Chalcogenide double index fibers: fabrication, design, and application as a chemical sensor
Introduction
Chalcogenide glasses are based on the chalcogen elements, such as S, Se, and Te, and the addition of other elements, such as Ge, As, and Sb, that facilitate the formation of stable glasses [1]. This category of glasses shows the tendency to transmit the mid-infrared (IR) light due to their low phonon energy associates with the combinations of heavy elements. Moreover, the addition of halogens X (Cl, Br, I) in some compositions increases the transmitting window, which can extend from 2 to 20 μm in case of few millimeters thick samples [2].
Among the numerous chalcogenide glassy systems, we have selected the Te–As–Se based compositions, called TAS glasses. They have favorable viscosity–temperature dependence near the drawing temperature that allows fabrication of optical fibers with a special design. In the form of fibers, the spectral transparency of these glasses lies approximately from 2 to 12 μm. This wavelength region is particularly attractive for optical sensing because it contains the IR fingerprints of the chemical and biological molecules. Based on the general concept of Fiber Evanescent Wave Spectroscopy (FEWS) [3], [4], [5], the use of fibers allows remote, sensitive, and in situ measurements of the IR fingerprints. Our chalcogenide fibers are very suitable candidates for such spectroscopy in the mid-IR [6]. Until now, a single index fiber was used as sensor and as waveguide. It has been demonstrated that the sensitivity is greatly improved using a tapered fiber [6]. On one hand, these fibers have a large diameter, greater than 400 μm, to allow the transmission of the maximum IR light from the source (black body) until the detector (Hg–Cd–Te), and, on the other hand, on a short length of a few centimeters corresponding to the sensing zone, the diameter must be as thin as possible, i.e. smaller than 100 μm. This goal is achieved using a chemical etching solution to locally and congruently dissolve the TAS glass [7].
In this paper, we will describe the first FEWS experiments carried out with double index chalcogenide fibers. To record such spectra, we have to dissolve up the cladding glass at the level of the sensing zone. The use of core/cladding fibers as sensor will be doubly interesting. Firstly, going towards single mode fiber should greatly improve the sensitivity of the sensor. Secondly, these fibers isolate the core, where the light propagates, from the coating polymer, which surround the cladding. The polymer makes the sensor easier to handle by improving its mechanical behavior and increasing its flexibility. But the consequence with a single mode fiber is the presence of the polymer absorption band on the FEWS spectra. The use of double index fiber avoids these artifacts. The first part of the article is devoted to the double index TAS fiber fabrication by a new method and to the implementation of the sensing zone design. Secondly, the IR spectroscopy experiments carried out with these core/cladding fibers are shown and discussed.
Section snippets
Chalcogenide glass preform fabrication
At the present time, double index chalcogenide glass fibers are made from the double crucible method [8] or preforms, which are elaborated by rod-in-tube [9] or extrusion [10] methods. An original procedure, based on the build-in-casting method in a sealed silica ampoule, has been investigated to fabricate chalcogenide preform [11].
The first step consists in preparing separately each glass from high purity elements as described in a previous paper [12]. The core and cladding glass compositions
Fiber characterizations
This new technique allows to obtain preforms with different core/cladding diameter ratios versus the following parameters: dimensions (diameter and length) of the silica tube where the preform casting is operated, time of quenching. The ratios may vary between 0.25 and 0.75 and they appear to remain constant along the preform. The preforms are drawn into fibers that present a good core/cladding interface and a good co-centering of core and cladding (Fig. 3). The optical losses, shown in Fig. 4,
Conclusion
IR spectra have been collected with the help of double index chalcogenide fibers manufactured by a new method. The technique is based on the build-in-casting method and is achieved in a sealed silica ampoule. The fiber shows a very good quality of core/cladding interface and its minimum of optical losses is about 1.7 dB/m between 6.5 and 9.5 μm. These fibers have been used as chemical sensors, after a mechanical and chemical treatment to remove the cladding and to reduce the diameter of the probe
References (19)
- et al.
J. Non-Cryst. Solids
(1990) - et al.
J. Non-Cryst. Solids
(2000) - et al.
Int. J. Inorg. Mater.
(2001) - et al.
J. Non-Cryst. Solids
(1999) - et al.
J. Non-Cryst. Solids
(1997) - et al.
J. Non-Cryst. Solids
(1999) - et al.
J. Non-Cryst. Solids
(1993) - et al.
J. Non-Cryst. Solids
(1993) - et al.
J. Non-Cryst. Solids
(2001)
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