Note: Descriptions are shown in the official language in which they were submitted.
22~230 4
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BROADWIDTH LINEWIDTH LASERS FOR
OPTICAL FIBER COMMUNICATION SYSTEMS
This application is a division of Canadian patent
application Serial No. 2,062,605 filed March 10, 1992.
The present invention relates to optical fiber
communication systems, and more particularly, to a method
and apparatus for reducing non-linear effects in an
optical fiber used for communicating AM or other
information signals.
Optical transmission systems are currently being
implemented for use in various communication
applications. For example, telephone systems are now in
use that utilize optical fiber technology to transmit
voice and data signals over long distances. Similarly,
cable television networks are available wherein optical
fiber technology is used for the transmission of both
analog and digital signals.
In order to transmit an information signal
(e.g., a television signal) over an optical fiber, a
light beam ("carrier") must be modulated with the
information signal. The modulated carrier is then
transmitted to a receiver via the optical fiber. At
high power levels, silica fibers exhibit non-linear
effects due to the interaction of the local electric
22~ 230 4
.
field across the fiber and the fiber material.
These non-linear effects also depend on the length
of the fiber, with a cumulative degradation of
performance resulting as the length of the fiber
increases.
Among the non-linear effects exhibited in silica
fibers at high power levels are four-wave mixing,
Brillouin gain, and Raman gain. The magnitude of
these interactions depend on the spectral density of
the applied field. The power of the optical signal
is also a factor in determining the severity of the
non-linear effects.
Very little effect on signal transmission is
seen below a threshold power density level.
Beginning at a critical power density level, power
will be shifted in wavelength by the non-linear
interaction between the traveling wave and the
material. Since optical fibers concentrate the
power into a small cross section, the large fields
required to make these effects significant arise at
modest absolute power levels. For long distance
signal transmission, these non-linear effects
constitute an upper limit on the power level that
can be transmitted. See, for example, Y. Aoki, K.
Tajima and I. Mito, "Input Power Limits of Single-
mode Optical Fiber Due to Simulated Brillouin
Scattering in Optical Communications Systems," IEEE
Journal of Liqhtwave Technology, May 1988, pp. 710-
727 and Agrawal, Govind P., "Non-Linear Fiber
~a 230 4
-
Optics", Academic Press 1989, ISBN 0-12-045140-9.
The non-linear effects in optical fibers are
particularly troublesome for the transmission of
amplitude modulated ("AM") signals, such as those
used in conventional analog television signal
broadcasting.
It would be advantageous to provide a method and
apparatus for reducing the non-linear effects in
optical fiber for the transmission of information
signals, such as AM vestigial sideband (VSB-AM)
television signals at high power levels. The
present invention provides such a method and
apparatus, including various embodiments of broad
linewidth lasers that output optical carriers for
use in communicating information signals via optical
fiber links.
3 0 4
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In accordance with the present invention, a
method and apparatus are provided for reducing non-
linear effects in an optical fiber used for
communicating information signals, such as AM
information signals, at high power levels. In the
common terminology used by those skilled in the art
of non-linear interactions, the terms "pump
wavelength" and "signal wavelength" are used to
describe the stimulated Brillouin interaction.
Using this terminology, the signal laser in
accordance with certain embodiments of the present
invention plays the role of the pump laser. In such
cases, the classical signal laser is absent since
there is no desire to use the Brillouin gain, which
gain would limit the achievable transmission
distance and increase the system relative intensity
noise from 0 Hz up to subcarriers a few times the
Brillouin bandwidth.
In the present invention, a laser output signal
is provided. The linewidth of the laser output
signal is increased to provide a broadened
optical signal. The optical signal is externally
modulated with an information signal (e.g., an AM
signal), and coupled to an optical link fiber for
transmission to a receiver. In order to increase
the linewidth of the laser output signal, the laser
output is optically modulated in one embodiment by
7 ~ 23~ 4
-- 5
broadband electrical noise. The noise can be either
frequency modulated or phase modulated on the broadened
optical signal. The bandwidth of the noise and/or the
optical modulation index used during the optical
modulation step is controlled to provide a desired
linewidth for the broadened optical signal.
