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BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention generally relates to a method for producing
reflectors in continuous lengths of optical fiber. More particularly, the
present invention involves the fabrication of reflectors in optical fibers
by fusion splicing. The present invention also relates to apparatus which
make use of fiber reflectors produced as a result of the claimed
invention.
2. Description of the Prior Art
A number of methods for fabricating taps in optical fibers have been
disclosed in the art. One such method involves the bending of the optical
fiber axis in order to couple out some of the light which would ordinarily
propagate through the substantially linear fiber. This method is used, for
example, in the Siecor Model M67-210Local Injection Detection System, as a
means of monitoring the transmitted power in a fusion splicing unit. The
tap produced as a result of this method of removing light is normally
referred to as a macrobend tap.
A second method known in the art discloses the use of two fibers having
relatively thin cores which are merged or placed in close proximity to
each other so that at least some of the propagated light couples from one
fiber to another. Such a method is generally disclosed in such commercial
applications as the Amphenol Model 945 Fiber Coupler, often referred to as
a fiber optic directional coupler.
Yet a third prior art method discloses the use of a reflective film
deposited or evaporated on the ends of oplique optical fibers which are
then physically combined at a joint or other similar bonding structure. In
such prior art applications, a dielectric film, such as TiO.sub.2 or
SiO.sub.2, is alternatively evaporated on the fiber ends in order to
reflect part of the light propagated through the fiber. Couplers of this
type generally utilize optical fibers cut at an angle of 45.degree. to
their respective axis, and utilize optical cement for joining the fiber
ends.
These prior art methods, however, suffer from a number of disadvantages.
When light is coupled out by bending or distorting the linear axis of the
optical fiber, it oftentimes becomes difficult to concentrate the
propagated light into a small area photodetector. This disadvantage
hinders high speed operation desirous in contemporary signal processing
applications. Further, such a method couples light out in only a forward
or lateral direction, but not in the reverse direction, as is often
required in preferred applications.
Another significant disadvantage of prior art methods based upon macrobend
or directional coupler taps is their tendency to introduce "modal noise"
into the coupled fiber system. Recognizable as a spurious amplitude
modulation at the receiver, modal noise is caused by the highly mode
selective nature of the optical taps normally created between spliced
fiber ends.
Other disadvantages of prior art methods include the general lack of
structural integrity associated with the cementing of optical fibers
coated with dielectric films. For practical applications for this kind of
coupler, therefore, mechanical support is generally needed, which support
greatly increases the overall bulk and expense of the final system.
SUMMARY OF THE INVENTION
The present invention overcomes the aforementioned and other disadvantages
by providing an inexpensive method for producing reflectors in continuous
lengths of optical fiber.
In a preferred embodiment of the present invention, optical fibers are
first prepared by cleaving or polishing their ends so as to establish a
flat, smooth bonding surface. After taking necessary precautions to remove
organic films or other contaminants, a selected portion of these fibers
are placed in a vacuum system and the prepared ends are then coated with a
metallic material such as Ti or a dielectric material such as TiO.sub.2.
This coating can be prepared by using thermal evaporation, electron beam
evaporation, or sputtering. After this coating has been applied to the
selected fibers, the prepared, coated fibers are removed from the vacuum
system and prepared for splicing. A reflector is then created in a
prepared, coated fiber by placing one of these coated fibers end-to-end
with an uncoated prepared fiber in a fusing splicing apparatus. One or
more arc discharges are then produced by activating the fusion splicing
apparatus until the fiber ends are joined together and the reflectivity of
the spliced region reaches a desired value.
Using a general aspect of the above described method, variably reflective
optical taps may be produced by utilizing the dielectric to metal phase
transitions of vanadium oxides which have been incorporated in reflectors
formed in a length of optical fiber. By passing electric current through a
resistive wire or film formed along a length of fiber containing the
reflector, the reflector is heated sufficiently to drive the selected
vanadium oxide coating through this phase transition, thus altering the
overall reflectivity of the fiber mirror. When the current is turned off
or reduced, the optical reflector fiber cools sufficiently to bring it
back through the phase transition to its original reflectivity.
