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Journal articles on the topic 'Plasmon damping'

Author: Grafiati

Published: 4 June 2021

Last updated: 1 February 2022

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1

Semenenko, Vyacheslav, Simone Schuler, Alba Centeno, Amaia Zurutuza, Thomas Mueller, and Vasili Perebeinos. "Plasmon–Plasmon Interactions and Radiative Damping of Graphene Plasmons." ACS Photonics 5, no. 9 (August 9, 2018): 3459–65. http://dx.doi.org/10.1021/acsphotonics.8b00544.

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2

TINKOV, V. A., and M. A. VASYLYEV. "THERMO-INDUCED SHIFT OF PLASMON ENERGY IN ELECTRON LOSS SPECTRA FOR THE ORDERING Pt80Co20(111) ALLOY SURFACE." Surface Review and Letters 16, no. 02 (April 2009): 249–58. http://dx.doi.org/10.1142/s0218625x0901255x.

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Electron energy loss spectroscopy has been used for the investigation of the surface and bulk plasmon excitations depending on the heating in the ultra-thin layers of ordering Pt 80 Co 20(111) alloy from the primary electron beam energies E0 ranging from 200 to 650 eV. Thermo-induced shift of plasmon energy and damping of intensity line of the surface plasmon relative to the bulk plasmon were observed. With an increase in alloy heating, the energy of surface and bulk plasmons is shifted with lowering energy in the whole range E0 and the higher the temperature the higher the shifts of plasmon energy. The physical processes that can influence on the energy shift of plasmon oscillations in the energy loss spectra at heating are considered. The relationship between the damping of oscillating concentration depth profile and the surface plasmon damping at heating was established.

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3

Jiang, Wei, Huatian Hu, Qian Deng, Shunping Zhang, and Hongxing Xu. "Temperature-dependent dark-field scattering of single plasmonic nanocavity." Nanophotonics 9, no. 10 (May 23, 2020): 3347–56. http://dx.doi.org/10.1515/nanoph-2020-0076.

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AbstractPlasmonic materials have long been exploited for enhanced spectroscopy, integrated nanophotonic circuits, sensing, light harvesting, etc. Damping is the key factor that limits their performance and restricts the development of the field. Optical characterization of single nanoparticle at low temperature is ideal for investigating the damping of plasmons but is usually technically impractical due to the sample vibration from the cryostat and the surface adsorption during the cooling process. In this work, we use a vibration-free cryostat to investigate the temperature-dependent dark-field scattering spectroscopy of a single Au nanowire on top of a Au film. This allows us to extract the contribution of electron-phonon scattering to the damping of plasmons without performing statistics over different target nanoparticles. The results show that the full width at half-maximum of the plasmon resonance increases by an amount of 5.8%, over the temperature range of 5−150 K. Electromagnetic calculations reveal that the temperature-insensitive dissipation channels into photons or surface plasmon polaritons on the Au film contribute up to 64% of the total dissipations at the plasmon resonance. This explains why the reduction of plasmon linewidth seems small at the single-particle level. This study provides a more explicit measurement on the damping process of the single plasmonic nanostructure, which serves as basic knowledge in the applications of nanoplasmonic materials.

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4

Pietroni, Massimo. "Plasmon Damping Rate forT→TC." Physical Review Letters 81, no. 12 (September 21, 1998): 2424–27. http://dx.doi.org/10.1103/physrevlett.81.2424.

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5

Witte, B. B. L., P. Sperling, M. French, V. Recoules, S. H. Glenzer, and R. Redmer. "Observations of non-linear plasmon damping in dense plasmas." Physics of Plasmas 25, no. 5 (May 2018): 056901. http://dx.doi.org/10.1063/1.5017889.

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6

Foerster, Benjamin, Vincent A. Spata, Emily A. Carter, Carsten Sönnichsen, and Stephan Link. "Plasmon damping depends on the chemical nature of the nanoparticle interface." Science Advances 5, no. 3 (March 2019): eaav0704. http://dx.doi.org/10.1126/sciadv.aav0704.