An apparatus described herein includes a light
source for providing an optical carrier. Means are
provided for optically modulating the carrier by
broadband electrical noise. External modulator means,
coupled to receive the optically modulated carrier,
modulate the carrier with an information signal. Means
are provided for coupling the information modulated
carrier from the external modulator means to an optical
transmission path such as an optical fiber. The optical
modulating means can comprise an optical frequency
modulation ("FM") modulator or an optical phase
modulation ("PM") modulator. The light source can
comprise a continuous wave ("CW") laser.
In a method according to the invention for
increasing the linewidth of a longitudinal mode of a
laser, a laser cavity is provided for outputting an
optical signal having a longitudinal mode. An active
medium is pumped with a pump laser to provide a source of
excess spontaneous emission at or near the lasing
wavelength of the laser cavity. The laser cavity is
pumped with the pump laser while excess spontaneous
emission from the source thereof is injected into the
3 1) 4
_ -- 6
laser cavity to increase the linewidth of said mode. In
an illustrated embodiment, the laser cavity is pumped by
energy received from the pump laser via the source of
spontaneous emission.
One embodiment of laser apparatus according to the
invention uses spontaneous emission to provide an optical
carrier having a broad linewidth. A laser cavity outputs
an optical signal having a longitudinal mode. An active
medium having an output coupled to the laser cavity is
provided for injecting spontaneous emission at or near
the wavelength of said mode into the cavity. A pump
laser is provided to pump the active medium for producing
spontaneous emission while simultaneously pumping the
laser cavity to produce the optical signal. In this
manner, the spontaneous emission in the laser cavity
increases the effective linewidth of said mode.
In an illustrated embodiment, the spontaneous
emission is injected into the laser cavity together with
the pumping energy for the laser cavity. The active
medium can comprise a grating and a gain medium coupled
in series with the laser cavity, for example, between the
pump laser and the laser cavity.
In another embodiment, laser apparatus for providing
an output signal with a broad linewidth comprises a laser
cavity for outputting an optical signal to a first port
of an optical circulator. Spontaneous emission means,
having an output coupled to a second port of the optical
circulator, injects spontaneous emissions at or near the
wavelength of a longitudinal mode of the optical signal
into the laser cavity via the first port of the optical
3 ~ 4
,
circulator. A third port on the optical circulator
outputs the optical signal with the effective
linewidth of said mode increased by said spontaneous
emission. The laser cavity can be contained in a
ring laser having a first end coupled to a first
port and a second end coupled to said third port of
the optical circulator. Such apparatus further
comprises an optical coupler coupled to the ring
laser for outputting the optical signal with the
increased effective linewidth.
Another embodiment of the present invention uses
a semiconductor laser to output an optical signal.
An optical amplifier is coupled in series with an
output of the laser for amplifying the optical
signal. The amplifier includes means for generating
spontaneous emissions at or near the wavelength of a
longitudinal mode of the optical signal. The
amplifier injects the spontaneous emissions into the
laser output. The spontaneous emissions injected
into the laser increase the effective linewidth of
said mode. Optical filter means can be coupled in
series between the laser and the optical amplifier,
for selecting at least one property of the
spontaneous emissions that are injected into the
laser output. For example, the filter means can
select the magnitude and spectral properties of the
spontaneous emissions.
Another embodiment of the present invention uses
a microchip or solid state laser for providing an
3 ~ 4
output signal with a broad linewidth. The laser is
responsive to pump energy for outputting an optical
signal. Means are provided for generating
spontaneous emissions at or near the wavelength of a
longitudinal mode of said optical signal. The
spontaneous emissions output from the generating
means are combined with the pump energy for input to
the microchip laser. The spontaneous emissions
input to the laser serve to increase the effective
linewidth of said mode.
