FIBEROPTIC SENSOR TECHNOLOGY HANDBOOK
FIBEROPTIC SENSOR TECHNOLOGY HANDBOOK
FIBEROPTIC SENSOR TECHNOLOGY HANDBOOK
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core. The central primary light-conducting region of a<br />
material medium, such as an optical fiber, the refractive<br />
index of which must be higher than that of<br />
its cladding in order for the lightwaves to be<br />
totally reflected or refracted. Most of the optical<br />
power is in the core.<br />
coupler. In optical transmission aystems, a component<br />
used to interconnect two or more optical fibera.<br />
Also see connector; bulk coupler; electronic&llycontrollable<br />
coupler; reflective star-coupler; 3-dB<br />
coupler.<br />
coupling. The connection, attachment, or binding of<br />
optical elements, electric circuit elementa, electric<br />
and magnetic fields, propagation modes, or electromagnetic<br />
wave component, such as surface waves<br />
and evanescent waves, to internal waves in waveguides,<br />
dielectric slabs, or other interdependent<br />
associations and interactions of events and materials<br />
in a system. For example, two optical fibers or certain<br />
elements in an integrated optical circuit may<br />
be coupled together in some manner to preserve signal<br />
continuity. See evanescent field coupling.<br />
coupling coefficient. Synonym for coupling ratio.<br />
coupling efficiency. In fiberoptic transmission, the<br />
ratio of the optical power on one side of an interface<br />
to the optical power on the other side. For<br />
example, the ratio of the power developed by a light<br />
aource to the power accepted by a bundle of fibers,<br />
or the power received at the end of a bundle of<br />
fibers to the power that impinges on a photodetector.<br />
For light sources with emitting areas larger than<br />
fiber core diameters, the product of fiber numerical<br />
aperture (N.A.) and core diameter is a good indicator<br />
of maximum coupling efficiency. For other<br />
sources, such as small laser diodes with emitting<br />
areas small than the fiber core diameter, the N.A.<br />
alone is a relevant indicator of coupling efficiency,<br />
usually expresaed as a percentage.<br />
critical angle. The angle, with the normal, at which<br />
an electromagnetic wave incident upon an interface<br />
surface between two dielectric media, at which total<br />
reflection of the incident ray first occurs as the<br />
incident angle with the normal to the incident aurface<br />
is increased from zero, and beyond which total<br />
internal reflection continues to occur although with<br />
increased attenuation at a rate determined not only<br />
by the electromagnetic parameters of the transmission<br />
medium, but also by the frequency and the incidence<br />
angle. The wave is guided along the reflecting<br />
surface with no average transport of energy into<br />
the second medium, and the intensity of the reflected<br />
wave is exactly equal to the intensity of the<br />
incident wave. The wave in an optical fiber will<br />
be confined to the fiber for all incidence angles<br />
greater than the critical angle. The critical angle<br />
is given by sin ec = (~2/~1) 1/2 where 9C is the<br />
critical angle and Cz and c1 are the permittivities<br />
of the transmitted (outside) and incident medium<br />
(inside), respectively, and where El is always greater<br />
than =2; e.g. , the case for an optical fiber (conducting<br />
a wave), and air. In terms of refractive<br />
indices, the critical angle is the incidence angle<br />
from a denser medium, at an interface between the<br />
denser and less dense medium, at which all of the<br />
light is refracted along the interface, i.e., the<br />
angle of refraction is 90°. When the critical<br />
angle is exceeded, the light is totally reflected<br />
back into the denaer medium. The critical angle<br />
varies with the refractive indices of the two media<br />
with the relationship, sin Oc = n2/nl, where n2 is<br />
the index of refraction of the less dense medium, nl<br />
is the refractive index of the denser medium, and 9C<br />
is the critical angle, as above. In terms of total<br />
internal reflection in an optical fiber, the critical<br />
angle is the smallest angle made by a meridional<br />
ray in an optical fiber that can be totally reflected<br />
from the innermost interface and thus determines<br />
the maximum acceptance angle at which a meridional<br />
ray can be accepted for transmission along a fiber.<br />
Also see total internal reflection.<br />
critical radius. The largest radius of curvature of an<br />
optical fiber, containing an axially propagated<br />
electromagnetic wave, at which the field outside the<br />
fiber still detaches itself from the fiber and radiates<br />
into space because the phase-front velocity<br />
must increase to maintain a proper relationship with<br />
the guided wave inside the fiber. Thia velocity cannot<br />
exceed the velocity of light, aa the wavefront<br />
sweeps around the outside of the curved fiber. This<br />
causes attenuation due to a radiation loss. The<br />
field outside the fiber decays exponentially in a<br />
direction transverse to the direction of propagation.<br />
It is the radius of curvature of an optical<br />
fiber at which there is an appreciable propagation<br />
mode conversion loss, due to the abruptness of the<br />
transition from straight to curved. For a radius<br />
of curvature greater than the critical value, the<br />
fields behave essentially as in a straight guide.<br />
For radii smaller than the critical value, considerable<br />
mode conversion takea place.<br />
coupling loss. In a fiberoptic coupling, the optical<br />
power loss caused by the coupling itself, a loss<br />
that would not occur if the optical fiber were continuous<br />
without the coupling.<br />
coupling ratio. The ratio of power on the output side<br />
of a coupling to the power on the input side. The<br />
coupling ratio is always less than unity. Synonymous<br />
with coupling coefficient. Also see 3-dB coupler.<br />
A-4<br />
D<br />
dark current. ~’e current that flows in a photodetector<br />
when there is no radiant energy or luminous flux<br />
incident upon its aensitive surface, i.e., when there<br />
is total darkness. Dark current generally increaaea<br />
with increaaed temperature for most photodetectors.<br />
For example, in a photoemissive photodetector, the<br />
dark current is given by:<br />
Id = AT2eq’$lkT<br />
where A is the surface area constant, T is the absolute<br />
temperature, q is the electron charge, $ ia<br />
the work function of the photoemisaive surface material,<br />
and k is Boltzmann’s constant.<br />
darkfield sensor. In fiberoptic, a sensor in which<br />
the optical power tapped and modulated by the sensor<br />
is a small fraction of the total optical power fed<br />
to or available to the sensor. Contrast with brightfield<br />
sensor.<br />
data. Representation of facts, concepts, or instructions<br />
in a manner suitable for communication, interpretation,<br />
or processing by human, manual, semiautomatic,<br />
or fully-automatic means. The characters<br />
used as data may assume any form or pattern to which<br />
meaning may be assigned in order to represent infor-