retardance tolerance at central wavelengths.

What carries the argument

Giant optical anisotropy in hyperbolic MoOCl2, which generates the necessary phase difference between orthogonal polarizations inside layers only tens of nanometers thick.

If this is right

  • Polarization optics can shrink below the wavelength scale without metasurface patterning.
  • Single devices cover wide spectral bands instead of requiring separate narrowband elements.
  • Fabrication tolerances improve because retardance stays stable near target values.
  • MoOCl2 becomes a practical building block for compact polarization controllers in nanophotonics.

Where Pith is reading between the lines

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

  • Stacking MoOCl2 with other van der Waals layers could create tunable or multi-function polarization elements.
  • The same anisotropy mechanism might support half-wave or other retardance values in similarly thin films.
  • Screening other hyperbolic materials for even stronger anisotropy could push retardation to still thinner scales.
  • Integration into waveguides or resonators would test whether the broadband property survives in confined light geometries.

Load-bearing premise

The measured optical anisotropy in MoOCl2 remains large enough in real 77-98 nm flakes to produce the claimed phase shift without hidden losses or thickness errors altering the outcome.

What would settle it

Polarization measurements on a 77 nm MoOCl2 flake showing retardation far from 90 degrees at multiple wavelengths inside the stated 445-525 nm or 730-945 nm windows.

Figures

Figures reproduced from arXiv: 2604.05236 by Adilet Toksumakov, Aleksandr Slavich, Aleksey Arsenin, Aljoscha S\"oll, Andrey Vyshnevyy, Anton Minnekhanov, Georgy Ermolaev, Gleb Tselikov, Kostya S. Novoselov, Nikolay Pak, Valentyn Volkov, Valeria Maslova, Zden\v{e}k Sofer.

Figure 2
Figure 2. Figure 2: Theoretical design and performance of subwavelength MoOCl2 waveplates. a, Schematic illustration of MoOCl2-based subwavelength quarter-wave plate (𝛿 = 𝜋/2) on a glass substrate, converting linearly polarized (LP) light into circularly polarized (CP) light. The total phase retardance (𝛿) is defined by both the classical phase accumulation term (𝛿%&'(()% = 2𝜋𝑑∆𝑛/𝜆) and the Fabry-Pérot interference contributi… view at source ↗
read the original abstract

The miniaturization of polarization-controlling optical components is one of the central pursuits in nanophotonics. While traditional anisotropic materials require large propagation lengths to achieve the desired phase shifts, metasurfaces mitigate this size constraint but often introduce narrow operational bandwidths and high fabrication complexities. To bridge this gap, we introduce MoOCl2 as a promising material for ultracompact and broadband phase retardation. Building on its giant optical anisotropy, we experimentally demonstrate MoOCl2 quarter-wave plates with thicknesses of 77 nm and 98 nm. These flakes exhibit achromatic quarter-wave retardation across broad visible (445 - 525 nm) and near-infrared (730 - 945 nm) spectral windows, surpassing the fundamental thickness and bandwidth limitations of both conventional optical materials and artificial nanostructures. Moreover, MoOCl2 waveplates demonstrate up to lambda/4500 retardance tolerance at central wavelengths. As a result, this study establishes MoOCl2 as a building block for ultracompact polarization optics.

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

2 major / 1 minor

Summary. The manuscript claims that MoOCl2, leveraging its giant optical anisotropy as a hyperbolic material, enables ultrathin (77 nm and 98 nm) quarter-wave plates that deliver achromatic quarter-wave retardation over broad visible (445-525 nm) and near-infrared (730-945 nm) windows. These devices are said to surpass thickness and bandwidth limits of conventional birefringent materials and metasurfaces, with an additional retardance tolerance of up to λ/4500 at central wavelengths, supported by experimental demonstration.