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The chemical nature of surface adsorbates affects the localized surface plasmon resonance of metal nanoparticles. However, classical electromagnetic simulations are blind to this effect, whereas experiments are typically plagued by ensemble averaging that also includes size and shape variations. In this work, we are able to isolate the contribution of surface adsorbates to the plasmon resonance by carefully selecting adsorbate isomers, using single-particle spectroscopy to obtain homogeneous linewidths, and comparing experimental results to high-level quantum mechanical calculations based on embedded correlated wavefunction theory. Our approach allows us to indisputably show that nanoparticle plasmons are influenced by the chemical nature of the adsorbates 1,7-dicarbadodecaborane(12)-1-thiol (M1) and 1,7-dicarbadodecaborane(12)-9-thiol (M9). These surface adsorbates induce inside the metal electric dipoles that act as additional scattering centers for plasmon dephasing. In contrast, charge transfer from the plasmon to adsorbates—the most widely suggested mechanism to date—does not play a role here.

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7

Kurasawa, Haruki, Kazuhiro Yabana, and Toshio Suzuki. "Damping width of the Mie plasmon." Physical Review B 56, no. 16 (October 15, 1997): R10063—R10066. http://dx.doi.org/10.1103/physrevb.56.r10063.

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8

Barlas, T. R., and N. L. Dmitruk. "Damping of Surface Plasmon–Phonon Polaritons." physica status solidi (b) 187, no. 1 (January 1, 1995): 109–15. http://dx.doi.org/10.1002/pssb.2221870110.

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9

Falkovsky, L. A. "Damping of coupled phonon-plasmon modes." Journal of Experimental and Theoretical Physics 96, no. 2 (February 2003): 335–39. http://dx.doi.org/10.1134/1.1560406.

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10

Кособукин, В. А. "Двумерные кулоновские плазмон-экситоны: релаксация возбуждений." Физика твердого тела 63, no. 8 (2021): 1157. http://dx.doi.org/10.21883/ftt.2021.08.51171.078.

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A theory is developed for the relaxation of two-dimensional non-radiative (Coulomb) plasmon-excitons in thin closely located layers of a metal and a semiconductor. In the framework of classical electrodynamics, the equations of motion are formulated for the polarization waves of non-radiative plasmons and excitons with taking into account the Coulomb coupling and the near-field of external polarization. In the model of coupled harmonic oscillators represented by the polarization fields of excitations, the problem of relaxation is solved for Coulomb plasmons, excitons and plasmon-excitons. It is shown that the two dispersion branches of normal plasmon-exciton modes undergo anticrossing (mutual repulsion) at the resonance between plasmon and exciton. With dissipative damping and power interchange between the excitations taken into account, the process of plasmon-exciton relaxation depending on time is investigated. The theory displays the principal analogies between dynamics of plasmon-excitons and of excitations in other objects of linear vibration theory, such as mechanical oscillators, resonant electric chains, etc.

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11

Lewandowski, Cyprian, and Leonid Levitov. "Intrinsically undamped plasmon modes in narrow electron bands." Proceedings of the National Academy of Sciences 116, no. 42 (September 27, 2019): 20869–74. http://dx.doi.org/10.1073/pnas.1909069116.

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Surface plasmons in 2-dimensional electron systems with narrow Bloch bands feature an interesting regime in which Landau damping (dissipation via electron–hole pair excitation) is completely quenched. This surprising behavior is made possible by strong coupling in narrow-band systems characterized by large values of the “fine structure” constant α=e2/ℏκvF. Dissipation quenching occurs when dispersing plasmon modes rise above the particle–hole continuum, extending into the forbidden energy gap that is free from particle–hole excitations. The effect is predicted to be prominent in moiré graphene, where at magic twist-angle values, flat bands feature α≫1. The extinction of Landau damping enhances spatial optical coherence. Speckle-like interference, arising in the presence of disorder scattering, can serve as a telltale signature of undamped plasmons directly accessible in near-field imaging experiments.

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12

Kluczyk, K., C. David, J. Jacak, and W. Jacak. "On Modeling of Plasmon-Induced Enhancement of the Efficiency of Solar Cells Modified by Metallic Nano-Particles." Nanomaterials 9, no. 1 (December 20, 2018): 3. http://dx.doi.org/10.3390/nano9010003.

