U.S. patent application number 14/269102 was filed with the patent office on 2014-08-28 for wide-bandwidth signal canceller.
This patent application is currently assigned to PHOTONIC SYSTEMS, INC.. The applicant listed for this patent is Charles H. Cox, Kevin M. Cuomo. Invention is credited to Charles H. Cox, Kevin M. Cuomo.
Application Number | 20140242935 14/269102 |
Document ID | / |
Family ID | 44972871 |
Filed Date | 2014-08-28 |
United States Patent
Application |
20140242935 |
Kind Code |
A1 |
Cox; Charles H. ; et
al. |
August 28, 2014 |
Wide-Bandwidth Signal Canceller
Abstract
A signal canceller includes a dual-drive electro-optic modulator
having separate first and second electrical inputs. The first
electrical input is coupled to a first portion of a first signal
and the second electrical input is coupled to a second signal and
to a second portion of the first signal. A laser generates an
optical beam that propagates from the optical input to an optical
output of the electro-optic modulator. The dual-drive electro-optic
modulator modulates the optical beam with the first and second
portions of the first signal and with the second signal. The
modulation cancels at least some the first signal and generates a
modulation signal with reduced first signal modulation
component.
Inventors: |
Cox; Charles H.; (Carlisle,
MA) ; Cuomo; Kevin M.; (Carlisle, MA) |
|
Applicant: |
Name |
City |
State |
Country |
Type |
Cox; Charles H.
Cuomo; Kevin M. |
Carlisle
Carlisle |
MA
MA |
US
US |
|
|
Assignee: |
PHOTONIC SYSTEMS, INC.
Billerica
MA
|
Family ID: |
44972871 |
Appl. No.: |
14/269102 |
Filed: |
May 3, 2014 |
Related U.S. Patent Documents
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Application
Number |
Filing Date |
Patent Number |
|
|
12785437 |
May 22, 2010 |
8755750 |
|
|
14269102 |
|
|
|
|
Current U.S.
Class: |
455/302 |
Current CPC
Class: |
H04B 1/12 20130101; H04B
10/6973 20130101; H04B 1/525 20130101 |
Class at
Publication: |
455/302 |
International
Class: |
H04B 1/12 20060101
H04B001/12; H04B 10/69 20060101 H04B010/69 |
Claims
1-28. (canceled)
29. A signal canceller comprising: a. an optical subtractor having
separate first and second electrical inputs, the first electrical
input being coupled to a first portion of a first signal and the
second electrical input being coupled to a second signal and to a
second portion of the first signal; and b. a laser that is coupled
to an optical input of the optical subtractor, the laser generating
an optical beam that propagates from the optical input to an
optical output of the optical subtractor, the optical subtractor
modulating the optical beam with at least one of the first and
second portions of the first signal and with the second signal,
thereby generating an intensity modulated optical beam with a
reduced first signal modulation component compared with the first
signal coupled to the first and second electrical inputs.
30. The signal canceller of claim 1 wherein the first and second
portions of the first signal have substantially the same temporal
characteristics.
31. The signal canceller of claim 1 wherein the first and second
portions of the first signal have substantially the same amplitude
and phase characteristics.
32. The signal canceller of claim 1 wherein the first portion of
the first signal includes the same signal path delay as the second
portion of the first signal.
33. The signal canceller of claim 1 wherein an overlap integral of
the modulation and an optical mode of the electro-optic modulator
is selected so that the first and second portions of the first
signal substantially cancel during modulation.
34. The signal canceller of claim 33 wherein the first and second
portions of the first signal substantially cancel during modulation
when the first and second portions of the first signal are
substantially the same.
35. The signal canceller of claim 1 further comprising a coupler
that couples the first portion of the first signal into the first
input.
36. The signal canceller of claim 35 wherein the coupler couples a
portion of a transmission signal.
37. The signal canceller of claim 1 wherein the second input is
coupled to an antenna that receives the second signal.
38. A signal canceller comprising: a. a Mach-Zehnder
interferometric modulator comprising a first electrode
electromagnetically coupled to a first arm of the Mach-Zehnder
interferometric modulator and having an input coupled to a first
portion of a first signal and a second electrode
electromagnetically coupled to a second arm of the Mach-Zehnder
interferometric modulator and having an input coupled to a second
signal and to a second portion of the first signal; and b. a laser
that is coupled to an optical input of the Mach-Zehnder
interferometric modulator, the laser generating an optical beam
that propagates from the optical input to an optical output of the
Mach-Zehnder interferometric modulator, the Mach-Zehnder
interferometric modulator modulating the optical beam with the
first and second portions of the first signal and with the second
signal, the modulation cancelling at least some of the first
signal, thereby generating a modulation signal with reduced first
signal modulation component compared with the coupled first
signal.
