The DOI matches its Crossref record; 48 of the 49 references it cites were found in a registry or an index; none of the 4 sources its claims cite is checked for support yet.
Optical skyrmion lattice in evanescent electromagnetic fields
Open accessAbstract
Generating a lattice of optical skyrmions: The topological properties of systems can be robust to defects and imperfections. Skyrmions are one such topological entity, which resemble “hedgehog-like” structures. Tsesses et al. controlled the interference of plasmon polaritons on a patterned metallic surface to generate a lattice of optical skyrmions. Such control could potentially optically mimic complex condensed matter systems or help in the development of robust optical communications and circuits. Science , this issue p. 993
Overview
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Written from the paper’s full text.
TL;DR
The paper predicts and experimentally observes an optical skyrmion lattice formed by interfering evanescent electromagnetic waves, specifically surface plasmon polaritons. It shows that the electric-field vector can form Néel-type or bubble-type skyrmions and that the topological invariant is robust to losses and imperfections.
Key findings
- An optical skyrmion lattice is theoretically described using six interfering TM guided waves, with each lattice site forming a Néel-type skyrmion and calculated skyrmion number \(S = 1\).
- The skyrmion domain walls can be tuned from bubble-type to Néel-type by changing the transverse wave vector; the skyrmion number density contrast converges to 0.5 for the Néel-type case.
- Experimentally, surface plasmon polaritons on an air–gold interface produce a plasmonic skyrmion lattice with measured skyrmion number \(S = 0.997 \pm 0.058\).
- Loss robustness is quantified: 49 unit cells can exhibit \(S > 0.99\) if the waves persist for roughly 400 periods before decaying; the experimental sample had 37 lattice sites.
Methods
- Theory: six equal-amplitude TM guided waves propagating in the transverse plane with transverse wave vectors of similar magnitude create three standing waves at 0°, 60°, and 120°; the axial electric field is expressed as a sum of three cosine functions, and the skyrmion number is computed from the normalized three-component electric field.
- Experiment: SPPs are excited at an air–gold interface using a hexagonally shaped coupling slit and 660 nm circularly polarized light; the sample consists of six gratings on a 200 nm Au layer on a 1 mm glass substrate, with grating periodicity corresponding to the plasmonic wavelength of 636 nm.
- Measurement: phase-resolved near-field optical microscopy (s-NSOM) with pseudo-heterodyne interferometric detection measures the axial electric field at 20 nm resolution; spatial Fourier filtering is used to remove noise before extracting transverse field components and skyrmion number.
Limitations
- Stated: losses distort the unit vector \(e = E/|E|\) and create an unwanted phase difference between components; in the small-loss regime the real part still yields a well-defined skyrmion lattice, but \(S\) deviates slightly from its quantized value due to weak breaking of lattice translation symmetry, increasingly for unit cells farther from the origin.
- Stated: the finite structure and unequal SPP amplitudes—caused by different propagation lengths of SPPs generated by two slit edges and propagation loss—distort the skyrmion lattice.
- Evident from the text: the experiment demonstrates a bubble-type lattice at the center of the sample, while the full tuning from bubble-type to Néel-type skyrmions is shown theoretically; TE-polarized magnetic-field skyrmions are proposed but not experimentally demonstrated.
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Claims the paper makes
0 of 4 cited sources checked · 0 supported · 0 flagged
- Findingnone given
Once the electromagnetic waves gain evanescence in free-space, the skyrmion number jumps to the value of 1, independent of the change in the transverse wave vector.
“Once the electromagnetic waves gain evanescence in free-space, the skyrmion number jumps to the value of 1, independent of the change in the transverse wave vector.”
Quote in the paperSubstantial claim - Findingreasoning
In the small-loss regime, the skyrmion number S deviates slightly from its quantized value at zero losses due to the weak breaking of the lattice translation symmetry, increasingly more so for unit cells farther away from the point of origin.
“In this regime, the skyrmion number S deviates slightly from its quantized value at zero losses due to the weak breaking of the lattice translation symmetry, increasingly more so for unit cells which are farther away from the point of origin.”
Quote in the paperSubstantial claim - Findingreasoning
The property that all electric field components are real for evanescent waves does not hold for propagating waves.
“and hence does not hold for propagating waves (see Supplementary).”
Quote in the paperSubstantial claim - Findingown data
Optical skyrmion lattices are robust to imperfections.
“while illustrating their robustness to imperfections”
- Also stated in: § Discussion · plain
“We have also explored, theoretically and experimentally, the robustness of the topological properties of the system to losses, finiteness and other imperfections.”
Quote in the paperSubstantial claim - Also stated in: § Discussion · plain
- Findingreasoning
Free-space electromagnetic waves do not exhibit skyrmions.
“A more thorough explanation as to why free-space electromagnetic waves do not exhibit skyrmions can be found in the Supplementary.”
Quote in the paperSubstantial claim
- Findingown data
The interference of the SPPs in the middle of the coupling slit creates a plasmonic skyrmion lattice with characteristics typical to bubbles.
“The interference of the SPPs in the middle of the coupling slit creates a plasmonic skyrmion lattice with characteristics typical to bubbles, as portrayed in Fig. 5.”
Quote in the paperSubstantial claim - Findingown data
Optical skyrmion lattices can be easily created and controlled.
“we discover and observe optical skyrmion lattices that can be easily created and controlled”
Quote in the paperSubstantial claim - Findingown data
A configuration in which 49 sites exhibit S>0.99 is obtained if the electromagnetic waves creating it persist for roughly 400 periods before decaying.
“For example, a configuration in which 49 sites exhibit 0.99 S is obtained if the electromagnetic waves creating it persist for roughly 400 periods before decayingan easily achieved goal in many photonic systems.”
Quote in the paperNot a substantial claim - Findingnone given
Even guided modes with a relatively high amount of loss (decaying after 100 oscillations) can create skyrmion lattices.
“Moreover, they show that even guided modes with a relatively high amount of loss (decaying after 100 oscillations) can create skyrmion lattices.”
Quote in the paperNot a substantial claim - Findingown data
The extracted skyrmion number density at the center of the lattice resembles that of the bubble-type skyrmion lattice shown in the inset of Fig. 2 (point A).
“Fig. 5E depicts the extracted skyrmion number density at the center of the lattice, which resembles that of the bubble-type skyrmion lattice shown in the inset of Fig. 2 (point A).”
Quote in the paperNot a substantial claim - Premisereasoning
Surface plasmon polaritons are by design an imperfect system, due to the ohmic losses generated by the metal.
“Furthermore, they are by design an imperfect system, due to the ohmic losses generated by the metal.”
Quote in the paperSubstantial claim - Study design and conductcitation
The experimental setup enables phase-resolved measurement of the electric field normal to the surface by means of pseudo-heterodyne interferometric detection.
“The experimental setup used to detect optical skyrmions is depicted in Fig. 4 a scattering nearfield scanning optical microscope (s-NSOM), which enables phase-resolved measurement of the electric field normal to the surface by means of pseudo-heterodyne interferometric detection (42).”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [42]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationnone given
The optical skyrmions presented are entirely engineered by the boundary conditions of a linear system.
“whereas the optical skyrmions we present are entirely engineered by the boundary conditions of a linear system.”