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We demonstrate that the direct application of numerical packets like Comsol to plasmonic effect in solar cells metallically modified in nano-scale may be strongly inaccurate if quantum corrections are neglected. The near-field coupling of surface plasmons in metallic nanoparticles deposited on the top of a solar cell with band electrons in a semiconductor substrate strongly enhances the damping of plasmons in metallic components, which is not accounted for in standard numerical packets using the Drude type dielectric function for metal (taken from measurements in bulk or in thin layers) as the prerequisite for the numerical e-m field calculus. Inclusion of the proper corrections to plasmon damping causes additional enhancement of the plasmon-induced photo-effect efficiency growth of a metalized photo-diode by ten percent, at least, in comparison to only effect induced by the electric field concentration near metallic nanoparticles. This happens to be consistent with the experimental observations which cannot be explained by only local increases of the electrical field near the curvature of metallic nanoparticles determined by a finite-element solution of the Maxwell–Fresnel boundary problem as given by a numerical system like Comsol. The proper damping rate for plasmons can be identified by application of the Fermi Golden Rule approach to the plasmon-band electron coupling. We demonstrate this effect including the material and size dependence in two types of solar cells, multi-crystalline Si and CIGS (copper-indium-gallium-diselenide) as idealized photo-diode semiconductor substrate modified by various metallic nano-particles, in comparison to the experimental data and Comsol simulation.

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13

Mendonça, J. T., and R. Bingham. "Plasmon beam instability and plasmon Landau damping of ion acoustic waves." Physics of Plasmas 9, no. 6 (June 2002): 2604–8. http://dx.doi.org/10.1063/1.1479142.

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14

Gao, Yi, Zhe Yuan, and Shiwu Gao. "Semiclassical approach to plasmon–electron coupling and Landau damping of surface plasmons." Journal of Chemical Physics 134, no. 13 (April 7, 2011): 134702. http://dx.doi.org/10.1063/1.3575185.

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15

Melikyan, A., and H. Minassian. "On surface plasmon damping in metallic nanoparticles." Applied Physics B 78, no. 3-4 (February 2004): 453–55. http://dx.doi.org/10.1007/s00340-004-1403-z.

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16

Schinner, Andreas, Martina E. Bachlechner, and Helga M. Böhm. "Plasmon damping and proton stopping in jellium." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 93, no. 2 (July 1994): 181–85. http://dx.doi.org/10.1016/0168-583x(94)95685-5.

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17

Politano, A., V. Formoso, and G. Chiarello. "Dispersion and Damping of Gold Surface Plasmon." Plasmonics 3, no. 4 (October 10, 2008): 165–70. http://dx.doi.org/10.1007/s11468-008-9070-2.

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18

Lee, Stephen A., and Stephan Link. "Chemical Interface Damping of Surface Plasmon Resonances." Accounts of Chemical Research 54, no. 8 (March 31, 2021): 1950–60. http://dx.doi.org/10.1021/acs.accounts.0c00872.

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19

Moon, Seong Woo, Philippe Vuka Tsalu, and Ji Won Ha. "Single particle study: size and chemical effects on plasmon damping at the interface between adsorbate and anisotropic gold nanorods." Physical Chemistry Chemical Physics 20, no. 34 (2018): 22197–202. http://dx.doi.org/10.1039/c8cp03231a.

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20

Xu, Pengyu, Xuxing Lu, Junwei Zhao, Yue Li, Sheng Chen, Junfei Xue, Weihui Ou, Song Han, Yaping Ding, and Weihai Ni. "Metal Adsorbate-Induced Plasmon Damping in Gold Nanorods: The Difference Between Metals." Nano 11, no. 09 (September 2016): 1650099. http://dx.doi.org/10.1142/s1793292016500995.

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We presented a single particle study on the metal adsorbate-induced plasmon damping in Au nanorods (AuNRs) through adsorbing clusters of different metals including Pt, Au and Ag. AuNRs with different longitudinal surface plasmon resonance (LSPR) wavelength were measured and investigated individually. Linewidth broadening, plasmon shift and reduction of plasmonic resonance of single AuNRs were studied and compared between Pt, Au and Ag adsorbates. The measured linewidths perfectly match the theoretical predictions of the billiard model with increased scattering coefficients resulted from the metal adsorbates. The results indicate that the plasmon damping in case of Ag is significantly weaker than Pt and Au, which can be attributed to longer relaxation time of free electrons in Ag and therefore less loss of the oscillating plasmon electrons. In contrast to the red shift observed from Au and Pt, blue shift of the LSPR is observed in case of Ag. It suggests that plasmonic properties brought by the metal adsorbates can exert dramatic influence on the nanoparticle that is adsorbed with. We believe that our study not only provides important understanding on plasmon damping but pave the road for the fabrication of complex nanostructures with two or more metal elements.