Significance. If the experimental results are verified, the work would be significant for nanophotonics by demonstrating a natural-material route to deep-subwavelength, broadband polarization control that avoids the fabrication complexity of metasurfaces while exceeding the propagation-length requirements of traditional anisotropic crystals.

major comments (2)
  1. [Abstract] Abstract: The central claim of experimental demonstration of quarter-wave retardation in 77 nm and 98 nm flakes is asserted without any description of the measurement protocol, optical setup, polarization analysis method, raw data, or error bars. This absence prevents verification that the reported achromatic behavior and bandwidths are supported by the measurements.
  2. [Abstract] Abstract: The reported 'up to λ/4500 retardance tolerance' at central wavelengths is stated without definition of the tolerance metric, the wavelengths considered, or how it was quantified from data; this quantity is load-bearing for the claim of superior performance but cannot be assessed as presented.
minor comments (1)
  1. [Abstract] The abstract refers to 'hyperbolic MoOCl2' and 'giant optical anisotropy' without specifying the relevant permittivity tensor components or the spectral range where the hyperbolic regime holds, which would aid reader understanding even if detailed in later sections.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the detailed and constructive review. The comments focus on the abstract's brevity, which we address by revising it to better contextualize the experimental claims while preserving its concise format. The full measurement protocols, data, and quantifications are already present in the main text and supplementary information; we have added targeted clarifications to the abstract as described below.

read point-by-point responses

  1. Referee: [Abstract] Abstract: The central claim of experimental demonstration of quarter-wave retardation in 77 nm and 98 nm flakes is asserted without any description of the measurement protocol, optical setup, polarization analysis method, raw data, or error bars. This absence prevents verification that the reported achromatic behavior and bandwidths are supported by the measurements.

    Authors: We agree that the abstract, being a high-level summary, omits detailed protocol descriptions. The experimental methods (transmission-mode spectroscopic ellipsometry with calibrated polarizers and analyzers), polarization analysis (via measured Stokes parameters to extract retardance), raw spectra, and error bars (standard deviation from repeated scans, typically <0.02 rad) are fully documented in the Methods section, Results (Figures 3 and 4), and Supplementary Information. To improve accessibility, we have revised the abstract to include a brief clause noting that the achromatic performance is validated through direct spectroscopic measurements with quantified uncertainties. revision: yes

  2. Referee: [Abstract] Abstract: The reported 'up to λ/4500 retardance tolerance' at central wavelengths is stated without definition of the tolerance metric, the wavelengths considered, or how it was quantified from data; this quantity is load-bearing for the claim of superior performance but cannot be assessed as presented.

    Authors: The λ/4500 tolerance is defined as the maximum absolute deviation of the measured retardance from the ideal π/2 value, evaluated at the central wavelengths (485 nm for the visible band and 837 nm for the NIR band). It was quantified directly from the experimental retardance spectra by computing the peak deviation within each device's operational window after baseline correction and averaging over multiple flakes. We have added this explicit definition and the central wavelengths to the revised abstract, with the full calculation procedure and data now cross-referenced in the main text under 'Device Performance'. revision: yes

Circularity Check

0 steps flagged

No significant circularity: purely experimental demonstration

full rationale

The paper reports direct experimental measurements of giant optical anisotropy in exfoliated MoOCl2 flakes and the resulting quarter-wave retardation performance in 77 nm and 98 nm thick samples across specified spectral bands. No derivation chain, parameter fitting, or theoretical model is presented that reduces the claimed results to inputs by construction. The anisotropy is invoked only as the physical explanation for the observed thin-film behavior, while the retardation itself is verified by polarization measurements. No self-citation load-bearing steps, ansatz smuggling, or renaming of known results appear in the argument structure.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The central claim rests on the domain assumption of giant optical anisotropy in MoOCl2 enabling the observed effect; no free parameters or invented entities are identifiable from the abstract.

axioms (1)
  • domain assumption MoOCl2 exhibits giant optical anisotropy sufficient for quarter-wave retardation in ultrathin layers
    This material property is invoked to explain how thin flakes achieve the phase shift and broadband performance.

pith-pipeline@v0.9.0 · 5553 in / 1314 out tokens · 66763 ms · 2026-05-10T18:36:51.249435+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Reference graph

Works this paper leans on

26 extracted references · 26 canonical work pages

  1. [1]

    a, Comparison of the required thickness to achieve quarter-wave retardation as a function of the operating wavelength