A spontaneous emission source having a high
spectral density at a desired wavelength is also
provided. The source comprises a guided wave
optical path that includes a grating and an active
medium. Optical energy is passed across said
grating and active medium within the optical path.
The optical energy excites the active medium without
lasing to output spontaneous emissions from the
optical path at a wavelength established by the
grating. The grating can reside in the active
medium portion of the optical path. In a preferred
embodiment, the grating is an in-fiber grating
provided in an optical fiber, and the active medium
comprises a rare earth doped portion of the optical
fiber.
3 ~ 4
~ g
In the drawings,
Figure 1 is a block diagram illustrating apparatus
that uses broadband noise to increase linewidth;
Figure 2 is a block diagram illustrating apparatus
that uses a periodic function input to an external
modulator to increase linewidth;
Figure 3 is a block diagram illustrating apparatus
wherein a periodic function directly modulates a laser to
increase linewidth;
Figure 4 is a block diagram illustrating apparatus
in accordance with an embodiment of the present invention
that uses a spontaneous emission source in series with a
laser cavity to increase linewidth;
Figure 5 is a block diagram illustrating apparatus
in accordance with another embodiment of the present
invention that couples a spontaneous emission source to
a laser cavity via an optical circulator;
Figure 6 is a block diagram illustrating apparatus
in accordance with a further embodiment of the present
invention that uses an optical circulator to couple a
spontaneous emission source to a ring laser to increase
linewidth;
Figure 7 is a block diagram illustrating apparatus
utilizing a different type of ring laser;
Figure 8 is a block diagram illustrating another
apparatus in accordance with the present invention that
uses an optical amplifier to inject spontaneous emissions
into a semiconductor laser to increase linewidth; and
2 3 ~ 4
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- 10
Figure 9 is a block diagram illustrating still
another apparatus in accordance with the present
invention wherein spontaneous emissions are input to a
microchip laser to increase linewidth.
3 ~ 4
,
11 --
In accordance with the present invention, the
non-linear effects exhibited in an optical fiber at
high power levels due to the spectral density of the
optical signal are reduced to a level enabling the
transmission of AM communication signals at
relatively high power levels. Currently, a high
power solid state or semiconductor laser for use in
communications will produce a signal on the order of
30 milliwatts or so. The output powers of such
lasers are increasing at a rapid pace, and output
powers on the order of four watts or so are expected
to become commercial in the future. It is expected
that even higher power lasers will be available for
communication purposes in the not too distant
future.
High power optical communication systems are
advantageous in that a signal can be split into a
plurality of paths (e.g., in a tree and branch
distribution network). In addition, high power
enables the signals to be transmitted over longer
distances without the need for signal amplification.
This reduces the cost of the communication system.
Non-linear effects such as four-wave mixing and
Brillouin gain have hampered efforts to provide a
cost effective high power optical communication
system for AM signals, such as television signals
transmitted over a cable television network. In
3 ~ 4
- 12 -
order to overcome the non-linear effects for
relatively high power AM signals communicated over
an optical fiber, the present invention increases
the effective linewidth of the carrier light source
(e.g., laser) to reduce the effects of fiber non-
linearity. Broadening the optical linewidth reduces
the spectral density of the signal, distributing the
same power over a broader range.
As an example, the Brillouin gain threshold is
reduced by the ratio ~VB/ (~VB+~Vp) where ~vp is the
optical linewidth (i.e., the linewidth of the
optical field that induces the non-linearity) and
~vB is the gain bandwidth of the Brillouin gain.
For typical single mode fibers, ~vB is
approximately equal to 100 MHz. For a modulated
distributed feedback ("DFB") laser, the effective
~vp is on the order of 10 GHz and up. When a CW
laser and an external modulator serve as the pump
laser, ~vp can be as small as a few kilohertz
depending on the specific source laser. Thus, a
wide range of ~vp can exist, depending on the type
of laser used.