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21

VASYLYEV, M. A., and V. A. TINKOV. "LOW ENERGY ELECTRON INDUCED PLASMON EXCITATIONS IN THE ORDERING Pt80Co20(111) ALLOY SURFACE." Surface Review and Letters 15, no. 05 (October 2008): 635–40. http://dx.doi.org/10.1142/s0218625x08011809.

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Surface and bulk plasmon excitations from the ordering Pt 80 Co 20(111) alloy surface are studied by means electron energy loss spectroscopy in the low energy range of the primary electron energy E0. Deviation of the plasmon excitations from the theoretical value was found for Pt , Co metals, and Pt 80 Co 20(111) alloy as calculated in the free-electron gas model. For the ordered alloy, the bulk plasmon energy is 2–3 eV more than for the disordered alloy, whereas the difference for surface plasmon energy is 4–7 eV in the range E0 = 150–800 eV. The ration of intensity lines of plasmons η from E0 was investigated for the (dis)ordered state of the Pt 80 Co 20(111) alloy surface. For the ordered alloy, η has prolonged dependence from energy E0 in comparison with the disordered alloy. The relationship between layer-by-layer surface concentration and surface plasmon damping was observed.

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22

Kumar, Manish, Jyotirban Dey, Mrigank Singh Verma, and Manabendra Chandra. "Nanoscale plasmon–exciton interaction: the role of radiation damping and mode-volume in determining coupling strength." Nanoscale 12, no. 21 (2020): 11612–18. http://dx.doi.org/10.1039/d0nr01303j.

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23

Wang, Xing-Yuan, Yi-Lun Wang, Suo Wang, Bo Li, Xiao-Wei Zhang, Lun Dai, and Ren-Min Ma. "Lasing Enhanced Surface Plasmon Resonance Sensing." Nanophotonics 6, no. 2 (March 1, 2017): 472–78. http://dx.doi.org/10.1515/nanoph-2016-0006.

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AbstractThe resonance phenomena of surface plasmons has enabled development of a novel class of noncontact, real-time and label-free optical sensors, which have emerged as a prominent tool in biochemical sensing and detection. However, various forms of surface plasmon resonances occur with natively strong non-radiative Drude damping that weakens the resonance and limits the sensing performance fundamentally. Here we experimentally demonstrate the first lasing-enhanced surface plasmon resonance (LESPR) refractive index sensor. The figure of merit (FOM) of intensity sensing is ~84,000, which is about 400 times higher than state-of-the-art surface plasmon resonance (SPR) sensor. We found that the high FOM originates from three unique features of LESPR sensors: high-quality factor, nearly zero background emission and the Gaussian-shaped lasing spectra. The LESPR sensors may form the basis for a novel class of plasmonic sensors with unprecedented performance for a broad range of applications.

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24

Markov, Yu A., and M. A. Markova. "Nonlinear plasmon damping in the quark-gluon plasma." Journal of Physics G: Nuclear and Particle Physics 26, no. 10 (September 21, 2000): 1581–619. http://dx.doi.org/10.1088/0954-3899/26/10/311.

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25

Liechtenstein, A. I., O. Gunnarsson, M. Knupfer, J. Fink, and J. F. Armbruster. "Plasmon damping and response function in doped compounds." Journal of Physics: Condensed Matter 8, no. 22 (May 27, 1996): 4001–16. http://dx.doi.org/10.1088/0953-8984/8/22/005.

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26

Kleinert, P. "Damping of Long-Wavelength Coupled Plasmon-Phonon Excitations." physica status solidi (b) 156, no. 1 (November 1, 1989): K41—K44. http://dx.doi.org/10.1002/pssb.2221560149.

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27

Rocca, M., Li Yibing, F. Buatier de Mongeot, and U. Valbusa. "Surface plasmon dispersion and damping on Ag(111)." Physical Review B 52, no. 20 (November 15, 1995): 14947–53. http://dx.doi.org/10.1103/physrevb.52.14947.

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28

Brodin, G., R. Ekman, and J. Zamanian. "Nonlinear wave damping due to multi-plasmon resonances." Plasma Physics and Controlled Fusion 60, no. 2 (December 14, 2017): 025009. http://dx.doi.org/10.1088/1361-6587/aa979d.

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29

Lee, Geunseop, P. T. Sprunger, and E. W. Plummer. "Surface plasmon dispersion and damping on Ag(110)." Surface Science Letters 286, no. 1-2 (April 1993): L547—L553. http://dx.doi.org/10.1016/0167-2584(93)90607-k.

