Fiber-loop ring-down spectroscopy: A sensitive absorption technique for small liquid samples
2003; American Institute of Physics; Volume: 74; Issue: 11 Linguagem: Inglês
10.1063/1.1614877
ISSN1527-2400
AutoresZhaoguo Tong, Michael B. Jakubinek, Alexander Wright, Alison Gillies, Hans‐Peter Loock,
Tópico(s)Laser Design and Applications
ResumoCavity ring-down spectroscopy has proven to be a very sensitive gas-phase spectroscopic technique, suitable to record either very weak transitions of abundant gases or stronger transitions of trace gases. Here, an adaptation of the ring-down measurement principle to optical waveguides is presented. Fiber-loop ring-down spectroscopy (FLRDS) allows for the measurement of absorption spectra of minute quantities of liquid solutions. An optical fiber is wound into a loop using a fiber splice connector. A nanosecond laser light pulse (λ∼810 nm) is coupled into the loop and the light pulses are detected using a photomultiplier detector. It is found that once the light is coupled into the fiber it experiences very little loss and the light pulses do a large number of round trips before their intensity is below the detection threshold. The characteristic ring-down time is obtained by exponential fitting of the envelope of the wave form. This method is well suited to characterize low-loss processes in fiber optic transmission independent from power fluctuations of the light source. The strengths of the technique are demonstrated by characterization of a variety of loss processes—in particular by the measurement of the absolute loss of the optical fiber and of the fiber connector, losses due to macrobending of a section of the fiber loop, as well as losses due to lateral and longitudinal displacement in the fiber–fiber connection. Furthermore, it is shown that FLRDS is useful as an absorption spectroscopic technique for very small sample volumes and may be applied as an absorption detection method in analytical chemistry devices. A crude 47 μm channel in polydimethylsiloxane polymer was fabricated between the fiber end facets and the dye 1,1′-diethyl-4,4′-dicarbocyanine iodide (DDCI) was introduced into the channel. From the concentration dependence of ring-down time the sample volume was determined as 700 pL and the detection limit as about 10−10 mol, or 7×10−8 g of DDCI.
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