Quote in the paperSubstantial claim - Interpretationreasoning
The bubble-like characteristics are a result of the relatively small transverse wave vector, leading to an axial field component 5 times larger than the transverse ones.
“This is a result of the relatively small transverse wave vector, leading to an axial field component 5 times larger than the transverse ones.”
Quote in the paperSubstantial claim - Interpretationreasoning
The transition from bubble-type to Néel-type skyrmions stems directly from the scaling factor k_z/k, which can be tuned by varying the effective index of a guided mode.
“This stems directly from the scaling factor / z kk , which can be tuned by varying the effective index (normalized propagation constant) of a guided mode.”
Quote in the paperSubstantial claim - Interpretationreasoning
The results are ubiquitous to any photonic system exhibiting evanescence, e.g. planar waveguide modes and waves undergoing total internal reflection (TIR).
“Our results are ubiquitous to any photonic system exhibiting evanescence, e.g.planar waveguide modes and waves undergoing total internal reflection (TIR).”
Quote in the paperSubstantial claim - Premisereasoning
The skyrmion number S, being an integer, is robust to deformations of the field e as long as e remains non-singular and maintains the periodicity of the lattice.
“The skyrmion number S, being an integer, is robust to deformations of the field e as long as e remains non-singular and maintains the periodicity of the lattice.”
Quote in the paperSubstantial claim - Study design and conductreasoning
The phase information, filtering ability and high spatial resolution of the measurement enable the correct extraction of the transverse field components and thus of the skyrmion number.
“The phase information, filtering ability and high spatial resolution of the measurement enable the correct extraction of the transverse field components and thusof the skyrmion number.”
Quote in the paperSubstantial claim - Interpretationown data
The electric field vector of electromagnetic waves can be structured to meet all requirements needed to create a skyrmion lattice, similarly to the magnetization vector of skyrmion lattices in chiral magnets.
“Interestingly, we find that the electric field vector of electromagnetic waves can be structured so as to meet all the requirements needed to create a skyrmion lattice, similarly to the magnetization vector of the skyrmion lattices in chiral magnets.”
Quote in the paperSubstantial claim
- It may state two separate claims as one. 11
- Probably not a substantial claim. 2
It may state two separate claims as one.
FindingreasoningFor k slightly larger than k0, the skyrmions are spatially confined (density contrast close to 1), with clear domain walls separating between two specific field states, effectively creating bubble-type skyrmions.
“For k slightly larger than 0 k , the skyrmions are spatially confined (density contrast close to 1), with clear domain walls separating between two specific field states, effectively creating bubble-type skyrmions (point A).”
Quote in the paperSubstantial claimIt may state two separate claims as one.
Findingown dataOptical skyrmions are experimentally demonstrated by interfering surface plasmon polaritons and measured via phase-resolved near-field optical microscopy.
“Optical skyrmions are experimentally demonstrated by interfering surface plasmon polaritons and are measured via phase-resolved near-field optical microscopy.”
Quote in the paperSubstantial claimIt may state two separate claims as one.
Findingown dataWe discovered and experimentally demonstrated an optical skyrmion lattice through the interference of electromagnetic waves.
“We discovered and experimentally demonstrated an optical skyrmion lattice through the interference of electromagnetic waves.”
Quote in the paperSubstantial claimIt may state two separate claims as one.
FindingreasoningAs k grows, the domain walls start to smear, creating skyrmions with increasingly uniform skyrmion number density, converging to the Néel-type field formation shown in Fig. 1 (point C, density contrast of 0.5).
“As k grows, the domain walls start to smear (point B), creating skyrmions with increasingly uniform skyrmion number density, converging to the Néel-type field formation shown in Fig. 1 (point C, density contrast of 0.5).”
Quote in the paperSubstantial claimIt may state two separate claims as one.
Findingnone givenIn the specific system used here, SPPs are excited at the interface of air and gold, resulting in both a small propagation decay and a transverse wave vector just slightly larger than the free-space wavenumber (k = (1.038+0.003i)k0).
“In the specific system used here (inset Fig. 4), SPPs are excited at the interface of air and gold, resulting in both a small propagation decay and a transverse wave vector just slightly larger than the free-space wavenumber ( 0 1.038 0.003 k i k ).”
Quote in the paperSubstantial claimIt may state two separate claims as one.
Findingown dataThe measured skyrmion number in each lattice site is S=0.997±0.058, demonstrating the robustness of the optical skyrmions.
“Calculating the skyrmion number in each lattice site, we reach the result 0.997 0.058 S , demonstrating the robustness of the optical skyrmions.”
- Also stated in: § Discussion · plain
“The measured skyrmion number of a single lattice site was 0.997 0.058 S , which, together with the figures, shows a good match to the theoretical prediction.”
Quote in the paperSubstantial claim- Also stated in: § Discussion · plain
It may state two separate claims as one.
FindingcitationFor waves evanescently decaying in one dimension, all electric field components are entirely real (up to a global phase), allowing definition of a real unit vector e=E/|E| and enabling description of the field configuration as an optical skyrmion lattice.
“Namely, for waves evanescently decaying in one dimension, all electric field components are entirely real (up to a global phase), allowing to define a real unit vector e= EE associated with the electric field and enabling a description of the field configuration as an optical skyrmion lattice.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [39]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
It may state two separate claims as one.
Findingown dataThe normalized three-dimensional electric field confirms the formation of a skyrmion lattice, with each lattice site exhibiting the distinct features of a Néel-type skyrmion and a calculated skyrmion number S=1.
“The normalized three-dimensional electric field (Fig. 1D) confirms the formation of a skyrmion latticeeach lattice site exhibits the distinct features of a Néel-type skyrmion (21), with their calculated skyrmion number, using Eq. ( 1), being 1 S .”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [21]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
It may state two separate claims as one.
FindingreasoningIn the regime of small losses, the configuration of the real part of the field still yields a well-defined skyrmion lattice, while being sufficiently larger than the imaginary part such that the latter is negligible.
“However, in the regime of small losses, the configuration of the real part of the field still yields a well-defined skyrmion lattice, while being sufficiently larger than the imaginary part such that the latter is negligible (see full derivation in the Supplementary).”
Quote in the paperSubstantial claimIt may state two separate claims as one.
Findingown dataThe real electric field is slightly distorted, as expected, but still shows similarity to the electric field configuration presented in Fig. 1.
“While the real electric field is slightly distorted, as expected (Fig. 5A-C), it still shows similarity to the electric field configuration presented in Fig. 1.”
Quote in the paperNot a substantial claimProbably not a substantial claim. The paper’s conclusions may not depend on it.
Premisenone givenThe optical skyrmions described in this work are in the frequency domain, i.e., formed in a physical field oscillating in time, as opposed to other skyrmions, which are field formations constant in time.
“It is worth emphasizing that the optical skyrmions described in this work are in the frequency domain, i.e., formed in a physical field oscillating in time, as opposed to other skyrmions, which are field formations constant in time.”
Quote in the paperNot a substantial claimIt may state two separate claims as one.
PremisecitationSurface plasmon polaritons only exist in TM polarization and the phase difference between SPPs propagating along different directions can be easily controlled.
