2016
DOI: 10.1103/physreva.93.033831
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Radiative decay of a quantum emitter placed near a metal-dielectric lamellar nanostructure: Fundamental constraints

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Cited by 12 publications
(12 citation statements)
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“…Chen et al [18] nu mer i cally in ves ti gated op ti cal re sponses of deep slits at trans verse mag netic by us ing rig or ous cou pled-wave anal y sis and found that the op ti cal re sponse was much dif fer ent for slits with dif fer ent at tached fea tures. Klimov et al [19] re ported on the fun da men tal con straints per tain ing to the en hance ment of the ra di a tive emis sion rate achiev able with pla nar lamellar metamaterials of any kind. Zheng [20] fo cused on a meth od ol ogy about ad just ing the wave length se lec tiv ity of thin films em bed ded with nanoparticles.…”
Section: Introductionmentioning
confidence: 99%
“…Chen et al [18] nu mer i cally in ves ti gated op ti cal re sponses of deep slits at trans verse mag netic by us ing rig or ous cou pled-wave anal y sis and found that the op ti cal re sponse was much dif fer ent for slits with dif fer ent at tached fea tures. Klimov et al [19] re ported on the fun da men tal con straints per tain ing to the en hance ment of the ra di a tive emis sion rate achiev able with pla nar lamellar metamaterials of any kind. Zheng [20] fo cused on a meth od ol ogy about ad just ing the wave length se lec tiv ity of thin films em bed ded with nanoparticles.…”
Section: Introductionmentioning
confidence: 99%
“…In recent times, such couplings have been experimentally realized on various systems such as metal‐integrated semiconductor nanowires, [ 1 ] metal‐coated dielectric structures, [ 2 ] microsphere coupled with metallic particles, [ 3 ] dielectric nanospheres placed near metallic film. [ 4,5 ] These hybrid structures have been utilized, to design single photon devices, [ 6–8 ] optical antenna, [ 9,10 ] to tune the photoluminescence dynamics of emitters [ 11,12 ] and for enhanced spontaneous emission from emitters [ 13–15 ] down to the level of single molecule with minimized ohmic losses. [ 16,17 ]…”
Section: Figurementioning
confidence: 99%
“…When the molecule is close to the surface of the metal ( 0 z D < ), the significant contribution to the total spontaneous decay rate is due to the nonradiative channel. If the molecule remoteness is more than D, the influence of the hole on the molecular emission becomes weak, and the approach «the molecule near the metal film without a hole» stats to work well [27,31]. At a distance of more than 4D, the total spontaneous decay rate of the molecule can be described right by the asymptotic «molecule near a perfectly conducting screen without a hole» [24,28,29].…”
Section: Molecule Located Nearmentioning
confidence: 99%
“…In this section, the thickness of the metal layer h is 80 nm. We have chosen such thickness for comparison with the study of radiative decay rates enhancement due to «leaky» surface plasmon waves in a multilayer structure without a hole [31]. Fig.…”
Section: Placed On a Dielectric Substratementioning
confidence: 99%
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