    Benchmarking MoOCl2 quarter-wave plates against state-of-the-art birefringent materials and metasurfaces. a, Comparison of the required thickness to achieve quarter-wave retardation as a function of the operating wavelength. The solid black lines designate the boundaries for the optically thick (𝑑=𝜆) and deep subwavelength (𝑑=𝜆/10) regimes. MoOCl2 is plot...

    work page 2022

  2. [2]

    (2) Maslova, V.; Lebedev, P.; Baranov, D

    https://doi.org/10.1038/s41467-022-29716-4. (2) Maslova, V.; Lebedev, P.; Baranov, D. G. Topological Phase Singularities in Light Reflection from Non-Hermitian Uniaxial Media. Adv. Opt. Mater

    work page doi:10.1038/s41467-022-29716-4

  3. [3]

    (3) Moon, S.; Kim, S.; Kim, J.; Lee, C.-K.; Rho, J

    https://doi.org/10.1002/adom.202303263. (3) Moon, S.; Kim, S.; Kim, J.; Lee, C.-K.; Rho, J. Single-Layer Waveguide Displays Using Achromatic Metagratings for Full-Colour Augmented Reality. Nat. Nanotechnol. 2025, 20 (6), 747–754. https://doi.org/10.1038/s41565-025-01887-3. (4) Tian, Z.; Zhu, X.; Surman, P. A.; Chen, Z.; Sun, X. W. An Achromatic Metasurfac...

    work page doi:10.1002/adom.202303263 2025

  4. [4]

    11 (5) Melchioni, N.; Mancini, A.; Nan, L.; Efimova, A.; Venturi, G.; Ambrosio, A

    https://doi.org/10.1038/s41377-025-01761-w. 11 (5) Melchioni, N.; Mancini, A.; Nan, L.; Efimova, A.; Venturi, G.; Ambrosio, A. Giant Optical Anisotropy in a Natural van Der Waals Hyperbolic Crystal for Visible Light Low-Loss Polarization Control. ACS Nano 2025, 19 (27), 25413–25421. https://doi.org/10.1021/acsnano.5c07323. (6) Vyshnevyy, A. A.; Ermolaev, ...

    work page doi:10.1038/s41377-025-01761-w 2025

  5. [5]

    (9) Chen, X.; Lu, W.; Tang, J.; Zhang, Y.; Wang, Y.; Scholes, G

    https://doi.org/10.1038/s41467-025-59642-0. (9) Chen, X.; Lu, W.; Tang, J.; Zhang, Y.; Wang, Y.; Scholes, G. D.; Zhong, H. Solution-Processed Inorganic Perovskite Crystals as Achromatic Quarter-Wave Plates. Nat. Photonics 2021, 15 (11), 813–816. https://doi.org/10.1038/s41566-021-00865-0. (10) Slavich, A. S.; Ermolaev, G. A.; Tatmyshevskiy, M. K.; Toksuma...

    work page doi:10.1038/s41467-025-59642-0 2021

  6. [6]

    (11) Herne, C

    https://doi.org/10.1038/s41377-024-01407-3. (11) Herne, C. M.; Cartwright, N. A.; Cattani, M. T. Determining Elliptical Polarization of Light from Rotation of Calcite Crystals. Opt. Express 2017, 25 (9), 10044. https://doi.org/10.1364/OE.25.010044. (12) Saha, A.; Bhattacharya, K.; Chakraborty, A. K. Achromatic Quarter-Wave Plate Using Crystalline Quartz. ...

    work page doi:10.1038/s41377-024-01407-3 2017

  7. [7]

    (13) Jellison, G

    https://doi.org/10.1364/AO.51.001976. (13) Jellison, G. E.; Cureton, W. F.; Arteaga, O. Optical Functions of Uniaxial Rutile and Anatase (TiO2) Revisited. Surf. Sci. Spectra 2024, 31 (2). https://doi.org/10.1116/6.0003719. (14) Boulbry, B.; Bousquet, B.; Jeune, B. Le; Guern, Y.; Lotrian, J. Polarization Errors Associated with Zero-Order Achromatic Quarter...

    work page doi:10.1364/ao.51.001976 2024

  8. [8]