Variably reflective optical taps may also be formed utilizing Fabry-Perot
cavities arranged along a length of optical fiber. The Fabry-Perot
cavities themselves are formed using much of the methodology described
earlier for the formation of optical taps. An electrically resistive
medium is then deposited along the fiber segment between the optical
reflectors such that the introduction of an electric current through the
medium brings about a calculated change in reflectivity.
Optical fiber taps produced as a result of the aforedescribed method have a
variety of applications. One of the primary applications for these fiber
reflectors are as taps in tapped delay line filters, or transversal
filters. The use of variable reflectors in such taps also serves to make
the tap weight programmable. Also, and similar to other types of
transversal filters, these optical taps can function as matched filters,
correlators, waveform or sequence generators, and deconvolvers.
Using the aforedescribed methods, optical fibers can be prepared with the
surface normal to the axis or with the surface at an angle. When the angle
between the surface and the axis is 45.degree., for example, the light
will be reflected out of the film in a direction approximately normal to
its axis. A fiber with this sort of surface to axis configuration could be
used as a tapping element in fiber communication systems or in a fiber
sensor, thus providing an alternative to a directional coupler.
A variable reflectivity optical tap incorporating a vanadium oxide may have
significant utility in applications where it is necessary to determine and
quantify a fluctuation in system temperature. One such example is a
thermal sensor such as may be utilized in a progressively monitorable fire
alarm system. In optical taps incorporating vanadium oxides, a dramatic
change in reflectance will occur near the semiconductor-to-metal phase
transition temperature. With such optical tap systems placed at desired
locations along a continuous fiber line in a building or naval vessel, for
example, the progression of a fire may be monitored via a pulsed light
source. Since silica fibers can withstand very high temperatures, this
type of system should continue to function properly even when a part of
the fiber cable is engulfed in flames.
Fabry-Perot interferometers consisting of single mode fibers with optical
mirrors disposed at their ends have been used in the art as
interferometric sensors and as discriminators for coherent communication
systems. Using the method of the present invention, Fabry-Perot
interferometers may be incorporated into a continuous length of optical
fiber. In this fashion also, low-finesse Fabry-Perots, monitored in
reflection, may be used as temperature sensors.
The taps produced as a result of the present invention are strongly
polarization-selective. This polarization selectivity may be utilized in
single mode systems, such as in fiber gyroscopes, which necessitate
polarizing elements. In such applications, the mirrors produced in the
taps would be oriented at Brewsters angle so that all of the light
polarized in a first plane is transmitted through the mirror, while light
polarized in a second plane is partially reflected. Thus, a highly
polarized, transmitted beam may be obtained using multilayer quarter wave
coatings.
It is appreciated in the art that reflection from external cavities can
lead to mode stabilization and line narrowing in diode lasers. The mirrors
produced as a result of the present invention, in conjunction with
pigtailed lasers, are ideal for this application. For modelocking
applications, an array of mirrors may be utilized. In such a case, the
round trip delay phase between the mirrors could equal the spacing of the
mode locked pulses and would approximate the inverse of the laser
relaxation frequency.
The present invention has many advantages over the prior art. One chief
advantage is the ability to produce reflectors simply and inexpensively in
continuous lengths of optical fiber. In signal processing applications,
this would allow the fabrication of transversal filters for operation with
very high bandwidth analog (e.g. > lGHz)) or high data rate (e.g. > lG
bit/sec) digital signals.
Another advantage of the present invention is the overall mechanical
strength of the resultant tap. Using the method of the claimed invention,
the strength of the fiber material may be maintained at the tap site so
that no mechanical support is needed, thus enhancing the flexibility of
the junction while decreasing the overall bulk of the system.
Another advantage of the present invention is the ability to fabricate an
optical tap that can be made to reflect light out of the side of a fiber,
or to reflect it back down the fiber axis.
Yet another advantage of the claimed method is that the reflectance of the
resultant tap can be adjusted to a desired value at the time the tap is
being produced.
Yet another advantage of the present invention is the simple, efficient
removal of light from a multi-mode fiber so as to substantially reduce
modal noise. The method of the present invention results in an optical tap
having uniform reflectance across the fiber cross-section. With such
uniform reflectance, modal noise produced by the coupler itself is much
lower than for directional coupler taps in multi-mode systems.