“SPPs only exist in TM polarization and the phase difference between SPPs propagating along different directions can be easily controlled (41).”
Quote in the paperSubstantial claim0 of 1 sources checked- cites [41]
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim.
Study design and conductreasoningThe new definition of e as the real part of the local unit vector of the electric field is completely consistent with the prior description of optical skyrmions in the ideal case.
“This new definition is completely consistent with the prior description of optical skyrmions in the ideal case, which is determined by Eqs.(2,3) in a lossless medium.”
Quote in the paperSubstantial claim
The paper relies on this without support.
The field of optical skyrmions has so far remained untapped by experimental investigation.
“However, only recently has there been any experimental investigation of optical topological domain walls (38), while the field of optical skyrmions has so far remained untapped.”
Self-check
Percentages, sums and reported differences re-computed from the paper’s own numbers.
Each contradiction between two passages listed here was confirmed by an independent check.
Figure 1 cites Eq. 4 for a field defined by Eq. 3
MinorThe caption attributes the transverse electric-field amplitude to Eq. 4, but the paper identifies Eqs. (2,3) as the equations describing the electric field in Figure 1; Eq. 3 is introduced as the transverse-field equation.
“(B) Amplitude of the transverse (in-plane) electric field (Eq.4).”
“Figure 1 depicts the electric field described by Eqs.(2,3)”
Figure 5 points to Figure 3 for the measurement system
MinorFigure 5 says the measurement system is described in Figure 3, whereas Figure 4 is labeled as the experimental setup and sample characterization. Figure 3 instead concerns theoretical persistence in the presence of loss.
“The complex value of the axial electric field was measured with 20 nm resolution by the system described in Fig.3”
“Fig. 4. Experimental setup and sample characterization.”
Citations
Cites
Orbital angular momentum of light and the transformation of Laguerre-Gaussian laser modes
Allen, L., Beijersbergen, M. W., Spreeuw, R. J. C., & Woerdman, J. P. (1992) · Physical Review A · doi:10.1103/physreva.45.8185 · Cited by 10,455
Plasmonics: Fundamentals and Applications
Maier, S. A. (2007) · Springer eBooks · doi:10.1007/0-387-37825-1 · Cited by 9,943
Ordering, metastability and phase transitions in two-dimensional systems
Kosterlitz, J. M., & Thouless, D. J. (1973) · Journal of Physics C Solid State Physics · doi:10.1088/0022-3719/6/7/010 · Cited by 9,639
Vortices in high-temperature superconductors
Blatter, G., Feigel’man, M. V., Geshkenbeǐn, V. B., Larkin, A. I., & Vinokur, V. M. (1994) · Reviews of Modern Physics · doi:10.1103/revmodphys.66.1125 · Cited by 6,245
Skyrmion Lattice in a Chiral Magnet
Mühlbauer, S., Binz, B., Jonietz, F., Pfleiderer, C., Rosch, A., Neubauer, A., Georgii, R., & Böni, P. (2009) · Science · doi:10.1126/science.1166767 · Cited by 4,794
Topology of cosmic domains and strings
Kibble, T. W. B. (1976) · Journal of Physics A Mathematical and General · doi:10.1088/0305-4470/9/8/029 · Cited by 4,626
Topological properties and dynamics of magnetic skyrmions
Nagaosa, N., & Tokura, Y. (2013) · Nature Nanotechnology · doi:10.1038/nnano.2013.243 · Cited by 4,076
Real-space observation of a two-dimensional skyrmion crystal
Yu, X., Onose, Y., Kanazawa, N., Park, J. H., Han, J. H., Matsui, Y., Nagaosa, N., & Tokura, Y. (2010) · Nature · doi:10.1038/nature09124 · Cited by 3,453
Photonic Floquet topological insulators
Rechtsman, M. C., Zeuner, J. M., Plotnik, Y., Lumer, Y., Podolsky, D., Dreisow, F., Nolte, S., Segev, M., & Szameit, A. (2013) · Nature · doi:10.1038/nature12066 · Cited by 3,332
FERT, A., Cros, V., & Sampaio, J. (2013) · Nature Nanotechnology · doi:10.1038/nnano.2013.29 · Cited by 3,210
Observation of unidirectional backscattering-immune topological electromagnetic states
Wang, Z., Chong, Y., Joannopoulos, J. D., & Soljačić, M. (2009) · Nature · doi:10.1038/nature08293 · Cited by 3,123
A unified field theory of mesons and baryons
Skyrme, T. H. R. (1962) · Nuclear Physics · doi:10.1016/0029-5582(62)90775-7 · Cited by 2,596
Photonic topological insulators
Khanikaev, A. B., Hossein Mousavi, S., Tse, W.-K., Kargarian, M., MacDonald, A. H., & Shvets, G. (2013) · Nature Materials · doi:10.1038/nmat3520 · Cited by 1,971
Vortices in a Bose-Einstein Condensate
Matthews, M. R., Anderson, B. P., Haljan, P. C., Hall, D. S., Wieman, C., & Cornell, E. (1999) · Physical Review Letters · doi:10.1103/physrevlett.83.2498 · Cited by 1,842
Nucleation, stability and current-induced motion of isolated magnetic skyrmions in nanostructures
Sampaio, J., Cros, V., Rohart, S., Thiaville, A., & FERT, A. (2013) · Nature Nanotechnology · doi:10.1038/nnano.2013.210 · Cited by 1,788
Imaging topological edge states in silicon photonics
Hafezi, M., Mittal, S., Fan, J., Migdall, A., & Taylor, J. M. (2013) · Nature Photonics · doi:10.1038/nphoton.2013.274 · Cited by 1,715
Writing and Deleting Single Magnetic Skyrmions
Romming, N., Hanneken, C., Menzel, M., Bickel, J. E., Wolter, B., von Bergmann, K., Kubetzka, A., & Wiesendanger, R. (2013) · Science · doi:10.1126/science.1240573 · Cited by 1,553
Theory of the Motion of Vortices in Superconductors
Bardeen, J., & Stephen, M. J. (1965) · Physical Review · doi:10.1103/physrev.140.a1197 · Cited by 1,546
Topological insulator laser: Experiments
Bandres, M. A., Wittek, S., Harari, G., Parto, M., Ren, J., Segev, M., Christodoulides, D. N., & Khajavikhan, M. (2018) · Science · doi:10.1126/science.aar4005 · Cited by 1,315
Realizing effective magnetic field for photons by controlling the phase of dynamic modulation
Fang, K., Yu, Z., & Fan, S. (2012) · Nature Photonics · doi:10.1038/nphoton.2012.236 · Cited by 1,169
Mechanical equivalence of spin and orbital angular momentum of light: an optical spanner
Simpson, N. B., Dholakia, K., Allen, L., & Padgett, M. J. (1997) · Optics Letters · doi:10.1364/ol.22.000052 · Cited by 1,120
Über Integrale der hydrodynamischen Gleichungen, welche den Wirbelbewegungen entsprechen.
