DocumentCode :
1916226
Title :
Flexible optical microcavities and their sensing application
Author :
Ta, V.D. ; Chen, Ru Shan ; Nguyen, D.M. ; Sun, H.D.
Author_Institution :
Sch. of Math. & Phys. Sci., Nanyang Technol. Univ., Singapore, Singapore
fYear :
2013
fDate :
12-16 May 2013
Firstpage :
1
Lastpage :
1
Abstract :
Summary form only given. Due to high quality factor and small mode volume, optical whispering gallery microcavities have been employed for fundamental studies of light-matter interaction and significant applications such as low-threshold laser devices, dynamic filters [1], and recently label-free ultra-sensitive biosensors [2]. Here, we demonstrate a novel material composition together with effective methods to fabricate two different high quality microresonators namely microfibers and hemispheres. By incorporating dye molecules in these structures, optically pumped whispering gallery mode (WGM) laser was observed. Moreover, the microlasers can be used as high sensitive refractive index sensors. Microfibers are readily obtained by directly drawing from a mixture of epoxy resin and polymethylmethacrylate (PMMA) as shown in Figure 1(a) [3]. The weight ratio of PMMA and epoxy was about 1: 2. Figure 1(b) shows a scanning electron microscope (SEM) image of dye doped microfiber with a high uniformity and smooth outer surface. Interestingly, by changing the ratio to 1: 6 and placed the fabricated fiber on a hydrophobic distributed Bragg reflector (DBR), hemispheres are self-assembly because the fiber “want” to minimize its surface area as shown in Figure 1(c) [4]. To achieve lasing emission, pulse Nd:YAG laser (wavelength: 532 nm, pulse duration: 1 ns, repetition rate: 60 Hz) was used to excite individual microfiber or hemisphere and the photoluminescence (PL) was recorded by a charge-coupled device (CCD). Figure 1(d) and (e) show lasing spectra from a Rhodamine 6G (R6G) doped fiber and Rhodamine B (RhB) doped hemisphere, respectively. Positions of the lasing modes can be well-explained by WGM theory. In principle, if refractive index of the medium surrounding a cavity changes, spectral shift of resonant modes will be observed and the shifting value is a function of refractive index unit (RIU) [2]. Based on this phenomenon the fiber and hemisphere was used- for refractive index sensing of Tetrahydrofuran (THF) solution and acetone vapour with sensitivity around 300 and 130 nm/RIU, respectively [3,4]. In conclusion, we provide a new material composition and an effective technique to fabricate fiber and hemispherical microlasers, and demonstrate their potential application as sensitive optical sensors, which is important for developing of flexible photonic devices.
Keywords :
distributed Bragg reflector lasers; dyes; fibre lasers; fibre optic sensors; laser modes; measurement by laser beam; microcavities; microcavity lasers; optical fibre fabrication; optical fibre filters; optical polymers; optical pumping; optical resonators; photoluminescence; refractive index; resins; scanning electron microscopy; self-assembly; whispering gallery modes; CCD; DBR; PMMA; RIU; Rhodamine 6G doped fiber; Rhodamine B doped hemisphere; THF; Tetrahydrofuran solution; WGM theory; acetone vapour; charge-coupled device; dye doped microfiber; dye molecules; dynamic filters; epoxy resin; fiber microlaser fabrication; flexible optical microcavities; flexible photonic devices; hemispherical microlasers; high quality factor; high quality microresonators; high sensitive refractive index sensors; high uniformity surface; hydrophobic distributed Bragg reflector; individual microfiber; label-free ultrasensitive biosensors; lasing emission; lasing mode positions; lasing spectra; light-matter interaction; low-threshold laser devices; material composition; optical whispering gallery microcavities; optically pumped whispering gallery mode laser; photoluminescence; polymethylmethacrylate; pulse Nd:YAG laser; refractive index unit; resonant mode; scanning electron microscope; self-assembly; sensitive optical sensors; shifting value; small mode volume; smooth outer surface; spectral shift; surface area; time 1 ns; wavelength 130 nm; wavelength 300 nm; wavelength 532 nm; weight ratio; Biomedical optical imaging; Optical fiber sensors; Optical fiber theory;
fLanguage :
English
Publisher :
ieee
Conference_Titel :
Lasers and Electro-Optics Europe (CLEO EUROPE/IQEC), 2013 Conference on and International Quantum Electronics Conference
Conference_Location :
Munich
Print_ISBN :
978-1-4799-0593-5
Type :
conf
DOI :
10.1109/CLEOE-IQEC.2013.6800977
Filename :
6800977
Link To Document :
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