Tagged: Most Read

Reinhard Article Among Ten Most Read in February

April 27th, 2012 in Front Page, Publications, Reinhard, Björn

Professor Bjoern Reinhard

Professor Bjoern Reinhard

The article by Bjoern Reinhard, “Molding the flow of light on the nanoscale: from vortex nanogears to phase-operated plasmonic machinery” (Nanoscale, 2012, 4, 76-90; DOI: 10.1039/C1NR11406A), was amongst the top ten accessed articles from the online version of Nanoscale in February 2012. Launched in 2009, Nanoscale is a new peer reviewed journal publishing experimental and theoretical work across the breadth of nanoscience and nanotechnology.

The Reinhard Group research focuses on new optical materials and their application to interrogate fundamental life processes. They explore the interface between nanotechnology and biological systems. For an overview of current research projects, please visit their group’s website.

Plasmonic nanolens as an internal vortex nanogear transmission. (a) Schematic of the self-similar Ag nanolens proposed in ref 72 (r1 = 45 nm, r2 = 15 nm, r3 = 5 nm, d1 = 9 nm, d2 = 3 nm, ambient index n = 1.0). (b and c) Electric field intensity distribution in the nanolens illuminated on- (b) and off-resonance (c) with the near-field intensity maximum of the nanolens. Far-field (d) and near-field intensity enhancement (e) spectra of the nanolens. (f) The amplitude of the Poynting vector and the phase of the Poynting vector in the x–z plane at the center of the nanolens narrower interparticle gap as a function of wavelength. (g and h) Poynting vector intensity distribution and powerflow around the nanolens off (g) and on (h) the peak intensity wavelength. (i) Schematic of the VNT generated in the nanolens at the peak intensity resonance. Light flux in each nanogear is looped through nanoparticles .

Plasmonic nanolens as an internal vortex nanogear transmission. (a) Schematic of the self-similar Ag nanolens proposed in ref 72 (r1 = 45 nm, r2 = 15 nm, r3 = 5 nm, d1 = 9 nm, d2 = 3 nm, ambient index n = 1.0). (b and c) Electric field intensity distribution in the nanolens illuminated on- (b) and off-resonance (c) with the near-field intensity maximum of the nanolens. Far-field (d) and near-field intensity enhancement (e) spectra of the nanolens. (f) The amplitude of the Poynting vector and the phase of the Poynting vector in the x–z plane at the center of the nanolens narrower interparticle gap as a function of wavelength. (g and h) Poynting vector intensity distribution and powerflow around the nanolens off (g) and on (h) the peak intensity wavelength. (i) Schematic of the VNT generated in the nanolens at the peak intensity resonance. Light flux in each nanogear is looped through nanoparticles .

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