2009
DOI: 10.1364/ao.48.00b183
|View full text |Cite
|
Sign up to set email alerts
|

Evanescent field sensors and the implementation of waveguiding nanostructures

Abstract: Conventional fiber optic evanescent-field gas sensors are based on a high number of total reflections while the gas is passing the active bare core fiber and of course a suitable laser light source. The use of miniaturized laser sources for sensitive detection of CO(2) in gaseous and water-dissolved phase for environmental monitoring are studied for signal enhancing purposes. Additionally, the fiber optic sensor, consisting of a coiled bare multimode fiber core, was sensitized by an active polymer coating for … Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
9
0
1

Year Published

2011
2011
2019
2019

Publication Types

Select...
6
2
1

Relationship

3
6

Authors

Journals

citations
Cited by 22 publications
(11 citation statements)
references
References 12 publications
0
9
0
1
Order By: Relevance
“…The confinement of light is governed by the principle of total internal reflection at the interface between media with different indices of refraction. 8 As light propagates within the semiconductor waveguide, it undergoes total internal reflection if the angle of incidence is above a certain critical angle Θ c (determined by the ratio of the refractive indices by sin Θ c ¼ n 2 ∕n 1 ). Here, n 1 is the refractive index of the waveguide and n 2 is the refractive index of the medium above the waveguide.…”
Section: Fundamentals Of Pic-based Optical Sensingmentioning
confidence: 99%
See 1 more Smart Citation
“…The confinement of light is governed by the principle of total internal reflection at the interface between media with different indices of refraction. 8 As light propagates within the semiconductor waveguide, it undergoes total internal reflection if the angle of incidence is above a certain critical angle Θ c (determined by the ratio of the refractive indices by sin Θ c ¼ n 2 ∕n 1 ). Here, n 1 is the refractive index of the waveguide and n 2 is the refractive index of the medium above the waveguide.…”
Section: Fundamentals Of Pic-based Optical Sensingmentioning
confidence: 99%
“…9,10 The total absorption for an analyte maximally proved by the evanescent field, described by the Beer-Lambert Law, − ln IðλÞ I 0 ðλÞ ¼ aðλÞCL, can then be used to calculate the concentration (C) of the analyte, where I 0 is the input intensity, I is the transmitted intensity, aðλÞ is the wavelength-dependent attenuation coefficient, and L is the length of the sensing region. 8 Evident here is that sensor performance is determined not only by the analyte and its interaction strength with its receptor, but also by the physical design of the sensor, which determines the total analyte-light interaction (i.e., the length of the devices, the strength of the evanescent field, and its overlap with the optical cross section of the analyte).…”
Section: Fundamentals Of Pic-based Optical Sensingmentioning
confidence: 99%
“…The principle of these sensors is based on total internal reflection at the interface between two media with different refraction indexes [14]. When the incident angle is above the critical angle, light travelling through the high refractive index waveguide undergoes total internal reflection and most of the energy is confined within the high refractive index waveguide core.…”
Section: Theoretical Descriptionmentioning
confidence: 99%
“…2 strongly depends on the performance of the polymer sensory film for several reasons. First, since the film for the proposed LOF platform extends for only a very short distance, from one to several millimeters, signal accumulation through a long fiber segment [6], [7] is out of the question. A sufficiently high quantum yield is thus fundamental, and will also assist in reducing photo-bleaching of the polymer caused by high Ex power density.…”
Section: A Impact Of the Performance Of The Sensory Polymer Filmmentioning
confidence: 99%