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FIBEROPTIC SENSOR TECHNOLOGY HANDBOOK

FIBEROPTIC SENSOR TECHNOLOGY HANDBOOK

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fibers are cleaned carefully after removing the jacket.<br />

Then they are twisted together and while remaining<br />

twisted they are etched to remove most of the cladding,<br />

leaving approximately one or two microns of cladding<br />

around the core. The diameters of the fibers after<br />

etching are less than 10% of their initial diameters,<br />

therefore the resulting sections of fibers are quite<br />

fragile. The joint IS held fixed (ruggedized) by either<br />

potting in an indexmatching material or by fusing under<br />

an axial tension that prevents the fiber from sagging<br />

due to gravity and at the same time stretches the fiber<br />

slightly, thus forming a biconical taper. This is shown<br />

in Fig. 3.20 on the right. Index matching silicone<br />

liquids have been proven to be highly temperature dependent.<br />

Better results are obtained with index-matching<br />

silicone rubber. However, there is still a temperaturedependence<br />

problem. A great deal of success has been<br />

achieved recently using a gel glass material (see Ref.<br />

2 in Subsection 3.2.1) that is initially in liquid form.<br />

This material consists of metal oxides dissolved in an<br />

organic material. When heated the organic material is<br />

driven off and the metal oxides form a glass. The refractive<br />

index of the resulting glasa, and therefore<br />

the degree of coupling, can be controlled by adjusting<br />

the temperature and the length of time utilized to cure<br />

or form the gel glass.<br />

Temperature dependence can be minimized if<br />

the fibers are actually fused. The biconical taper<br />

arrangement mentioned above is shown in Fig. 3.21. To<br />

aturized bulk optical components similar to the laboratory<br />

devices shown in Figs 3.16, 3.17, and 3.18. These<br />

bulk components and fibers may be connected by various<br />

means, such as GRIN rods.<br />

Using similar techniques star couplers have<br />

been fabricated that allow the light from one fiber to<br />

be coupled equally into as many as 32 other fibers.<br />

Such devices would be useful for permitting a single<br />

optical source to simultaneously furnish optical power<br />

to a number of sensors.<br />

In summary, satisfactory techniques now exist<br />

for forming low-loss singlemode splices and remountable<br />

connectors and for fabricating low insertion loss<br />

singlemode couplers. Recently, commercially available<br />

remountable connectors have appeared on the market.<br />

Singlemode biconical tapered couplera are also becoming<br />

available. Several other types of couplers are under<br />

development by a number of groups and thus can be expected<br />

to appear on the market in the near future.<br />

3.2.1 References<br />

1.<br />

2.<br />

3.<br />

S. Sheem, Appl. Phys. Lett ~, 869 (1980).<br />

D. Tran, K. Koo, and S. Sheem, J. Quant. Electron.<br />

QE-17, 988 (1981).<br />

R. Ulrich, S. Rashleigh, ‘Beam-to-Fiber Coupling<br />

with Low Standing-Wave Rtutio”, Appl. Opt. ~, 2453<br />

(1980).<br />

END VIEW<br />

OF FIBER<br />

4.<br />

G.B. Hocker, “Unidirectional Star Coupler for Single-Fiber<br />

Distribution System”, Opt. Lett. ~, 124<br />

(1977).<br />

5.<br />

S. K. Sheem, T. G. Giallorenzi, “Single-Mode Fiber<br />

Optical Power Divider: Encapsulated Etching”, Opt.<br />

Lett. ~, 29 (1979).<br />

6.<br />

J. G. Ackerhusen, “Microlenses to Improve LED-to-<br />

Fiber Optical Coupling”, Appl. Opt. ~, 3694<br />

(1979).<br />

Fig. 3.21<br />

CROSS SECTION<br />

VIEW<br />

OF FUSED COUPLER<br />

A biconical (tapered)<br />

fiberoptic coupler.<br />

7.<br />

8.<br />

M. Saruwatari, K. Nawata, “Semiconductor Laaer to<br />

Single-Mode Fiber Coupler”, APP1. Opt. ~, 1847<br />

(1979).<br />

H. Kuwahara, N. Tokoyo, M. Sasaki, “Efficient<br />

Coupling from Semiconductor Lasers into Single-<br />

Mode Fibers with Tapered Heimspherical Ends”,<br />

Appl. Opt. g, 2578 (1980).<br />

make this coupler a portion of the cladding is removed<br />

from each of ‘the fibers. These are then twisted together<br />

and etched until the thickness of the remaining<br />

cladding is about half the core diameter. The twisted<br />

pair is then fused under some axial tension causing a<br />

decrease in diameter, especially in the region of contact,<br />

i.e., the interaction region. The original core<br />

dimensions indicated in the upper right of Fig. 3.21<br />

are reduced as shown in the lower center of Fig. 3.21.<br />

The result is that optical energy that initially was<br />

confined close to the core tends to spread into the<br />

cladding in the region where the core diameter has<br />

been decreased. This results in a stronger overlap and<br />

therefore a higher coupling ratio. The Electrooptics<br />

Product Division of ITT has recently developed a specialized<br />

optical fiber that allows them to produce<br />

fused copulers by this method without the necesaity of<br />

etching. These couplers are available for sale. An<br />

alternate to these fiber couplers is the use of mini-<br />

3.3 <strong>FIBEROPTIC</strong> CABLES<br />

3.3.1 General<br />

Just as with conventional wire interconnections<br />

and communication links, there is a need for fiberoptic<br />

cables to accomplish a number of different<br />

purposea. In many ways, the individual fibers in an<br />

optical cable are treated very much like varnished or<br />

plastic insulated copper wires. The individual fibera<br />

consist of 100- to 200-micron-OD core-cladding waveguide<br />

elements having an outer coating that may be as<br />

thin as several microns of lacquer or as thick as 200<br />

to 400 microns of plastic, such as nylon, teflon, or<br />

polypropylene. Cabling serves the purpose of spacedivision<br />

multiplexing, combining anywhere from a few to<br />

many individual fibers into a single conveniently-pack-<br />

3-7

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