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30

Lee, Geunseop, P. T. Sprunger, and E. W. Plummer. "Surface plasmon dispersion and damping on Ag(110)." Surface Science 286, no. 1-2 (April 1993): L547—L553. http://dx.doi.org/10.1016/0039-6028(93)90547-w.

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31

Khurgin, Jacob B. "Ultimate limit of field confinement by surface plasmon polaritons." Faraday Discussions 178 (2015): 109–22. http://dx.doi.org/10.1039/c4fd00193a.

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We show that electric field confinement in surface plasmon polaritons propagating at metal/dielectric interfaces enhances the loss due to Landau damping, which effectively limits the degree of confinement itself. We prove that Landau damping, and associated with it surface collision damping, follow directly from the Lindhard formula for the dielectric constant of a free electron gas. Furthermore, we demonstrate that even if all of the conventional loss mechanisms, caused by phonons, electron–electron interactions, and interface roughness scattering, were eliminated, the maximum attainable degree of confinement and the loss accompanying it would not change significantly compared to the best existing plasmonic materials, such as silver.

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32

Therrien, Andrew J., Matthew J. Kale, Lin Yuan, Chao Zhang, Naomi J. Halas, and Phillip Christopher. "Impact of chemical interface damping on surface plasmon dephasing." Faraday Discussions 214 (2019): 59–72. http://dx.doi.org/10.1039/c8fd00151k.

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33

Davoudi, B., and B. Tanatar. "Plasmon dispersion and damping in double-layer electron systems." Solid State Communications 117, no. 2 (December 2000): 89–92. http://dx.doi.org/10.1016/s0038-1098(00)00424-5.

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34

Zadoyan, R., H. Ye Seferyan, A. W. Wark, R. M. Corn, and V. A. Apkarian. "Interfacial Velocity-Dependent Plasmon Damping in Colloidal Metallic Nanoparticles." Journal of Physical Chemistry C 111, no. 29 (July 2007): 10836–40. http://dx.doi.org/10.1021/jp0715979.

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35

Veal, T. D., G. R. Bell, and C. F. McConville. "Plasmon damping in molecular beam epitaxial-grown InAs(100)." Journal of Vacuum Science & Technology B: Microelectronics and Nanometer Structures 20, no. 4 (2002): 1766. http://dx.doi.org/10.1116/1.1491541.

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36

Biagi, R., Carlo Mariani, and U. del Pennino. "Hole-plasmon damping on heavily dopedp-type GaAs(110)." Physical Review B 46, no. 4 (July 15, 1992): 2467–72. http://dx.doi.org/10.1103/physrevb.46.2467.

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37

Bachlechner, Martina E., Helga M. Böhm, and Andreas Schinner. "Screening effects on plasmon damping in an electron liquid." Physica B: Condensed Matter 183, no. 3 (March 1993): 293–302. http://dx.doi.org/10.1016/0921-4526(93)90040-d.

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38

Connolly, M. P., A. J. L. Ferguson, P. Dawson, I. R. Tamm, and D. G. Walmsley. "Fast mode surface plasmon damping on tunnel junction structures." Surface Science 245, no. 1-2 (April 1991): 225–31. http://dx.doi.org/10.1016/0039-6028(91)90481-7.

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39

Moon, Seong Woo, and Ji Won Ha. "Influence of the capping material on pyridine-induced chemical interface damping in single gold nanorods." Analyst 144, no. 8 (2019): 2679–83. http://dx.doi.org/10.1039/c9an00226j.

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40

Tserkezis, Christos, Wei Yan, Wenting Hsieh, Greg Sun, Jacob B. Khurgin, Martijn Wubs, and N. Asger Mortensen. "On the origin of nonlocal damping in plasmonic monomers and dimers." International Journal of Modern Physics B 31, no. 24 (September 30, 2017): 1740005. http://dx.doi.org/10.1142/s0217979217400057.

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The origin and importance of nonlocal damping is discussed through simulations with the generalized nonlocal optical response (GNOR) theory, in conjunction with time-dependent density functional theory (TDDFT) calculations and equivalent circuit modeling, for some of the most typical plasmonic architectures: metal–dielectric interfaces, metal–dielectric–metal gaps, spherical nanoparticles and nanoparticle dimers. It is shown that diffusive damping, as introduced by the convective–diffusive GNOR theory, describes well the enhanced losses and plasmon broadening predicted by ab initio calculations in few-nm particles or few-to-sub-nm gaps. Through the evaluation of a local effective dielectric function, it is shown that absorptive losses appear dominantly close to the metal surface, in agreement with TDDFT and the mechanism of Landau damping due to generation of electron–hole pairs near the interface. Diffusive nonlocal theories provide therefore an efficient means to tackle plasmon damping when electron tunneling can be safely disregarded, without the need to resort to more accurate, but time-consuming fully quantum-mechanical studies.