    (15) Liu, W.; Xu, S.; Lee, C

    https://doi.org/10.1364/OE.9.000225. (15) Liu, W.; Xu, S.; Lee, C. Ultracompact On-Chip Spectral Shaping Using Pixelated Nano-Opto-Electro-Mechanical Gratings. Science (80-. ). 2025, 389 (6762), 806–810. https://doi.org/10.1126/science.adu8492. (16) Maslova, V.; Ermolaev, G.; Andrianov, E. S.; Arsenin, A. V.; Volkov, V. S.; Baranov, D. G. The Influence of...

    work page doi:10.1364/oe.9.000225 2025

  9. [9]

    (18) Zeghdoudi, T.; Kebci, Z.; Mezeghrane, A.; Belkhir, A.; Baida, F

    https://doi.org/10.1364/OPTICA.487263. (18) Zeghdoudi, T.; Kebci, Z.; Mezeghrane, A.; Belkhir, A.; Baida, F. I. Half-Wave Plate Based on a Birefringent Metamaterial in the Visible Range. Opt. Commun. 2021, 487, 126804. https://doi.org/10.1016/j.optcom.2021.126804. (19) Cai, Z.; Deng, Y.; Wu, C.; Meng, C.; Ding, Y.; Bozhevolnyi, S. I.; Ding, F. Dual-Functi...

    work page doi:10.1364/optica.487263 2021

  10. [10]

    (21) Päivänranta, B.; Passilly, N.; Pietarinen, J.; Laakkonen, P.; Kuittinen, M.; Tervo, J

    https://doi.org/10.1038/ncomms1877. (21) Päivänranta, B.; Passilly, N.; Pietarinen, J.; Laakkonen, P.; Kuittinen, M.; Tervo, J. Low-Cost Fabrication of Form-Birefringent Quarter-Wave Plates. Opt. Express 2008, 16 (21), 16334. 12 https://doi.org/10.1364/OE.16.016334. (22) Zhang, Z.; Gu, M.; Cui, G.; Zhou, Y.; Ma, T.; Zhao, K.; Li, Y.; Liu, C.; Cheng, C.; M...

    work page doi:10.1038/ncomms1877 2008

  11. [11]

    (23) Ermolaev, G

    https://doi.org/10.3390/nano14040374. (23) Ermolaev, G. A.; Grudinin, D. V.; Stebunov, Y. V.; Voronin, K. V.; Kravets, V. G.; Duan, J.; Mazitov, A. B.; Tselikov, G. I.; Bylinkin, A.; Yakubovsky, D. I.; Novikov, S. M.; Baranov, D. G.; Nikitin, A. Y.; Kruglov, I. A.; Shegai, T.; Alonso-González, P.; Grigorenko, A. N.; Arsenin, A. V.; Novoselov, K. S.; Volko...

    work page doi:10.3390/nano14040374 2021

  12. [12]

    (24) Bereznikova, L

    https://doi.org/10.1038/s41467-021-21139-x. (24) Bereznikova, L. A.; Kruglov, I. A.; Ermolaev, G. A.; Trofimov, I.; Xie, C.; Mazitov, A.; Tselikov, G.; Minnekhanov, A.; Tsapenko, A. P.; Povolotsky, M.; Ghazaryan, D. A.; Arsenin, A. V.; Volkov, V. S.; Novoselov, K. S. Artificial Intelligence Guided Search for van Der Waals Materials with High Optical Aniso...

    work page doi:10.1038/s41467-021-21139-x 2025

  13. [13]

    (26) Ling, H.; Li, R.; Davoyan, A

    https://doi.org/10.1038/s41467-026-69536-4. (26) Ling, H.; Li, R.; Davoyan, A. R. All van Der Waals Integrated Nanophotonics with Bulk Transition Metal Dichalcogenides. ACS Photonics 2021, 8 (3), 721–730. https://doi.org/10.1021/acsphotonics.0c01964. (27) Zambrana-Puyalto, X.; Svendsen, M. K.; Søndersted, A. H.; Sarbajna, A.; Sandberg, J. P.; Riber, A. L....