BRIEF DESCRIPTION OF THE DRAWINGS
FIGS. la-e generally illustrate the basic process of the present invention
by which a reflector may be formed in a continuous length of optical
fiber.
FIG. 2 schematically illustrates an optical time domain reflectometer
(OTDR). The configuration illustrated in FIG. 2 also finds application as
a tapped-delay-line signal processing device.
FIGS. 3a-c generally illustrate various methods for producing variably
reflective optical taps in a continuous length of optical fiber.
FIGS. 4a-b generally illustrate optical fibers prepared with reflectors
positioned at angles relative to the fiber axis.
FIG. 5 schematically illustrates a general embodiment of a transversal
filter which can be implemented in fiber optic form using the
configuration of FIG. 2.
FIG. 6 illustrates an interferometer incorporated in a continuous length of
optical fiber.
FIGS. 7a-b schematically illustrate a series of variably reflective optical
taps as they may be distributed along a continuous length of optical fiber
such as to form a progressively monitorable fire alarm system.
DESCRIPTION OF THE PREFERRED EMBODIMENT
FIG. 1 generally illustrates one embodiment of the present invention in
which reflectors may be formed in a continuous length of optical fiber. In
one preferred embodiment, reflectors may be formed by the fusion splicing
of two graded index multimode fibers, one of which is coated on the end
with a TiO.sub.2 layer or film. Other preferred embodiments make use of a
single mode fiber, and may incorporate a variety of coating materials.
Referring to FIGS. la-1e, an optical fiber 2 is first prepared by cleaving
and/or polishing the ends of the fiber 2 with a scribing tool 1 or the
like such that the ends are flat and smooth. After taking any necessary
precautions to remove organic films or other contaminants, this fiber 2 is
placed in a dc planar magnetron system 6 where a TiO.sub.2 film 4 is
deposited on the ends by sputtering in a 70% argon-30% oxygen produced
atmosphere.
The prepared, coated fiber 2 is then removed from the vacuum system 6 where
it is placed end-to-end with an uncoated prepared fiber 3 in a splicing
unit which uses an electric arc between electrodes 8 and 9. This splicing
unit, e.g. a Siecor Model M-67 fusion splicer, is operated at a much lower
arc current and arc duration (typically, 5 mA and 0.3s) than the
recommended value of 14 mA and 1.5 s for splicing uncoated fibers. A
number of splicing pulses in sequence are used to produce each reflector
10.
It is envisioned that many other reflectively dissimilar materials might be
deposited on the prepared fiber for use in making optical reflectors. Such
materials include Zn, ZnO, Ta, Al, A1.sub.2 O.sub.3, Ag, Au, V, VO.sub.2,
and V.sub.2 O.sub.5. Additionally, these materials may be deposited using
alternate methods of thermal evaporation or electron beam evaporation.
The duration, current, and number of discharges are parameters of the
process which can be varied to obtain optimum fiber strength and splice
reflectivity. If desired, the reflectivity of the splice can be monitored
during the fabrication process using an optical time domain reflectometer
(OTDR) as illustrated in FIG. 2. In such a setup, short pulses at 0.83
.mu.m from a diode laser 12 are injected into an optical fiber 2, which
has been provided with a series of dielectric mirrors 7. The optical
pulses reflected from a beam splitter 15, are then monitored with a
silicon avalanche photodiode 14. It should be understood that other laser
wavelengths, such as 1.3 .mu.m, and other photodetector types, such as
germanium avalanche photodiodes, may be used. It should be further
appreciated that a fiber optic directional coupler could be used as a beam
splitter.
FIGS. 3a-3c illustrate two distinct methods for forming variably reflective
taps in a continuous length of optical fiber. As noted, some vanadium
oxides undergo a thermally induced dielectric to metal transition, thereby
enabling the construction of variably reflective mirrors. FIG. 3a
illustrates a variable VO.sub.2 or V.sub.2 O.sub.5 reflector 20 formed in
a length of optical fiber 2. Placed across this reflector 20 is a
resistive film or wire 22 which is formed in contact with the fiber 2. The
resistive film or wire is preferably formed of A1, W, Cr, Ti, or alloys
thereof. When an electrical current is placed through this resistive film
or wire 22, the fiber 2 is heated sufficiently to drive the reflector 20
through its phase transition and thus alter its overall reflectivity. When
the current is turned off or reduced, the reflector 20 cools sufficiently
to return through the phase transition to its original reflectivity.
