2014
DOI: 10.1103/physreva.90.013421
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Geometric tailoring of plasmonic nanotips for atom traps

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Cited by 5 publications
(3 citation statements)
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“…Ref. [26]. For a refractive index of CdS at 1064 nm of n CdS = 2.344 we arrive at a polarizability α = 5.28 · 10 −35 Cm 2 /V.…”
Section: Concept Of a Deep Parabolic Mirror Dipole Trapmentioning
confidence: 92%
“…Ref. [26]. For a refractive index of CdS at 1064 nm of n CdS = 2.344 we arrive at a polarizability α = 5.28 · 10 −35 Cm 2 /V.…”
Section: Concept Of a Deep Parabolic Mirror Dipole Trapmentioning
confidence: 92%
“…The physical mechanism described in this paper can be applied to any statistical ensemble of emitters in a nanoscale volume. However, the specific system which we have in mind is that of an optical fiber which is tapered down at one of its ends to a nanotip in order to increase interactions with dipole emitters nearby the tip [13][14][15][16]. We assume the tip is immersed into a gas of cold atoms with number density ρ, and a classical light field emerging from the fiber end excites atoms in a small volume V in front of its apex, figure 1.…”
Section: Light Statistics Of Ensemblesmentioning
confidence: 99%
“…Consequently, a variation of geometry structures like nanotip, nanocavity, nano-bowtie, and nanopillar have been widely investigated for generating the localized surface plasmon modes for nanoscale particle trapping purposes [9][10][11][12][13]. Amongst them, the hybrid nanotip in particular exhibits great potential for flexibly controlling plasmon nanofocusing for nanoparticle trapping applications due to the intrinsic merit of a highly directional hotspot, as generated from the nanotip geometry [14][15][16][17][18].…”
Section: Introductionmentioning
confidence: 99%