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41

Kim, Wan-Joong, JaeTae Seo, Chil Seong Ah, Jasmine Austin, Shanghee Kim, Ansoon Kim, Gun Yong Sung, and Wan Soo Yun. "Colorimetric Analysis on Flocculation of Bioinspired Au Self-Assembly for Biophotonic Application." Journal of Nanomaterials 2009 (2009): 1–6. http://dx.doi.org/10.1155/2009/261261.

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Gold nanoparticles exhibited strong surface plasmon absorption and couplings between neighboring particles within bioactivated self-assembly modified their optical properties. Colorimetric analysis on the optical modification of surface plasmon resoanance (SPR) shift and flocculation parameter functionalized bioinspired gold assembly for biophotonic application. The physical origin of bioinspired gold aggregation-induced shifting, decreasing, or broadening of the plasmon absorption spectra could be explained in terms of dynamic depolarization, collisional damping, and shadowing effects.

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42

Segui, Silvina, Juana L. Gervasoni, and Néstor R. Arista. "Plasmon damping in the free-electron gas model of solids." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 408 (October 2017): 217–22. http://dx.doi.org/10.1016/j.nimb.2017.05.046.

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43

Zolnai, Zsolt, Dániel Zámbó, Zoltán Osváth, Norbert Nagy, Miklós Fried, Attila Németh, Szilárd Pothorszky, Dániel Péter Szekrényes, and András Deák. "Gold Nanorod Plasmon Resonance Damping Effects on a Nanopatterned Substrate." Journal of Physical Chemistry C 122, no. 43 (October 15, 2018): 24941–48. http://dx.doi.org/10.1021/acs.jpcc.8b07521.

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44

Gabovich, A. M., V. M. Rozenbaum, and A. I. Voitenko. "Importance of the Plasmon Damping for the Dynamical Image Forces." physica status solidi (b) 214, no. 1 (July 1999): 29–33. http://dx.doi.org/10.1002/(sici)1521-3951(199907)214:1<29::aid-pssb29>3.0.co;2-g.

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45

Xu, Pengyu, Xuxing Lu, Song Han, Weihui Ou, Yue Li, Sheng Chen, Junfei Xue, Yaping Ding, and Weihai Ni. "Dispersive Plasmon Damping in Single Gold Nanorods by Platinum Adsorbates." Small 12, no. 36 (May 9, 2016): 5081–89. http://dx.doi.org/10.1002/smll.201600533.

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46

Laitenberger, P., and R. E. Palmer. "Plasmon Dispersion and Damping at the Surface of a Semimetal." Physical Review Letters 76, no. 11 (March 11, 1996): 1952–55. http://dx.doi.org/10.1103/physrevlett.76.1952.

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47

Bachlechner, Martina E., Helga M. Böhm, and Andreas Schinner. "Long wavelength plasmon damping in the two-dimensional electron gas." Physics Letters A 178, no. 1-2 (July 1993): 186–91. http://dx.doi.org/10.1016/0375-9601(93)90749-p.

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48

Nguyen-Truong, Hieu T. "Energy-loss function including damping and prediction of plasmon lifetime." Journal of Electron Spectroscopy and Related Phenomena 193 (March 2014): 79–85. http://dx.doi.org/10.1016/j.elspec.2014.03.010.

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49

Abid, I., P. Benzo, B. Pécassou, S. Jia, J. Zhang, J. Yuan, J. B. Dory, et al. "Plasmon damping and charge transfer pathways in Au@MoSe2 nanostructures." Materials Today Nano 15 (August 2021): 100131. http://dx.doi.org/10.1016/j.mtnano.2021.100131.

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50

Kolwas, Krystyna. "Decay Dynamics of Localized Surface Plasmons: Damping of Coherences and Populations of the Oscillatory Plasmon Modes." Plasmonics 14, no. 6 (May 17, 2019): 1629–37. http://dx.doi.org/10.1007/s11468-019-00958-1.

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