In practical vestigial sideband AM systems that
use external modulators, approximately 95% of the
optical power is concentrated within ~vp at vO,
where vO is the optical frequency of the non-linear
pump. For a typical single mode fiber having a
- 2~3~4
Brillouin gain bandwidth of about 100 MHz, a laser
providing a linewidth of two kHz will produce a gain
~VB/ (~V~+~VP) ~1. For a DFB laser having a
linewidth of six GHz, the Brillouin gain
~VB/ (~VB+~VP) = . 016. Thus, we see the Brillouin
gain is much higher for the laser which has a two
kHz linewidth.
In accordance with the present invention, the
output of a semiconductor or solid state laser
having a narrow linewidth is broadened. For
example, optical broadening can be achieved by an
optical angle modulator (e.g., frequency or phase
modulation) driven by broadband electrical noise
; (e.g., white noise having a 100 MHz to 300 MHz
bandwidth) or a periodic function (e.g., sine wave)
to effectively increase the optical linewidth.
Injection of excess spontaneous emissions into a
laser cavity can also be used to broaden the optical
linewidth of an output signal. As illustrated in
the embodiment shown in Figure 1, continuous wave
laser 10 produces an optical spectrum 12 having an
optical frequency vO. The narrow linewidth of the
laser output signal is increased by modulating it
with broadband electrical noise input to an optical
modulator 14 at terminal 16. The resultant spectrum
18 output from optical modulator 14 has a
substantially increased linewidth ~v. This optical
signal, still centered around optical frequency vO,
~23~ 4
_ ~4 -
serves as an optical carrier for communication of an
information signal to a conventional receiver 26
over a link fiber 24.
In order to modulate the optical carrier with
the information signal, an external modulator 20 is
provided. This modulator can comprise, for example,
an electrooptic device such as a Mach Zehnder
modulator. External optical modulators are well
known in the art. See, e.g., S. E. Miller, T. Li,
and E. A. J. Marcatili, "Research Toward Optical
Fiber Transmission Systems", Proc. IEEE, Vol. 61,
pp. 34-35, Dec. 1973. In the embodiment illustrated
in the figure, an RF AM signal, such as an AM VSB
television signal, is input to external modulator 20
via coaxial cable input terminal 2Z. The AM
modulated optical carrier is then received by
receiver 26 via the link fiber.
Optical modulator 14 can comprise either a phase
modulator or a frequency modulator. The linewidth
of the signal output from modulator 14 is selected
by controlling the bandwidth of the electrical noise
source and/or the optical modulation index of the
optical modulator. Optical phase modulators that
can be used in connection with the present invention
are commercially available. For example, the Model
PM 315 modulator sold by Crystal Technology of Palo
Alto, California and the Model IOC 1000 modulator
sold by BT&D of Wilmington, Delaware.
3 ~ 4
- 15 -
A dlfficulty in realizing a pure optical phase
modulator such as modulat-or 14 illustrated in the
embodiment of Figure 1, is that if there are any
reflections the phase modulator acts as a Fabry
Perot interferometer, which introduces unwanted
amplitude noise, i.e., relative intensity noise
(RIN). It has been recently reported that a lithium
niobate modulator can achieve virtually ideal phase
modulation. S. K. Korotky, et al., "High-Speed Low
Power Optical Modulator with Adjustable Chirp
Parameter," Inteqrated Photonics Research
Conference, Paper TuG2, April 9-11, 1991, Monterey,
California. Such a modulator can be used to
increase linewidth using a broadband electrical
noise source as illustrated in Figure 1.
Alternatively, such a modulator can be used to
increase linewidth using a sine wave as illustrated
in the embodiment of Figure 2.