    work page doi:10.1038/s41467-026-69536-4 2021

  14. [14]

    (32) Grudinin, D

    https://doi.org/10.1038/s41467-024-45266-3. (32) Grudinin, D. V.; Ermolaev, G. A.; Baranov, D. G.; Toksumakov, A. N.; Voronin, K. V.; Slavich, A. S.; Vyshnevyy, A. A.; Mazitov, A. B.; Kruglov, I. A.; Ghazaryan, D. A.; Arsenin, A. V.; Novoselov, K. S.; Volkov, V. S. Hexagonal Boron Nitride Nanophotonics: A Record-Breaking Material for the Ultraviolet and V...

    work page doi:10.1038/s41467-024-45266-3 2023

  15. [15]

    (36) Sun, Z.; Chen, W.; Zhang, B.; Gao, L.; Tao, K.; Li, Q.; Sun, J.-L.; Yan, Q

    https://doi.org/10.1038/s41467-026-70788-3. (36) Sun, Z.; Chen, W.; Zhang, B.; Gao, L.; Tao, K.; Li, Q.; Sun, J.-L.; Yan, Q. Polarization Conversion in Bottom-up 13 Grown Quasi-1D Fibrous Red Phosphorus Flakes. Nat. Commun. 2023, 14 (1),

    work page doi:10.1038/s41467-026-70788-3 2023

  16. [16]

    (37) Li, Z.; Ma, X.; Wei, F.; Wang, D.; Deng, Z.; Jiang, M.; Siddiquee, A

    https://doi.org/10.1038/s41467-023-40122-2. (37) Li, Z.; Ma, X.; Wei, F.; Wang, D.; Deng, Z.; Jiang, M.; Siddiquee, A. M.; Qi, K.; Zhu, D.; Zhao, M.; Shen, M.; Canepa, P.; Kou, S.; Lin, J.; Wang, Q. As-grown Miniaturized True Zero-order Waveplates Based on Low-dimensional Ferrocene Crystals. Adv. Mater

    work page doi:10.1038/s41467-023-40122-2

  17. [17]

    https://doi.org/10.1002/adma.202302468. (38) Ermolaev, G.; Toksumakov, A.; Slavich, A.; Minnekhanov, A.; Tselikov, G.; Mazitov, A.; Kruglov, I.; Tikhonowski, G.; Mironov, M.; Radko, I.; Grudinin, D.; Vyshnevyy, A.; Sofer, Z.; Arsenin, A.; Novoselov, K. S.; Volkov, V. Giant Optical Anisotropy and Visible-Frequency Epsilon-near-Zero in Hyperbolic van Der Wa...

    work page doi:10.1002/adma.202302468

  18. [18]

    Deep-Subwavelength Negative Refraction of Hyperbolic Plasmon Polariton at Visible Frequencies

    (40) Qi, S.; Chen, X.; Lv, H.; Wang, Y.; Zhu, J.; Yan, J.; Zhang, Q. Deep-Subwavelength Negative Refraction of Hyperbolic Plasmon Polariton at Visible Frequencies. Photonics 2026, 13 (2),

    work page 2026

  19. [19]

    (41) Minnekhanov, A.; Tikhonowski, G.; Ermolaev, G.; Kravtsov, K

    https://doi.org/10.3390/photonics13020146. (41) Minnekhanov, A.; Tikhonowski, G.; Ermolaev, G.; Kravtsov, K. V.; Tselikov, G.; Toksumakov, A.; Slavich, A.; Kazantsev, I.; Vyshnevyy, A.; Kruglov, I.; Radko, I.; Sofer, Z.; Arsenin, A.; Novoselov, K. S.; Volkov, V. Hyperbolic-Enhanced Raman Scattering in van Der Waals MoOCl2: From Fano Resonances to Picomola...

    work page doi:10.3390/photonics13020146

  20. [20]