Helmholtz, H. (1858) · Journal für die reine und angewandte Mathematik (Crelles Journal) · doi:10.1515/crll.1858.55.25 · Cited by 899
Skyrmion flow near room temperature in an ultralow current density
Yu, X., Kanazawa, N., Zhang, W. Z., Nagai, T., Hara, T., Kimoto, K., Matsui, Y., Onose, Y., & Tokura, Y. (2012) · Nature Communications · doi:10.1038/ncomms1990 · Cited by 894
Theory of the Superfluidity of Helium II
Landau, L. (1941) · Physical Review · doi:10.1103/physrev.60.356 · Cited by 882
Topological insulator laser: Theory
Harari, G., Bandres, M. A., Lumer, Y., Rechtsman, M. C., Chong, Y. D., Khajavikhan, M., Christodoulides, D. N., & Segev, M. (2018) · Science · doi:10.1126/science.aar4003 · Cited by 848
Khanikaev, A. B., Mousavi, S. H., Tse, W.-K., Kargarian, M., MacDonald, A. H., & Shvets, G. B. (2012) · arXiv (Cornell University) · doi:10.48550/arxiv.1204.5700 · Cited by 813
Nonreciprocal lasing in topological cavities of arbitrary geometries
Bahari, B., Ndao, A., Vallini, F., El Amili, A., Fainman, Y., & Kanté, B. (2017) · Science · doi:10.1126/science.aao4551 · Cited by 770
Néel-type skyrmion lattice with confined orientation in the polar magnetic semiconductor GaV4S8
Kézsmárki, I., Bordács, S., Milde, P., Neuber, E., Eng, L. M., White, J. S., Rønnow, H. M., Dewhurst, C. D., Mochizuki, M., Yanai, K., et al. (2015) · Nature Materials · doi:10.1038/nmat4402 · Cited by 703
Pseudoheterodyne detection for background-free near-field spectroscopy
Ocelic, N., Huber, A. J., & Hillenbrand, R. (2006) · Applied Physics Letters · doi:10.1063/1.2348781 · Cited by 588
Topological charge and angular momentum of light beams carrying optical vortices
Soskin, M. S., Gorshkov, V. N., Vasnetsov, M. V., Malos, J. T., & Heckenberg, N. R. (1997) · Physical Review A · doi:10.1103/physreva.56.4064 · Cited by 554
On the vortex theory of screw propellers
Goldstein, S. (1929) · Proceedings of the Royal Society of London Series A Containing Papers of a Mathematical and Physical Character · doi:10.1098/rspa.1929.0078 · Cited by 527
Observation of the Spin-Based Plasmonic Effect in Nanoscale Structures
Gorodetski, Y., Niv, A., Kleiner, V., & Hasman, E. (2008) · Physical Review Letters · doi:10.1103/physrevlett.101.043903 · Cited by 446
Skyrmions in a ferromagnetic Bose–Einstein condensate
Khawaja, U. A., & Stoof, H. T. C. (2001) · Nature · doi:10.1038/35082010 · Cited by 403
Universal spin-momentum locking of evanescent waves
Mechelen, T. V., & Jacob, Z. (2016) · Optica · doi:10.1364/optica.3.000118 · Cited by 366
Revealing the subfemtosecond dynamics of orbital angular momentum in nanoplasmonic vortices
Spektor, G., Kilbane, D., Mahro, A.-K., Frank, B., Ristok, S., Gal, L., Kahl, P., Podbiel, D., Mathias, S., Giessen, H. W., et al. (2017) · Science · doi:10.1126/science.aaj1699 · Cited by 297
Electrical detection of single magnetic skyrmions in metallic multilayers at room temperature
Maccariello, D., Legrand, W., Reyren, N., Garcia, K. L., Bouzéhouane, K., Collin, S., Cros, V., & FERT, A. (2018) · Nature Nanotechnology · doi:10.1038/s41565-017-0044-4 · Cited by 296
LXIII. On Integrals of the hydrodynamical equations, which express vortex-motion
von Helmholtz, H. (1867) · The London Edinburgh and Dublin Philosophical Magazine and Journal of Science · doi:10.1080/14786446708639824 · Cited by 282
Quasi-two-dimensional Skyrmion lattices in a chiral nematic liquid crystal
Fukuda, J., & ŽUMER, S. (2011) · Nature Communications · doi:10.1038/ncomms1250 · Cited by 262
Realization of ground-state artificial skyrmion lattices at room temperature
Gilbert, D. A., Maranville, B. B., Balk, A. L., Kirby, B. J., Fischer, P., PIERCE, D. T., Unguris, J., Borchers, J. A., & Liu, K. (2015) · Nature Communications · doi:10.1038/ncomms9462 · Cited by 234
Polarization Singularities from Unfolding an Optical Vortex through a Birefringent Crystal
Flossmann, F., Schwarz, U. T., Maier, M., & Dennis, M. R. (2005) · Physical Review Letters · doi:10.1103/physrevlett.95.253901 · Cited by 224
Creating an Artificial Two-Dimensional Skyrmion Crystal by Nanopatterning
Sun, L., Cao, R., Miao, B. F., Feng, Z., You, B., Wu, D., Zhang, W., Hu, A., & Ding, H. (2013) · Physical Review Letters · doi:10.1103/physrevlett.110.167201 · Cited by 201
Berruto, G., Madan, I., Murooka, Y., Vanacore, G. M., Pomarico, E., Rajeswari, J., Lamb, R. J., Huang, P., Kruchkov, A., Togawa, Y., et al. (2018) · Physical Review Letters · doi:10.1103/physrevlett.120.117201 · Cited by 178
Dynamics and switching processes for magnetic bubbles in nanoelements
Moutafis, C., Komineas, S., & Bland, J. A. C. (2009) · Physical Review B · doi:10.1103/physrevb.79.224429 · Cited by 160
Huygens-Fresnel principle for surface plasmons
Teperik, T. V., Archambault, A., Marquier, F., & Greffet, J. (2009) · Optics Express · doi:10.1364/oe.17.017483 · Cited by 89
Experimental and theoretical study of the domain configuration in thin layers of BaFe_ O_
Kooy, C. L. D. (1960) · Cited by 78
Polarization domain walls in optical fibres as topological bits for data transmission
Gilles, M., Bony, P.-Y., Garnier, J. C., Picozzi, A., Guasoni, M., & Fatome, J. (2017) · Nature Photonics · doi:10.1038/nphoton.2016.262 · Cited by 63
Nanoscale control over optical singularities
Ostrovsky, E., Cohen, K. J., Tsesses, S., Gjonaj, B., & Bartal, G. (2018) · Optica · doi:10.1364/optica.5.000283 · Cited by 55
Self-citationSpin-patterned plasmonics: towards optical access to topological-insulator surface states
Spektor, G., David, A., Bartal, G., Orenstein, M., & Hayat, A. (2015) · Optics Express · doi:10.1364/oe.23.032759 · Cited by 24
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Flagged first, then by citations
1 of the 49 references couldn’t be matched to a known paper.