As illustrated in Figure 2, a continuous wave
laser 30 provides an optical output signal having a
longitudinal mode 31 that is modulated in a phase
modulator 32 by a periodic function such as a sine
wave provided by source 34. By modulating this mode
with a sine wave in phase modulator 32, the
effective linewidth of mode 31 is increased as
illustrated by dotted line 33, to extend between the
first sideband components of the sinusoidal
modulation. Thus, if the periodic function input
to phase modulator 32 is a 1 GHz sine wave, the
3 ~ 4
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- 16 -
effective linewidth of the mode 31 will be broadened
to extend from -1 GHz to +l GHz. Those skilled in
the art will appreciate that the actual width of
mode 31 remains narrow, but its effective linewidth
is increased by the frequency dithering caused by
the sinusoidal modulation.
The periodic function provided by source 34 has
a frequency that is high enough with respect to an
information signal to be carried by the optical
lo signal, such that sidebands of the periodic function
will not interfere with the information signal.
Thus, for example, in cable television applications
where the cable spectrum extends from about 50 MHz
to 550 MHz, a sine wave having a frequency on the
order of 1 GHz can be used to provide a modulating
signal for phase modulator 32.
- The output 33 of phase modulator 32 is coupled
to an external modulator 36 that is the same as
modulator 20 described in connection with Figure 1.
An information signal input to the external
modulator modulates the optical signal for
transmission of the information via link fiber 40 to
a receiver 42.
Figure 3 illustrates another embodiment wherein
a distributed feedback (DFB) laser 50 is directly
modulated with a periodic function, such as a sine
wave provided by source 52. DFB laser 50 is
modulated at a frequency that is high compared to
-the video subcarrier modulation. The modulation of
~ ~
- 17 -
the DFB laser broadens the optical linewidth and
reduces the source coherence. For providing an
optical carrier for cable television applications,
an RF sine wave of about 1 GHz can be used to
directly modulate DFB laser 50. The output of the
laser will comprise an optical signal having a
longitudinal mode that sweeps back and forth with
the sine wave modulation between -1 GHz to +l GHz.
In other words, the original longitudinal mode of
the laser is dithered between bounds established by
the frequency of the input periodic function. The
effect is that the average linewidth is widened,
providing a broadened output signal to reduce the
system Brillouin threshold allowing higher power
operation. The added advantage of reduced
coherence length serves to reduce the susceptibility
of the system to beat noise degradation. Beat noise
degradation is the interferometric conversion of
optical phase noise to intensity noise. In a
directly modulated DFB laser, beat noise degradation
is manifest in the system as an increase in system
relative intensity noise (RIN). In a standard
externally modulated VSB-AM system, beat noise
degradation is seen as an increase in the phase
noise of the RF carriers.
The embodiment of Figure 3 illustrates optional
optical amplifiers 54 and 60, which can be provided
at the input and output ends, respectively, of
external modulator 56. As in the embodiments -
~
r~ 2~ 23~ 4
- 18 -
illustrated in Figures 1 and 2, modulator 56 can
comprise a Mach Zehnder type modulator to which an
information signal is input via coaxial cable
terminal 58. The information is carried via link
fiber 62 to a receiver 64 in a conventional manner.
It is also possible to increase the linewidth of
a longitudinal mode by injecting excess spontaneous
emission into a laser cavity. Various
implementations of such a system are illustrated in
Figures 4 through 9. Figure 4 illustrates a linear
embodiment wherein an erbium fiber laser linewidth
is increased via the injection of excess spontaneous
emission into the laser cavity. An active fiber 74
between a grating 72 and an optical isolator 76
generates excess spontaneous emission at or near the
lasing wavelength provided by a laser cavity
generally designated 80. The lasing wavelength is
determined by grating 78 within the laser cavity.