In an alternate embodiment of the present invention, a variable
reflectivity optical tap may be produced by the fusing of a fiber segment
between two fiber optic reflectors of nominally equal reflectivity, this
fiber segment being disposed between the two mirrored segments such as to
form a Fabry-Perot cavity. These segments may be prepared, coated and
fused together according to the methodology previously described.
By changing the optical path length of this cavity, it is possible to
adjust the reflectivity in a range between a minimum value near zero and a
maximum value approximately 4 times the reflectivity of one of the mirrors
in the absence of such a cavity. This optical path length .DELTA.L.sub.opt
may be changed by heating the fiber, where the change in optical path
length .DELTA.L.sub.opt is then determined by the relationship
.DELTA.L.sub.opt =2.DELTA.(nL), where n is the reflective index, and L is
the length of the fiber. This optical path length may also be changed by
applying an electric field across the fiber in order to change its
refractive index. This change in path length is dictated by the Kerr
effect and may be expressed by .DELTA.L.sub.opt =KE.sup.2, where E is the
applied electric field and K is a constant which depends on the fiber
dimensions, and upon the Kerr constant of the fiber material.
FIGS. 3b and 3c generally illustrate a second method of producing variable
reflective optical taps employing the aforedescribed method. As seen in
FIG. 3b, two reflectors 30 and 32 of nominally equal reflectivity are
separated by a segment of fiber 36 in order to form a Fabry-Perot cavity.
Across this cavity is placed a resistive film or wire 40 which is in
contact with the film segment 36. The optical path length of this cavity
may be charged by heating the fiber 36 such as to change its refractive
index. Alternatively, and as seen in FIG. 3c, an electron field may be
created by applying a voltage between electrodes 41 and 42 across the
segment 36 to induce a refractive index change. Using this Fabry-Perot
cavity, it is possible to adjust the reflectivity of the resultant optical
splice in a range between a minimum value near zero and a maximum value
approximately four times the reflectivity of one of the reflectors in the
absence of such a cavity.
The fabrication of reflectors oriented at an angle to the fiber axis may be
seen in FIGS. 4a and 4b. These reflectors are produced by depositing
several films of a high and low refractive index on the fiber ends prior
to splicing. In these figures, a multilayer mirror 60 is created in an
optical fiber 2, said mirror 60 prepared with its reflective surface at an
angle 62 to the fiber axis 64.
FIG. 5 schematically illustrates a general embodiment of a transversal
filter which can be implemented in fiber optic form using the general
configuration of FIG. 2.
Referring to FIG. 6, Fabry-Perot interferometers 13 consisting of single
mode fibers 3 with mirrors 11 disposed at the ends, have use as
interferometric sensors, and as discriminators for coherent communication
systems. Using the aforedescribed method, an interferometer 13 may be
incorporated in a continuous length of optical fiber 3 as illustrated in
FIG. 6. In yet other embodiments, low-finesse Fabry-Perots, monitored in
reflection, may be used as temperature sensors such as that illustrated in
FIG. 7.
FIG. 7 illustrates yet another embodiment of the present invention in which
variably reflective optical taps are distributed along a continuous length
of optical fiber. It has been established that the fractional charge in
the refractive index of SiO.sub.2 fiber is approximately 10.sup.-5
/.degree. C. Therefore the reflectance of a Fabry-Perot cavity 10 cm goes
through one complete cycle over a 6.5.degree. temperature change at l.3
.mu.m. If a pulsed light source 80 is coupled to the fiber-tap system and
linked by a fiber optic coupler 81 to a receiver (not shown), a
progressively monitorable fire alarm system may be formed. In such a
system, reflectors 9 undergoing a temperature transition may be identified
by their higher power signatures as illustrated in FIG. 7b.
Yet another form of such a temperature sensor would make use of a phase
transition material such as VO.sub.2 to form the reflectors 9. A
reflective change for a particular reflector would occur when it is heated
above the transition temperature, which in the case of VO.sub.2, is
68.degree. C. .
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