Cited by
Sorted by citations
Towards higher-dimensional structured light
He, C., Shen, Y., & Forbes, A. (2022) · Light Science & Applications · doi:10.1038/s41377-022-00897-3 · Cited by 651
Optical skyrmions and other topological quasiparticles of light
Shen, Y., Zhang, Q., Shi, P., Du, L., Yuan, X., & Zayats, A. V. (2024) · Nature Photonics · doi:10.1038/s41566-023-01325-7 · Cited by 469
Du, L., Yang, A., Zayats, A. V., & Yuan, X. (2019) · Nature Physics · doi:10.1038/s41567-019-0487-7 · Cited by 416
Light–matter interactions with photonic quasiparticles
Rivera, N., & Kaminer, I. E. (2020) · Nature Reviews Physics · doi:10.1038/s42254-020-0224-2 · Cited by 400
Frontiers in multidimensional self-trapping of nonlinear fields and matter
Kartashov, Y. V., Astrakharchik, G. E., Malomed, B. A., & Torner, L. (2019) · Nature Reviews Physics · doi:10.1038/s42254-019-0025-7 · Cited by 382
Ultrafast vector imaging of plasmonic skyrmion dynamics with deep subwavelength resolution
Davis, T. J., Janoschka, D., Dreher, P., Frank, B., Meyer zu Heringdorf, F.-J., & Giessen, H. (2020) · Science · doi:10.1126/science.aba6415 · Cited by 296
Generation of Optical Skyrmions with Tunable Topological Textures
Shen, Y., Martínez, E. C., & Rosales-Guzmán, C. (2022) · ACS Photonics · doi:10.1021/acsphotonics.1c01703 · Cited by 278
Plasmonic topological quasiparticle on the nanometre and femtosecond scales
Dai, Y., Zhou, Z., Ghosh, A., Mong, R. S. K., Kubo, A., Huang, C., & Petek, H. (2020) · Nature · doi:10.1038/s41586-020-3030-1 · Cited by 277
Gao, S., Speirits, F. C., Castellucci, F., Franke-Arnold, S., Barnett, S. M., & Götte, J. B. (2020) · Physical Review A · doi:10.1103/physreva.102.053513 · Cited by 253
Statics and dynamics of skyrmions interacting with disorder and nanostructures
Reichhardt, C. J. O., Reichhardt, C. J. O., & Miloševıć, M. V. (2022) · Reviews of Modern Physics · doi:10.1103/revmodphys.94.035005 · Cited by 251
Particle-like topologies in light
Sugic, D., Droop, R., Otte, E., Ehrmanntraut, D., Nori, F., Ruostekoski, J., Denz, C., & Dennis, M. R. (2021) · Nature Communications · doi:10.1038/s41467-021-26171-5 · Cited by 221
Supertoroidal light pulses as electromagnetic skyrmions propagating in free space
Shen, Y., Hou, Y., Papasimakis, N., & Zheludev, N. I. (2021) · Nature Communications · doi:10.1038/s41467-021-26037-w · Cited by 213
Photonic Spin Lattices: Symmetry Constraints for Skyrmion and Meron Topologies
Lei, X., Yang, A., Shi, P., Xie, Z., Du, L., Zayats, A. V., & Yuan, X. (2021) · Physical Review Letters · doi:10.1103/physrevlett.127.237403 · Cited by 178
Roadmap on photonic metasurfaces
Schulz, S. A., Oulton, R. F., Kenney, M., Alù, A., Staude, I., Bashiri, A., Fedorova, Z., Kołkowski, R., Koenderink, A. F., Xiao, X., et al. (2024) · Applied Physics Letters · doi:10.1063/5.0204694 · Cited by 171
Non-local skyrmions as topologically resilient quantum entangled states of light
Ornelas, P., Nape, I., de Mello Koch, R., & Forbes, A. (2024) · Nature Photonics · doi:10.1038/s41566-023-01360-4 · Cited by 167
Nonseparable States of Light: From Quantum to Classical
Shen, Y., & Rosales‐Guzmán, C. (2022) · Laser & Photonics Reviews · doi:10.1002/lpor.202100533 · Cited by 160
Observation of localized magnetic plasmon skyrmions
Deng, Z.-L., Shi, T., Krasnok, A., Li, X., & Alù, A. (2022) · Nature Communications · doi:10.1038/s41467-021-27710-w · Cited by 157
Bliokh, K. Y., Karimi, E., Padgett, M. J., Alonso, M. A., Dennis, M. R., Dudley, A. L., Forbes, A., Zahedpour, S., Hancock, S. W., Milchberg, H. M., et al. (2023) · Journal of Optics · doi:10.1088/2040-8986/acea92 · Cited by 143
Shen, Y. (2021) · Optics Letters · doi:10.1364/ol.431122 · Cited by 142
Vortex laser arrays with topological charge control and self-healing of defects
Piccardo, M., Oliveira, M. D., Toma, A., Aglieri, V., Forbes, A., & Ambrosio, A. (2022) · Nature Photonics · doi:10.1038/s41566-022-00986-0 · Cited by 140
Visible-to-THz near-field nanoscopy
Hillenbrand, R., Abate, Y., Liu, M. K., Chen, X., & Basov, D. N. (2025) · Nature Reviews Materials · doi:10.1038/s41578-024-00761-3 · Cited by 140
Optical vortex lattice: an exploitation of orbital angular momentum
Zhu, L., Tang, M., Li, H., Tai, Y., & Li, X. (2021) · Nanophotonics · doi:10.1515/nanoph-2021-0139 · Cited by 136
Topological phononic metamaterials
Zhu, W., Deng, W., Liu, Y., Lu, J., Wang, H., Lin, Z., Huang, X., Jiang, J., & Liu, Z. (2023) · Reports on Progress in Physics · doi:10.1088/1361-6633/aceeee · Cited by 130
Observation of Acoustic Skyrmions
Ge, H., Xu, X.-Y., Liu, L., Xu, R., Lin, Z.-K., Yu, S.-Y., Bao, M., Jiang, J.-H., Lu, M.-H., & Chen, Y.-F. (2021) · Physical Review Letters · doi:10.1103/physrevlett.127.144502 · Cited by 125
Topological transformation and free-space transport of photonic hopfions
Shen, Y., Yu, B., Wu, H., Li, C., Zhu, Z., & Zayats, A. V. (2023) · Advanced Photonics · doi:10.1117/1.ap.5.1.015001 · Cited by 123
Karnieli, A., Tsesses, S., Bartal, G., & Arie, A. (2021) · Nature Communications · doi:10.1038/s41467-021-21250-z · Cited by 122
Self-citationMicrocavity-based generation of full Poincaré beams with arbitrary skyrmion numbers
Lin, W., Ota, Y., Arakawa, Y., & Iwamoto, S. (2021) · Physical Review Research · doi:10.1103/physrevresearch.3.023055 · Cited by 122
Diffractive optical elements 75 years on: from micro-optics to metasurfaces
Zhang, Q., He, Z., Xie, Z., Tan, Q., Sheng, Y., Jin, G., Cao, L., & Yuan, X. (2023) · Photonics Insights · doi:10.3788/pi.2023.r09 · Cited by 118
Advances in light transverse momenta and optical lateral forces
Shi, Y., Xu, X., Nieto‐Vesperinas, M., Song, Q., Liu, A. Q., Cipparrone, G., Su, Z., Yao, B., Wang, Z., Qiu, C., et al. (2023) · Advances in Optics and Photonics · doi:10.1364/aop.489300 · Cited by 117