Active fiber 74 does not lase since isolator 76
provides a very low back reflection. Thus, the
erbium fiber extending from grating 72 to isolator
76 provides a spontaneous emission source, when
pumped by a pump laser 70, for injection of
spontaneous emission into laser cavity 80 via
isolator 76. Unabsorbed pump power from pump laser
70 also propagates through isolator 76 to excite
laser cavity 80. The unabsorbed pump power pumps
the erbium fiber laser defined by grating 78 and
reflector 84. Although such a design would be most
r ;~ 3n 4
-- 19 --
efficient for delivering spontaneous emissions at
wavelengths that differ from the lasing wavelength,
spontaneous emissions at or near the lasing
wavelength (i.e., the wavelength defined by grating
78) can be provided if grating 78 is chosen to have
a reflectivity that passes a relatively large amount
of the spontaneous emission from the emission
source. For example, such a result can be achieved
if the reflectivity of grating 78 is on the order of
50% at the lasing wavelength. Mode selection within
the laser cavity is provided by conventional means
82, such as the provision of a narrow Fabry Perot
within the laser cavity. Specific techniques for
mode selection are disclosed in commonly assigned,
co-pending Canadian patent application No. 2,055,324-3,
filed November 13, 19~1. Af~e~ mode selection, the
light from laser cavity 80 is passed through an
optical isolator 86 for output to an external
modulator for the information signal.
In the embodiment of Figure S, an optical
circulator 100 is used to couple spontaneous
emissions into the laser cavity. Unlike the
embodiment of Figure 4, wherein the same pump laser
was used for both the spontaneous emission source
and the laser cavity, separate pump lasers are
provided in the embodiment of Figure 5. Pump laser
9o is used to excite a fiber laser generally
designated 94. A grating 92 is used to set the
) 4
_ 20 -
lasing wavelength, and conventional mode selection
components 96 select a desired longitudinal mode.
The laser cavity extends between grating 92 and a
reflector 98, the output of which is coupled to a
first input port 102 of optical circulator 100.
A second pump laser 110 excites an active fiber
generally designated 114. A grating 112 selects the
wavelength of the spontaneous emission. The
spontaneous emissions are input to a second port 104
of optical circulator lO0. The spontaneous
emissions are coupled via circulator 100 to first
port 102, where they are fed back into laser cavity
94 via reflector 98, which passes the spontaneous
emission wavelength. The resultant broadened
optical signal is output via port 106 of optical
circulator lO0, to an optical isolator 108. The
optical circulator provides an efficient method for
coupling spontaneous emission into the laser cavity.
Figure 6 illustrates an embodiment of the
present invention wherein a ring cavity generally
designated 140 is used for the laser. Pump laser
120 is provided to excite the laser cavity. The
pump energy is coupled to the ring cavity via a
wavelength division multiplexer 122. An active
laser medium, for example an erbium doped fiber 141,
extends between wavelength division multiplexer 122
and a mode selector 124. A spontaneous emission
source generally designated 142 comprises a length
of erbium fi~er having a grating 144 for
r
-- 21 ~
establishing the wavelength of the spontaneous
emission. Pump laser 148 is provided to pump the
erbium fiber to produce the spontaneous emission.
The output of the spontaneous emission generator is
coupled to an optical circulator 126 via port 130.
The spontaneous emission is injected into the laser
cavity 140 via port 128 of the optical circulator.
The resultant laser output signal enters optical
circulator 126 via port 128, and outputs the
circulator via port 132. An optical coupler 134 is
used to output the laser signal via an optical
isolator 138. An optical isolator 136 is provided
within the laser ring cavity in a conventional
manner.
Another ring laser configuration is illustrated
in Figure 7. In this embodiment, pump laser 150
pumps the laser cavity 156. Mode selection is
provided by conventional components 154. An optical
circulator 158 receives spontaneous emissions from
source 168 via port 162. The spontaneous emission
source includes a pump laser 172, grating 170, and
active medium such as an erbium doped fiber 167.
Laser cavity 156 includes an active medium such as
erbium fiber 155 between the mode selector 154 and
optical circulator 158. The optical signal
generated by the laser cavity is input to port 160
of circulator 158 for output via port 164, optical
coupler 152, and optical isolator 166.
