1982
DOI: 10.1021/j100223a007
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Use of a perfectly conducting sphere to excite the plasmon of a flat surface. 1. Calculation of the local field with applications to surface-enhanced spectroscopy

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Cited by 93 publications
(96 citation statements)
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“…29,30 In the case of the plasmonic nanoparticles, it has been shown that "hot spots" are naturally generated in the aggregation process, which enhances the plasmon coupling interactions. Theoretical studies 31 support the conclusion that the "hot spots" are localized in the region between two interacting nanoparticles where the electric field is strongly intensified under the influence of the longitudinal plasmon resonance, which, on the other hand, is responsible for the red shifted coupling band. The electric field in the "hot spot" region depends on the direction of the electric dipole vector of the electromagnetic radiation relative to the interparticle axis, reaching the maximum when the polarization vector is parallel to this axis ( Figure 4).…”
Section: Plasmon Resonance and Serssupporting
confidence: 48%
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“…29,30 In the case of the plasmonic nanoparticles, it has been shown that "hot spots" are naturally generated in the aggregation process, which enhances the plasmon coupling interactions. Theoretical studies 31 support the conclusion that the "hot spots" are localized in the region between two interacting nanoparticles where the electric field is strongly intensified under the influence of the longitudinal plasmon resonance, which, on the other hand, is responsible for the red shifted coupling band. The electric field in the "hot spot" region depends on the direction of the electric dipole vector of the electromagnetic radiation relative to the interparticle axis, reaching the maximum when the polarization vector is parallel to this axis ( Figure 4).…”
Section: Plasmon Resonance and Serssupporting
confidence: 48%
“…The electric field in the "hot spot" region depends on the direction of the electric dipole vector of the electromagnetic radiation relative to the interparticle axis, reaching the maximum when the polarization vector is parallel to this axis ( Figure 4). 31 Another important aspect is that the metal-adsorbate structure permits new excitations, such as the chargetransfer (CT) transitions from the Fermi level (E F ) to the lowest unnoccupied molecular orbitals of the molecule (E F →LUMO) or from the highest occupied molecular orbital to E F (HOMO→E F ). When the excitation is in resonance with the electronic transition in the metaladsorbate complex, the surface-enhanced Raman scattering can also incorporate this type of metal-molecule chargetransfer mechanism, as originally proposed by Otto et al 32 Usually, the Fermi level for metals (e.g., -4.3 eV for Ag) lies above the HOMO of most molecules (e.g., -9.26 eV for pyridine), and lower than their LUMO level.…”
Section: Plasmon Resonance and Sersmentioning
confidence: 99%
“…[7][8][9][10][11] Since the magnitude of EM enhancement and the resonance wavelength are controllable with the dimer geometry, metallic dimers are considered as a good candidate of well-defined hot spots. Indeed, we have already reported that the metallic nanodimer arrays, which were fabricated with an angle-resolved nanosphere lithography ͑AR-NSL͒ technique, 12 exhibited anisotropic and enormous enhancement of the SERS cross section.…”
mentioning
confidence: 99%
“…[ [39][40][41] For the complex RhCl 3 (C 6 H 5 SCH 3 ) 3 . Three strong bands at 337cm -1 , 320cm -1 and at 293cm This decrease is due to the fact that the OCH 3 group at para position behaves as a strong electron releasing one here the resonance effect outweighs the electron -with drawing inductive effect and the -OCH 3 group has a net electron-releasing tendency to the benzene ring, and so the v(Rh-S) stretching frequency is decreased to a lower region than that of the A similar observation is made in NMR studies of some substituted phenyl methyl sulphides.…”
Section: Electronic Spectra Of Complexesmentioning
confidence: 99%