2008 IEEE International RF and Microwave Conference 2008
DOI: 10.1109/rfm.2008.4897467
|View full text |Cite
|
Sign up to set email alerts
|

A simple analytical solution for loss in S-bend optical waveguide

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

1
4
0

Year Published

2016
2016
2022
2022

Publication Types

Select...
5
1
1

Relationship

0
7

Authors

Journals

citations
Cited by 9 publications
(5 citation statements)
references
References 10 publications
1
4
0
Order By: Relevance
“…Bending losses for conventional S bend waveguides (half a cosine function) depend most strongly on the change of curvature56. We therefore plot total power transmission (calculated by integrating the real part of the Poynting vector of the output light directly across the required area, and dividing it by the source power) up to a wavelength away from the myelin sheath boundaries (see Methods and Supplementary Information) as a function of the change of curvature, Δ κ  = 4 Ak 2 ( k is the wavenumber of the sinusoidal function) for 3 different wavelengths in Fig.…”
Section: Resultsmentioning
confidence: 99%
“…Bending losses for conventional S bend waveguides (half a cosine function) depend most strongly on the change of curvature56. We therefore plot total power transmission (calculated by integrating the real part of the Poynting vector of the output light directly across the required area, and dividing it by the source power) up to a wavelength away from the myelin sheath boundaries (see Methods and Supplementary Information) as a function of the change of curvature, Δ κ  = 4 Ak 2 ( k is the wavenumber of the sinusoidal function) for 3 different wavelengths in Fig.…”
Section: Resultsmentioning
confidence: 99%
“…3b shows the EFPL as a straight-mode passes through. Bending losses for conventional S bend waveguides (half a cosine function) depend most strongly on the change of curvature [52]. We therefore plot total power transmission (calculated by integrating the real part of the Poynting vector of the output light directly across the required area, and dividing it by the source power) up to a wavelength away from the myelin sheath boundaries (see Methods and Supplementary Information) as a function of the change of curvature, ∆κ = 4Ak 2 (k is the wavenumber of the sinusoidal function) for 3 different wavelengths in Fig.…”
Section: Resultsmentioning
confidence: 99%
“…This demonstrates declining length requirements for equivalent loss when S-bend structures with larger widths are required. This relationship in S-bend builds has been observed by previous authors [31,88]. Raised-sine S-bends are preferred as the S-bend design of choice when WGs exhibit low propagation loss (< 1 dB/cm).…”
Section: S-bend Foot-print Requirementssupporting
confidence: 78%