Meron Spin Textures in Momentum Space
Guo, C., Xiao, M., Guo, Y., Yuan, L., & Fan, S. (2020) · Physical Review Letters · doi:10.1103/physrevlett.124.106103 · Cited by 113
Transverse spin dynamics in structured electromagnetic guided waves
Shi, P., Du, L., Li, C., Zayats, A. V., & Yuan, X. (2021) · Proceedings of the National Academy of Sciences · doi:10.1073/pnas.2018816118 · Cited by 112
Observation of emergent momentum–time skyrmions in parity–time-symmetric non-unitary quench dynamics
Wang, K., Qiu, X., Xiao, L., Zhan, X., Bian, Z., Sanders, B. C., Yi, W., & Xue, P. (2019) · Nature Communications · doi:10.1038/s41467-019-10252-7 · Cited by 109
Topological polarization singularities in metaphotonics
Liu, W., Liu, W., Shi, L., & Kivshar, Y. (2021) · Nanophotonics · doi:10.1515/nanoph-2020-0654 · Cited by 107
Spin‐Manipulated Photonic Skyrmion‐Pair for Pico‐Metric Displacement Sensing
Yang, A., Lei, X., Shi, P., Meng, F., Lin, M., Du, L., & Yuan, X. (2023) · Advanced Science · doi:10.1002/advs.202205249 · Cited by 103
Topological protection of optical skyrmions through complex media
Wang, A. A., Zhao, Z., Ma, Y., Cai, Y., Zhang, R., Shang, X., Zhang, Y., Qin, J., Pong, Z.-K., Marozsák, T., et al. (2024) · Light: Science & Applications · doi:10.1038/s41377-024-01659-z · Cited by 102
Spin–Orbit Interaction of Light in Plasmonic Lattices
Tsesses, S., Cohen, K., Ostrovsky, E., Gjonaj, B., & Bartal, G. (2019) · Nano Letters · doi:10.1021/acs.nanolett.9b01343 · Cited by 101
Self-citationPolarization singularities: Progress, fundamental physics, and prospects
Wang, Q., Tu, C., Li, Y., & Wang, H. (2021) · APL Photonics · doi:10.1063/5.0045261 · Cited by 101
Optical polarization skyrmionic fields in free space
Gutiérrez–Cuevas, R., & Pisanty, E. (2021) · Journal of Optics · doi:10.1088/2040-8986/abe8b2 · Cited by 100
Rays, waves, SU(2) symmetry and geometry: toolkits for structured light
Shen, Y. (2021) · Journal of Optics · doi:10.1088/2040-8986/ac3676 · Cited by 100
Optical skyrmions from metafibers with subwavelength features
He, T., Meng, Y., Wang, L., Zhong, H., Mata-Cervera, N., Li, D., Yan, P., Liu, Q., Shen, Y., & Xiao, Q. (2024) · Nature Communications · doi:10.1038/s41467-024-54207-z · Cited by 96
Free-space topological optical textures: tutorial
Shen, Y., Wang, H., & Fan, S. (2025) · Advances in Optics and Photonics · doi:10.1364/aop.547634 · Cited by 94
Topological metasurface: from passive toward active and beyond
You, J. W., Lan, Z., Ma, Q., Gao, Z. L., Yang, Y., Gao, F., Xiao, M., & Cui, T. J. (2022) · Photonics Research · doi:10.1364/prj.471905 · Cited by 93
Water-Wave Vortices and Skyrmions
Smirnova, D. A., Nori, F., & Bliokh, K. Y. (2024) · Physical Review Letters · doi:10.1103/physrevlett.132.054003 · Cited by 90
Roadmap for Photonics with 2D Materials
de Abajo, F. J. G., Basov, D. N., Koppens, F. H. L., Orsini, L. M., Ceccanti, M., Castilla, S., Cavicchi, L., Polini, M., Gonçalves, P. A. D., Costa, A. T., et al. (2025) · ACS Photonics · doi:10.1021/acsphotonics.5c00353 · Cited by 90
Self-citationSpin photonics: from transverse spin to photonic skyrmions
Shi, P., Du, L., & Yuan, X. (2021) · Nanophotonics · doi:10.1515/nanoph-2021-0046 · Cited by 89
Optical sorting: past, present and future
Yang, M., Shi, Y., Song, Q., Wei, Z., Dun, X., Wang, Z. M., Wang, Z., Qiu, C., Zhang, H., & Cheng, X. (2025) · Light Science & Applications · doi:10.1038/s41377-024-01734-5 · Cited by 88
Disorder-Induced Topological State Transition in the Optical Skyrmion Family
Liu, C., Zhang, S., Maier, S. A., & Ren, H. (2022) · Physical Review Letters · doi:10.1103/physrevlett.129.267401 · Cited by 87
Topological Structures of Energy Flow: Poynting Vector Skyrmions
Wang, S., Zhou, Z., Zheng, Z., Sun, J., Cao, H., Song, S., Deng, Z., Qin, F., Cao, Y., & Li, X. (2024) · Physical Review Letters · doi:10.1103/physrevlett.133.073802 · Cited by 85
Conformal frequency conversion for arbitrary vectorial structured light
Wu, H.-J., Yu, B.-S., Zhu, Z.-H., Gao, W., Ding, D.-S., Zhou, Z.-Y., Hu, X.-P., Rosales-Guzmán, C., Shen, Y., & Shi, B.-S. (2022) · Optica · doi:10.1364/optica.444685 · Cited by 84
Topological water-wave structures manipulating particles
Wang, B., Che, Z., Cheng, C., Tong, C., Shi, L., Shen, Y., Bliokh, K. Y., & Zi, J. (2025) · Nature · doi:10.1038/s41586-024-08384-y · Cited by 81
Topological Approach of Characterizing Optical Skyrmions and Multi‐Skyrmions
McWilliam, A., Cisowski, C. M., Ye, Z., Speirits, F. C., Götte, J. B., Barnett, S. M., & Franke‐Arnold, S. (2023) · Laser & Photonics Reviews · doi:10.1002/lpor.202300155 · Cited by 80
Hopf Solitons in Helical and Conical Backgrounds of Chiral Magnetic Solids
Voinescu, R., Tai, J. B., & Smalyukh, I. I. (2020) · Physical Review Letters · doi:10.1103/physrevlett.125.057201 · Cited by 80
Ferroelectric incommensurate spin crystals
Rusu, D., Peters, J. J. P., Hase, T. P. A., Gott, J. A., Nisbet, G. A. A., Strempfer, J., Haskel, D., Seddon, S. D., Beanland, R., Sánchez, A. M., et al. (2022) · Nature · doi:10.1038/s41586-021-04260-1 · Cited by 80
Topologically controlled multiskyrmions in photonic gradient-index lenses
Shen, Y., He, C., Song, Z., Chen, B., He, H., Ma, Y., Fells, J., Elston, S. J., Morris, S., Booth, M. J., et al. (2024) · Physical Review Applied · doi:10.1103/physrevapplied.21.024025 · Cited by 79
Wan, C., Shen, Y., Chong, A., & Zhan, Q. (2022) · eLight · doi:10.1186/s43593-022-00030-2 · Cited by 78
Ultrafast microscopy of a twisted plasmonic spin skyrmion
Dai, Y., Zhou, Z., Ghosh, A., Kapoor, K., Da̧browski, M., Kubo, A., Huang, C., & Petek, H. (2022) · Applied Physics Reviews · doi:10.1063/5.0084482 · Cited by 78
