2010
DOI: 10.1103/physrevb.81.125431
|View full text |Cite
|
Sign up to set email alerts
|

Finite-element modeling of spontaneous emission of a quantum emitter at nanoscale proximity to plasmonic waveguides

Abstract: We develop a self-consistent finite element method to study spontaneous emission at nanoscale proximity of plasmonic waveguides. In the model, it is assumed that only one guided mode is dominatingly excited by the quantum emitter. With such one dominating mode assumption, the cross section of the plasmonic waveguide can be arbitrary. We apply our numerical method to calculate the coupling of a quantum emitter to a cylindrical nanowire and a rectangular waveguide, and compare the cylindrical nanowire to previou… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

7
145
0
1

Year Published

2011
2011
2021
2021

Publication Types

Select...
9

Relationship

2
7

Authors

Journals

citations
Cited by 131 publications
(153 citation statements)
references
References 50 publications
(77 reference statements)
7
145
0
1
Order By: Relevance
“…We compute the EM field excited by the dipole source with the finite element method (FEM) 62,63 using commercial software (COMSOL). The point dipole is modeled as a linear harmonic current of length l, intensity I 0 , and orientation given by the unit vector n. The associated dipole moment 63 is d = (iI 0 l/ω)n and, to satisfy the dipole approximation, the length l is kept very short in comparison with the emission wavelength (l = λ/330). To model infinitely long PWs, the spatial domain of interest is properly terminated with perfect matching layers that absorb the outgoing electromagnetic waves with negligible reflection.…”
Section: A Purcell Factormentioning
confidence: 99%
See 1 more Smart Citation
“…We compute the EM field excited by the dipole source with the finite element method (FEM) 62,63 using commercial software (COMSOL). The point dipole is modeled as a linear harmonic current of length l, intensity I 0 , and orientation given by the unit vector n. The associated dipole moment 63 is d = (iI 0 l/ω)n and, to satisfy the dipole approximation, the length l is kept very short in comparison with the emission wavelength (l = λ/330). To model infinitely long PWs, the spatial domain of interest is properly terminated with perfect matching layers that absorb the outgoing electromagnetic waves with negligible reflection.…”
Section: A Purcell Factormentioning
confidence: 99%
“…63,64 It is thus customary to express the total decay rate as the sum of those three contributions, γ = γ r + γ nr + γ pl . The photons absorbed in the metal and most photons radiated to vacuum do presumably not contribute to the qubit-qubit coupling.…”
Section: B β Factormentioning
confidence: 99%
“…Recent progress in nanophotonics and nanotechnology opens possibilities of engineering LDOS at nanometer scale and at highly advanced levels to achieve directional emission or enhanced light-matter interaction. [7][8][9][10][11][12][13][14] Such a nanophotonic approach has been applied to light emitting devices. [15][16][17][18][19][20][21][22]24,25 The rationale behind is that the transfer of energy from carriers in GaInN QW into localized optical plasmon supported by the metallic nanostructures will create an a afad@fotonik.dtu.…”
Section: Introductionmentioning
confidence: 99%
“…1, k has been calculated numerically using a full-vectorial finite element method [17], for a embedded point emitter. When this emitter is located on the wire axis, Fig.…”
mentioning
confidence: 99%