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Erratum to: Strong coupling of multiple plasmon modes and excitons with excitation light controlled active tuning

This erratum corrects the original online version which can be found here: https://doi.org/10.1515/nanoph-2022-0701
  • Yijie Niu , Long Gao , Hongxing Xu EMAIL logo and Hong Wei ORCID logo EMAIL logo
Published/Copyright: May 17, 2023
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Nanophotonics
From the journal Nanophotonics Volume 12 Issue 12

After the publication of this article [1], the authors found that the energy range of the photoluminescence (PL) spectrum in the top panel of Figure 3c is incorrect. The correct version of Figure 3 is shown below, and the caption of the figure remains the same. This error does not affect the conclusions of the article.

Figure 3: Analyses of PL spectra for Ag NW-WSe2 coupled systems. (a) PL spectra of Ag NWs on monolayer WSe2 with different E 2. The red arrow marks the redshift of SPL mode. The two plexciton peaks are labeled as P1 and P2. The PL spectrum of bare monolayer WSe2 without Ag NW is plotted at the bottom. (b) Energies of fitting peaks in the experimental PL spectra as a function of E 2 (orange, blue, and green dots). The black lines are the calculated results for the scattering in Figure 2b. The black hollow dots are the energies of SPL mode extracted from the corresponding scattering spectra. (c) Top: PL spectrum for a Ag NW-WSe2 coupled system when SP2 mode is close to exciton energy (E 2 = 1.650 eV). Middle: Normalized PL spectrum resulting from dividing the top spectrum by the PL spectrum of bare WSe2. Bottom: Scattering spectrum for the same coupled system.
Figure 3:

Analyses of PL spectra for Ag NW-WSe2 coupled systems. (a) PL spectra of Ag NWs on monolayer WSe2 with different E 2. The red arrow marks the redshift of SPL mode. The two plexciton peaks are labeled as P1 and P2. The PL spectrum of bare monolayer WSe2 without Ag NW is plotted at the bottom. (b) Energies of fitting peaks in the experimental PL spectra as a function of E 2 (orange, blue, and green dots). The black lines are the calculated results for the scattering in Figure 2b. The black hollow dots are the energies of SPL mode extracted from the corresponding scattering spectra. (c) Top: PL spectrum for a Ag NW-WSe2 coupled system when SP2 mode is close to exciton energy (E 2 = 1.650 eV). Middle: Normalized PL spectrum resulting from dividing the top spectrum by the PL spectrum of bare WSe2. Bottom: Scattering spectrum for the same coupled system.

Corresponding authors: Hongxing Xu, School of Physics and Technology, Center for Nanoscience and Nanotechnology, and Key Laboratory of Artificial Micro- and Nano-structures of Ministry of Education, Wuhan University, Wuhan 430072, China; and School of Microelectronics, Wuhan University, Wuhan 430072, China, E-mail: ; and Hong Wei, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China; and Songshan Lake Materials Laboratory, Dongguan 523808, China, E-mail:

Reference

[1] Y. J. Niu, L. Gao, H. X. Xu, and H. Wei, “Strong coupling of multiple plasmon modes and excitons with excitation light controlled active tuning,” Nanophotonics, vol. 12, no. 4, pp. 735–742, 2023. https://doi.org/10.1515/nanoph-2022-0701.Search in Google Scholar
Published Online: 2023-05-17

© 2023 the author(s), published by De Gruyter, Berlin/Boston

This work is licensed under the Creative Commons Attribution 4.0 International License.

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  19. Erratum
  20. Erratum to: Strong coupling of multiple plasmon modes and excitons with excitation light controlled active tuning
https://doi.org/10.1515/nanoph-2023-0263
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Articles in the same Issue

  1. Frontmatter
  2. Review
  3. Two-dimensional material integrated micro-nano fiber, the new opportunity in all-optical signal processing
  4. Perspective
  5. Multifunctional charge transfer plasmon resonance sensors
  6. Research Articles
  7. A chiral inverse Faraday effect mediated by an inversely designed plasmonic antenna
  8. High spatiotemporal resolved imaging of ultrafast control of nondiffracting surface plasmon polaritons
  9. Lasing properties and carrier dynamics of CsPbBr3 perovskite nanocrystal vertical-cavity surface-emitting laser
  10. Terahertz spin-to-charge conversion in ferromagnetic Ni nanofilms
  11. Rotating axis measurement based on rotational Doppler effect of spliced superposed optical vortex
  12. Germanium metasurface assisted broadband detectors
  13. Hybridization of surface lattice modes: towards plasmonic metasurfaces with high flexible tunability
  14. Dielectric dual-dimer metasurface for enhanced mid-infrared chiral sensing under both excitation modes
  15. Honeycomb-like aluminum antennas for surface-enhanced infrared absorption sensing
  16. Micro-structured polyethylene film as an optically selective and self-cleaning layer for enhancing durability of radiative coolers
  17. Time-refraction optics with single cycle modulation
  18. Sub-to-super-Poissonian photon statistics in cathodoluminescence of color center ensembles in isolated diamond crystals
  19. Erratum
  20. Erratum to: Strong coupling of multiple plasmon modes and excitons with excitation light controlled active tuning
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