Physical conversion and superposition of optical skyrmion topologies
Teng, H., Zhong, J., Chen, J., Lei, X., & Zhan, Q. (2023) · Photonics Research · doi:10.1364/prj.499485 · Cited by 78
Observation of Polarization Singularities and Topological Textures in Sound Waves
Muelas-Hurtado, R. D., Volke-Sepúlveda, K., Ealo, J. L., Nori, F., Alonso, M. A., Bliokh, K. Y., & Brasselet, E. (2022) · Physical Review Letters · doi:10.1103/physrevlett.129.204301 · Cited by 75
Real-time sub-wavelength imaging of surface waves with nonlinear near-field optical microscopy
Frischwasser, K., Cohen, K. J., Kher-Alden, J., Dolev, S., Tsesses, S., & Bartal, G. (2021) · Nature Photonics · doi:10.1038/s41566-021-00782-2 · Cited by 71
Self-citationA topological lattice of plasmonic merons
Ghosh, A., Yang, S., Dai, Y., Zhou, Z., Wang, T., Huang, C.-B., & Petek, H. (2021) · Applied Physics Reviews · doi:10.1063/5.0062133 · Cited by 70
Lei, X., Du, L., Yuan, X., & Zayats, A. V. (2021) · Nanophotonics · doi:10.1515/nanoph-2021-0201 · Cited by 69
Bloch-type photonic skyrmions in optical chiral multilayers
Zhang, Q., Xie, Z., Du, L., Shi, P., & Yuan, X. (2021) · Physical Review Research · doi:10.1103/physrevresearch.3.023109 · Cited by 69
Geometric descriptions for the polarization of nonparaxial light: a tutorial
Alonso, M. A. (2023) · Advances in Optics and Photonics · doi:10.1364/aop.475491 · Cited by 68
Multiple low-temperature skyrmionic states in a bulk chiral magnet
Bannenberg, L. J., Wilhelm, H., Cubitt, R., Labh, A., Schmidt, M. P., Lelièvre-Berna, E., Pappas, C., MOSTOVOY, M. V., & Leonov, A. O. (2019) · npj Quantum Materials · doi:10.1038/s41535-019-0150-7 · Cited by 66
Tai, J. B., & Smalyukh, I. I. (2020) · Physical review. E · doi:10.1103/physreve.101.042702 · Cited by 64
Tunable photon-induced spatial modulation of free electrons
Tsesses, S., Dahan, R., Wang, K., Bucher, T., Cohen, K. J., Reinhardt, O., Bartal, G., & Kaminer, I. E. (2023) · Nature Materials · doi:10.1038/s41563-022-01449-1 · Cited by 62
Self-citationOptical topological lattices of Bloch-type skyrmion and meron topologies
Zhang, Q., Xie, Z., Shi, P., Yang, H., He, H., Du, L., & Yuan, X. (2022) · Photonics Research · doi:10.1364/prj.447311 · Cited by 61
On-chip optical skyrmionic beam generators
Lin, W., Ota, Y., Arakawa, Y., & Iwamoto, S. (2024) · Optica · doi:10.1364/optica.540469 · Cited by 61
Dynamic Display of Full-Stokes Vectorial Holography Based on Metasurfaces
Zhang, S., Huang, L., Li, X., Zhao, R., Wei, Q., Zhou, H., Jiang, Q., Geng, G., Li, J., Li, X., et al. (2021) · ACS Photonics · doi:10.1021/acsphotonics.1c00307 · Cited by 59
Dynamic tailoring of an optical skyrmion lattice in surface plasmon polaritons
Bai, C., Chen, J., Zhang, Y., Zhang, D., & Zhan, Q. (2020) · Optics Express · doi:10.1364/oe.384718 · Cited by 57
Observation of phononic skyrmions based on hybrid spin of elastic waves
Cao, L., Wan, S., Zeng, Y., Zhu, Y., & Assouar, B. (2023) · Science Advances · doi:10.1126/sciadv.adf3652 · Cited by 55
Generation and detection of spin-orbit coupled neutron beams
Sarenac, D., Kapahi, C., Chen, W., Clark, C. W., Cory, D. G., Huber, M. G., Taminiau, I., Zhernenkov, K., & Pushin, D. A. (2019) · Proceedings of the National Academy of Sciences · doi:10.1073/pnas.1906861116 · Cited by 55
Dynamical Control of Topology in Polar Skyrmions via Twisted Light
Gao, L., Prokhorenko, S., Nahas, Y., & Bellaïche, L. (2024) · Physical Review Letters · doi:10.1103/physrevlett.132.026902 · Cited by 54
Controlled negative energy flow in the focus of a radial polarized optical beam
Li, H., Wang, C., Tang, M., & Li, X. (2020) · Optics Express · doi:10.1364/oe.391398 · Cited by 52
Orbital Angular Momentum in Nanoplasmonic Vortices
Prinz, E., Hartelt, M., Spektor, G., Orenstein, M., & Aeschlimann, M. (2023) · ACS Photonics · doi:10.1021/acsphotonics.2c01321 · Cited by 51
Photonic Spin Skyrmion with Dynamic Position Control
Lin, M., Zhang, W., Liu, C., Du, L., & Yuan, X. (2021) · ACS Photonics · doi:10.1021/acsphotonics.1c00762 · Cited by 50
Symmetry‐Protected Spoof Localized Surface Plasmonic Skyrmion
Yang, J., Zheng, X., Wang, J., Pan, Y., Zhang, A., Cui, T. J., & Vandenbosch, G. A. E. (2022) · Laser & Photonics Reviews · doi:10.1002/lpor.202200007 · Cited by 49
Observation of an acoustic topological Euler insulator with meronic waves
Jiang, B., Bouhon, A., Wu, S.-Q., Kong, Z., Lin, Z., Slager, R.-J., & Jiang, J. (2024) · 中国科学通报:英文版 · doi:10.1016/j.scib.2024.04.009 · Cited by 49
Nanophotonic quantum skyrmions enabled by semiconductor cavity quantum electrodynamics
Ma, J., Yang, J., Liu, S., Chen, B., Li, X., Song, C., Qiu, G., Zou, K., Hu, X., Li, F., et al. (2025) · Nature Physics · doi:10.1038/s41567-025-02973-y · Cited by 49
Building Paraxial Optical Skyrmions Using Rational Maps
Cisowski, C. M., Ross, C., & Franke‐Arnold, S. (2023) · Advanced Photonics Research · doi:10.1002/adpr.202200350 · Cited by 48
Skyrmion bags of light in plasmonic moiré superlattices
Schwab, J., Neuhaus, A., Dreher, P., Tsesses, S., Cohen, K. J., Mangold, F., Mantha, A., Frank, B., Bartal, G., zu Heringdorf, F. ‐. M., et al. (2025) · Nature Physics · doi:10.1038/s41567-025-02873-1 · Cited by 48
Self-citationCoherently amplified ultrafast imaging using a free-electron interferometer
Bucher, T., Nahari, H., Sheinfux, H. H., Ruimy, R., Niedermayr, A., Dahan, R., Yan, Q., Adiv, Y., Yannai, M., Chen, J., et al. (2024) · Nature Photonics · doi:10.1038/s41566-024-01451-w · Cited by 47
Self-citationZeng, Y., Yu, Y., Shen, X., Chen, J., & Zhan, Q. (2024) · Nanophotonics · doi:10.1515/nanoph-2023-0741 · Cited by 46
Observation of resilient propagation and free-space skyrmions in toroidal electromagnetic pulses
