FIBEROPTIC SENSOR TECHNOLOGY HANDBOOK
FIBEROPTIC SENSOR TECHNOLOGY HANDBOOK
FIBEROPTIC SENSOR TECHNOLOGY HANDBOOK
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angstrom. A unit of length equal to 10-10 meter, 10-1<br />
nanometer, and 10-4 micron.<br />
aperture. See numerical aperture (N. A. ).<br />
array.<br />
See sensor array.<br />
attenuation. The decrease in power of a signal, light<br />
beam, or lightwave, either absolutely or as a fraction<br />
of a reference value. The decrease usually<br />
occurs as a result of absorption, reflection, diffusion,<br />
scattering, deflection, or dispersion from<br />
an original level and usually not as a result of<br />
geometric spreading, i.e., the inverse sqwre of<br />
the distance. In an optical fiber, attenuation Is<br />
undesirable for transmission purposes but desirable<br />
for prevention of leakage or clandestine detection.<br />
Optical fibers have been classified as high-loss<br />
(over 100 dB/km), medium loss (20 to 100 db/km),<br />
and 10W1OSS (less than 20 dB/km).<br />
band.<br />
B<br />
See conduction band; energy band; valence band.<br />
bandwidth. 1. A range of frequencies, usually specifying<br />
the number of hertz of the band or the upper<br />
and lower limiting frequencies. 2. The range of<br />
. frequencies that a device is capable of generating,<br />
handling, passing, or allowing, usually the range<br />
of frequencies in which the response is not reduced<br />
greater than 3 dB from the maximum response.<br />
baseband. The band of frequencies associated with or<br />
comprising an original signal from a modulated<br />
source. In the process of modulation, the baseband<br />
is occupied by the aggregate of the transmitted signals<br />
used to modulate a carrier. In demodulation,<br />
it is the recovered aggregate of the transmitted<br />
signals. The termis commonly applied to cases where<br />
the ratio of the upper to the lower limit of the<br />
frequency band is large compared to unity.<br />
beam splitter. h optical device for dividing a light<br />
beam into two separated beams. One simple beam<br />
splitter consists of a plane parallel plate, with<br />
one surface coated with a dielectric or metallic<br />
coating that reflects a portion and transmits a portion<br />
of the incident beam; i.e., part of the light<br />
is deviated through an angle of 90°, and part iS<br />
unchanged in direction. A beam splitter may also<br />
be made by coating the hypotenuse face of a 45°-90”<br />
prism and cementing it to the hypotenuse face of<br />
another. The thickness of the metallic beam splitting<br />
interface will determine the proportions of the<br />
light reflected and transmitted. In metallic beam<br />
splitters, an appreciable amount of light is lost by<br />
absorption in the metal. It may also be necessary<br />
to match the reflected and transmitted beam for<br />
brightness and for color. In these cases, it is<br />
necessary to use a material at the interface that<br />
gives the same color of light by transmission and<br />
reflection. Nhere color matching at the surface or<br />
interface cannot be accomplished, a correcting color<br />
filter may be placed in one of the beams. In a<br />
fiber-to-fiber beam splitter, evanescent coupling<br />
can be used to transfer optical energy from one<br />
fiber to another.<br />
birefringence. The splitting of a light beam into two<br />
divergent components upon passage through a doublyrefracting<br />
transmission medium, with the two components<br />
propagating at different velocities in the<br />
medium. In an optical fiber, birefringence is related<br />
to the strain in the fiber which causes the<br />
fiber to be a single polarization transmission<br />
medium.<br />
Bragg cell. An acoustooptlc device that accepts fixed<br />
frequency monochromatic light and that has a baseband<br />
vibrating element capable of modulating the input<br />
lightwaves producing an output lightwave with a<br />
frequency equal to the frequency of the input lightwave<br />
plus the frequency of the baseband input signal.<br />
The Bragg cell has application as part of an interferometer<br />
in which heterodyne detection is used.<br />
Brewster angle. The angle, measured with respect to<br />
the normal, at which an electromagnetic wave incident<br />
upon an interface surface between two dielectric<br />
media of different refractive indices is totally<br />
transmitted into the second medium. The magnetic<br />
component of the incident wave must be parallel to<br />
the interface surfa~~l The Brewster angle is given<br />
by: tan B = (~2/E1)<br />
, where B is the Brewster angle,<br />
c1 is the electric permittivity of the incident<br />
medium, and e2 is the electric permittivity of the<br />
transmitted medium. The Brewster angle is a convenient<br />
angle to transmit all the energy in an optical<br />
fiber to an outside detector. There is no Brewster<br />
angle, for which there is total transmission and<br />
therefore zero reflection, when the electric field<br />
component is parallel to the interface, except when<br />
the permittivities are equal, in which case there<br />
is no interface. Mso, for entry into a more dense<br />
medium, such as from air into an optical fiber: tan<br />
B = (n2/nl), and from a more dense medium into a<br />
less dense medium, such as fiber to air: tan B =<br />
(nl/n2), where nl and n2 are the refractive indices<br />
of the air and fiber, respectively.<br />
brightfield sensor. In fiberoptic, a sensor in which<br />
the optical power modulated by the sensor is all or<br />
a large fraction of the total optical power fed to<br />
or available to the sensor. Synonymous with lightfield<br />
sensor. Contrast with darkfield sensor.<br />
budget. See optical power budget; power budget; risetime<br />
budget.<br />
bulk coupler. In fiberoptic, a coupler that has one<br />
input and many outputs.<br />
bundle jacket. The outer protective covering applied<br />
over a bundle of optical fibers.<br />
bus. 1. One or more conductors that serve as a common<br />
connection for a related group of devices. 2. One<br />
or more conductors used for transmitting optical or<br />
electrical power or signals.<br />
bend.<br />
See ordinary bend.<br />
bend loss.<br />
See microbend loss.<br />
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