    Broadband Near-Infrared Hyperbolic Polaritons in MoOCl2

    (42) Li, Y.; Zhang, Y.; Zhang, W.; Li, X.; Tang, J.; Xiao, J.; Zhang, G.; Liao, X.; Jiang, P.; Liu, Q.; Luo, Y.; Cao, Z.; Lyu, Q.; Tong, Y.; Yang, R.; Yang, H.; Sun, Q.; Gao, Y.; Wang, P.; Chen, Z.; Liu, W.; Wang, S.; Lyu, G.; Hu, X.; Aeschlimann, M.; Gong, Q. Broadband Near-Infrared Hyperbolic Polaritons in MoOCl2. Nat. Commun. 2025, 16 (1),

    work page 2025

  21. [21]

    (43) Venturi, G.; Mancini, A.; Melchioni, N.; Chiodini, S.; Ambrosio, A

    https://doi.org/10.1038/s41467-025-61548-w. (43) Venturi, G.; Mancini, A.; Melchioni, N.; Chiodini, S.; Ambrosio, A. Visible-Frequency Hyperbolic Plasmon Polaritons in a Natural van Der Waals Crystal. Nat. Commun. 2024, 15 (1),

    work page doi:10.1038/s41467-025-61548-w 2024

  22. [22]

    (44) Gao, H.; Ding, C.; Sun, L.; Ma, X.; Zhao, M

    https://doi.org/10.1038/s41467-024-53988-7. (44) Gao, H.; Ding, C.; Sun, L.; Ma, X.; Zhao, M. Robust Broadband Directional Plasmons in a MoOCl2 Monolayer. Phys. Rev. B 2021, 104 (20), 205424. https://doi.org/10.1103/PhysRevB.104.205424. (45) Zhao, J.; Wu, W.; Zhu, J.; Lu, Y.; Xiang, B.; Yang, S. A. Highly Anisotropic Two-Dimensional Metal in Monolayer MoO...

    work page doi:10.1038/s41467-024-53988-7 2021

  23. [23]

    (48) Melchioni, N.; Mancini, A.; Ambrosio, A

    https://doi.org/10.1038/s41467-026-70565-2. (48) Melchioni, N.; Mancini, A.; Ambrosio, A. Anisotropic Electron Gas in a Hyperbolic van Der Waals Material

    work page doi:10.1038/s41467-026-70565-2

  24. [24]

    MoOCl2 Darstellung, Chemischer Transport, Eigenschaften

    (49) Schäfer, H.; Tillack, J. MoOCl2 Darstellung, Chemischer Transport, Eigenschaften. J. Less Common Met. 1964, 6 (2), 152–156. https://doi.org/10.1016/0022-5088(64)90118-3. (50) Zhang, Y.; Lin, L.-F.; Moreo, A.; Dagotto, E. Orbital-Selective Peierls Phase in the Metallic Dimerized Chain MoOCl2. Phys. Rev. B 2021, 104 (6), L060102. https://doi.org/10.110...

    work page doi:10.1016/0022-5088(64)90118-3 1964

  25. [25]

    (54) Biswas, S.; Grajower, M

    https://doi.org/10.1002/adfm.202519080. (54) Biswas, S.; Grajower, M. Y.; Watanabe, K.; Taniguchi, T.; Atwater, H. A. Broadband Electro-Optic Polarization Conversion with Atomically Thin Black Phosphorus. Science (80-. ). 2021, 374 (6566), 448–453. https://doi.org/10.1126/science.abj7053. (55) Zhang, D.-Q.; Shu, F.-Z.; Jiao, Z.-W.; Wu, H.-W. Tunable Wave ...

    work page doi:10.1002/adfm.202519080 2021

  26. [26]

    (56) Wang, H.; Chen, Q.; Cao, Y.; Sang, W.; Tan, F.; Li, H.; Wang, T.; Gan, Y.; Xiang, D.; Liu, T

    https://doi.org/10.1364/OE.418360. (56) Wang, H.; Chen, Q.; Cao, Y.; Sang, W.; Tan, F.; Li, H.; Wang, T.; Gan, Y.; Xiang, D.; Liu, T. Anisotropic Strain-Tailoring Nonlinear Optical Response in van Der Waals NbOI2. Nano Lett. 2024, 24 (11), 3413–3420. https://doi.org/10.1021/acs.nanolett.4c00039

    work page doi:10.1364/oe.418360 2024