Wang, R., Bao, P.-Y., Hu, Z., Shi, S., Wang, B., Zheludev, N. I., & Shen, Y. (2024) · Applied Physics Reviews · doi:10.1063/5.0218207 · Cited by 46
Q -Plates: From Optical Vortices to Optical Skyrmions
Hakobyan, V., & Brasselet, E. (2025) · Physical Review Letters · doi:10.1103/physrevlett.134.083802 · Cited by 46
Generation and characterization of complex vector modes with digital micromirror devices: a tutorial
Hu, X., & Rosales‐Guzmán, C. (2021) · Journal of Optics · doi:10.1088/2040-8986/ac4671 · Cited by 46
Recent Advances and Prospects of Optical Metasurfaces
Zhang, S., Zhou, H., Liu, B., Su, Z., & Huang, L. (2023) · ACS Photonics · doi:10.1021/acsphotonics.2c01539 · Cited by 45
Optical skyrmion laser using a wedged output coupler
Kerridge‐Johns, W. R., Rao, A. S., & Omatsu, T. (2024) · Optica · doi:10.1364/optica.521901 · Cited by 45
Construction of optical spatiotemporal skyrmions
Teng, H., Liu, X., Zhang, N., Fan, H., Chen, G., Cao, Q., Zhong, J., Lei, X., & Zhan, Q. (2025) · Light Science & Applications · doi:10.1038/s41377-025-02028-0 · Cited by 44
Quantum field theory for spin operator of the photon
Yang, L., Khosravi, F., & Jacob, Z. (2022) · Physical Review Research · doi:10.1103/physrevresearch.4.023165 · Cited by 44
Optical second-order skyrmionic hopfion
Ehrmanntraut, D., Droop, R., Sugic, D., Otte, E., Dennis, M. R., & Denz, C. (2023) · Optica · doi:10.1364/optica.487989 · Cited by 43
Optical skyrmions in the Bessel profile
Rao, A. S. (2024) · Journal of the Optical Society of America A · doi:10.1364/josaa.522001 · Cited by 43
Perturbation-resilient integer arithmetic using optical skyrmions
Wang, A. A., Ma, Y., Zhang, Y., Zhao, Z., Cai, Y., Qiu, X., Dong, B., & He, C. (2025) · Nature Photonics · doi:10.1038/s41566-025-01779-x · Cited by 43
Dohi, T., Reeve, R. M., & Kläui, M. (2021) · Annual Review of Condensed Matter Physics · doi:10.1146/annurev-conmatphys-031620-110344 · Cited by 43
Original Data for Manuscript "Orbital angular momentum multiplication in plasmonic vortex cavities"
Spektor, G., Prinz, E., Hartelt, M., Mahro, A.-K., Aeschlimann, M., & Orenstein, M. (2021) · Figshare · doi:10.5281/zenodo.4773044 · Cited by 43
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Lu, C., Wang, B., Fang, X., Tsai, D. P., Zhu, W., Song, Q., Xiao, D., He, T., Gong, X., Luo, H., et al. (2023) · Nano Letters · doi:10.1021/acs.nanolett.3c03351 · Cited by 41
Topological Quasiparticles of Light: From Spin‐Orbit Coupling to Photonic Skyrmions
Lei, X., & Zhan, Q. (2025) · Laser & Photonics Review · doi:10.1002/lpor.202501427 · Cited by 41
Optical excitations of Skyrmions, knotted solitons, and defects in atoms
Parmee, C. D., Dennis, M. R., & Ruostekoski, J. (2022) · Communications Physics · doi:10.1038/s42005-022-00829-y · Cited by 40
Photonic Spin Hopfions and Monopole Loops
Wang, H., & Fan, S. (2023) · Physical Review Letters · doi:10.1103/physrevlett.131.263801 · Cited by 40
Symmetry‐Protected Photonic Chiral Spin Textures by Spin–Orbit Coupling
Shi, P., Du, L., Li, M., & Yuan, X. (2021) · Laser & Photonics Reviews · doi:10.1002/lpor.202000554 · Cited by 39
Metadata
- Authors
- Tsesses, S., Ostrovsky, E., Cohen, K., Gjonaj, B., Lindner, N. H., & Bartal, G.
- Affiliations
- Technion – Israel Institute of Technology (IL)
- Albanian University (AL)
- Corresponding author
- Bartal, G.
- Venue
- Science
- Published
- 2018-09-07
- Volume
- 361
- Issue
- 6406
- Pages
- 993-996
- ISSN
- 0036-8075 (ISSN-L)
- 1095-9203
- OpenAlex
- W2884207325
- Cited by
- 514
- References
- 49
- Citations by year
- 2026: 129 · 2025: 122 · 2024: 84 · 2023: 58 · 2022: 38 · 2021: 36 · 2020: 30 · 2019: 16 · 2018: 1
- FWCI
- 9.96
- Type
- journal article
- Language
- en
- Open access
- green
- arxiv.org
- Locations
- Science (publishedVersion)
- PubMed (publishedVersion)
- arXiv (Cornell University) (submittedVersion)
- Figshare (submittedVersion, public-domain)
- arXiv (Cornell University)
- Funders
- H2020 European Research Council (639172)
- “Circle of Light,” Israeli Centers for Research Excellence (Israel Science Foundation (ISF) (1802/12))
- "Circle of Light", Israeli Centers of Research Excellence (Israel Science Foundation (ISF) (1802/12))
- Topics
- Physical Sciences › Physics and Astronomy › Atomic and Molecular Physics, and Optics › Orbital Angular Momentum in Optics
- Physical Sciences › Physics and Astronomy › Atomic and Molecular Physics, and Optics › Plasmonic and Surface Plasmon Research
- Physical Sciences › Physics and Astronomy › Condensed Matter Physics › Topological Materials and Phenomena
- Keywords
- surface plasmon polaritons, topological defects, Néel skyrmions, topological domain walls, photonic systems, optical information processing
About these checks
Registry, retraction, Cites and statistics results are computed, not judged, with one exception: a printed reference that no index lists is read once by a model before it counts as a citation error. Claims are extracted by a model and kept only when their quote appears verbatim in the text; each cited source is then checked, with a model’s help, for whether it says what the claim relies on. Those verdicts can be wrong — read the claim’s quote and the cited source before relying on one.
A language model drew the claims from the paper on 2026-11-10, under version 3 of the claim definition (model deepseek-v4.1-flash, prompt extract-v3).
A second model labelled each claim on 2026-11-10 (model jev-1.13-20260917, definition revision gold-guideline-v0.2).
Statistics and arithmetic are recomputed, not judged.
Confidence bands are shown only for fields calibrated on our annotated test set. None is calibrated yet, so no band is shown.
What counts as a claim ›How we measure confidence ›How we check this ›
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