- 22 -
Spontaneous emission can also be used to broaden
the linewidth of a semiconductor laser signal.
Figure 8 illustrates an embodiment in accordance
with the present invention, wherein spontaneous
emission from an optical amplifier 184 is injected
into a semiconductor laser 180. In a preferred
embodiment, an optional optical filter 182 can be
provided to select the magnitude and spectral
property of the spontaneous emission fed back into
the laser. The injection of spontaneous emission
into laser 180 causes a line broadening as described
above. The optical signal produced by the laser is
output via an optical isolator 186.
Solid state or microchip lasers utilizing rare
earth laser systems can also be used in accordance
with the present invention. An example of such a
system is illustrated in Figure 9. An erbium
microchip laser 196 is co-doped with erbium
ytterbium (Yb3~) to facilitate pumping by pump laser
190 at 1.06 ~m. The pumping energy is coupled to
the microchip laser 196 via a lens 194 in a
conventional manner. A spontaneous emission source
generally desi-gnated 206 includes a pump laser 202,
grating 204, and an active medium 205 such as a
length of erbium fiber. As in the other
embodiments, grating 204 establishes the wavelength
of the spontaneous emissions. The spontaneous
emissions are coupled to the input of the microchip
laser via a wavelength division multiplexer 192.
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- 23 -
The wavelength of the microchip laser is
controlled by a coating on the chip and the pump
laser spot size, in a well known manner. For
example, the input surface 195 of the laser can have
a coating with high reflectivity at 1.5 ~m and a
high transmission at 1.06 ~m. In this example, the
coating on the output side 197 of the laser would
have a high reflectivity at 1.06 ~m and a low
reflectivity at 1.5 ~m. The broadened mode from
laser 196 is output via a lens 198, optical fiber
199, and optical isolator 200.
All of the laser embodiments illustrated in the
figures provide output signals with wide optical
line widths. These signals can be advantageously
used as optical carriers in communication systems,
by modulating the signals with an information signal
using an external modulator, such as a Mach Zehnder
modulator. The wide linewidth sources of the
present invention are applicable to any modulation
format which suffers from Brillouin gain. It should
be appreciated that although erbium laser systems
are used in the illustrated embodiments, the
inventive concepts may be applied to other laser
systems, including but not limited to neodymium
systems. The broadened optical signals provided in
accordance with the present invention reduce the
Brillouin threshold of the communication systems,
allowing higher launched power and therefore a
greater optical link budget. This advantage is
~ ~ ~2 3 0 ~
- 24 -
particularly useful in communication systems for
cable television applications, using VSB-AM signals.
It should now be appreciated that the present
invention provides apparatus and methods for
reducing the non-linear effects in link fiber by
increasing the optical linewidth of the signal
laser. In one illustrated embodiment, the optical
linewidth is increased by modulating the laser
output with broadband electrical noise using an
optical modulator. This spreads the linewidth to
reduce the effects of fiber non-linearities. Such
non-linearities may include four-wave mixing,
Brillouin gain and Raman gain. Other illustrated
embodiments utilize a periodic function, such as a
lS sine wave to externally or directly modulate a laser
to increase linewidth, or the injection of
spontaneous emission into the laser cavity to
achieve a broadened optical signal. Various
modulation formats will benefit from the broadened
linewidth sources, including VSB-AM, FM, PM, and
digital systems. The method and apparatus of the
present invention are effective for reducing any
fiber non-linear effect that depends on the optical
spectral density of the pump laser. As a result,
higher launch power can be accommodated.
3 ~ 4
. . .
- 25 -
Although the invention has been described in
- connection with a particular embodiment, those
skilled in the art will appreciate that numerous
modifications and adaptations may be made thereto
without departing ~rom the spirit and scope of the
invention as set forth in the claims.