39. The signal canceller of claim 38 wherein the Mach-Zehnder
interferometric modulator comprises a velocity matched Mach-Zehnder
interferometric modulator.
40. The signal canceller of claim 38 wherein the first and second
portions of the first signal have substantially the same temporal
characteristics.
41. The signal canceller of claim 38 wherein the first and second
portions of the first signal have substantially the same amplitude
and phase characteristics.
42. The signal canceller of claim 38 further comprising a coupler
that couples the first portion of the first signal into the first
input.
43. The signal canceller of claim 42 wherein the coupler couples a
portion of a transmission signal.
44. The signal canceller of claim 38 wherein the second input is
coupled to an antenna that receives the second signal.
45. A signal canceller comprising: a. a dual-drive electro-optic
modulator having a first electrical input being coupled to a first
portion of a first signal and a second electrical input being
coupled to a second signal and to a second portion of the first
signal; b. a laser that is coupled to an optical input of the
dual-drive electro-optic modulator, the laser generating an optical
beam that propagates from the optical input to an optical output of
the electro-optic modulator; and c. a signal processor having a
first input that is electromagnetically coupled to the optical
output of the electro-optic modulator, a second input that receives
a portion of the first signal, and an output that is coupled to the
first electrical input, the signal processor generating the first
portion of the first signal, the dual-drive electro-optic modulator
modulating the optical beam with the first and second portions of
the first signal and with the second signal, thereby generating an
intensity modulated optical beam with a reduced first signal
modulation component compared with the coupled first signal.
46. The signal canceller of claim 45 wherein the signal processor
comprises an adaptive signal processor.
47. The signal canceller of claim 45 wherein the signal processor
performs a recursive estimation to generate the first portion of
the first signal.
Description
[0001] The section headings used herein are for organizational
purposes only and should not to be construed as limiting the
subject matter described in the present application in any way.
INTRODUCTION
[0002] In many environments there are undesired electrical signals
present along with desired electrical signals. Often these
undesired electrical signals have significant power levels that can
interfere with the reception of the desired electrical signals.
Sometimes these electrical signals cannot be filtered when the
desired electrical signals are detected because they have the same
or nearly the same frequency as the desired electrical signals.
[0003] An example of systems where it is particularly difficult to
cancel the undesired electrical signals is wireless RF systems that
are co-located in a single platform, such as a ship or airplane.
The undesired signals often interfere with the ability to detect
and/or process the desired signals. In some systems, the magnitude
of the undesired signals is much greater than the magnitude of the
desired electrical signals. In these systems, it is typically
necessary to increase the dynamic range of components that must
process both the desired and the undesired electrical signals
beyond what would be required if only the desired electrical signal
was present. Increasing the dynamic range of components increases
the cost and sometimes the size of these systems.
BRIEF DESCRIPTION OF THE DRAWINGS
[0004] The present teaching, in accordance with preferred and
exemplary embodiments, together with further advantages thereof, is
more particularly described in the following detailed description,
taken in conjunction with the accompanying drawings. The skilled
person in the art will understand that the drawings, described
below, are for illustration purposes only. The drawings are not
necessarily to scale, emphasis instead generally being placed upon
illustrating principles of the teaching. The drawings are not
intended to limit the scope of the Applicant's teaching in any
way.
[0005] FIG. 1 is a block diagram of a known system for cancelling
or suppressing undesired electrical signals.
[0006] FIG. 2 is a block diagram of a photonic subtractor according
to the present teaching.
[0007] FIG. 3 is a block diagram of a co-site canceller including a
photonic subtractor according to the present teaching that is
configured to cancel transmitter signal leakage in the receive
signal path.
[0008] FIG. 4 is a block diagram of a photonic subtractor that
includes a signal processor according to the present teaching to
achieve more complete signal cancelation.
[0009] FIG. 5 illustrates results of a simulation that implements
the photonic subtractor with an adaptive signal processor according
to the present teaching.
DESCRIPTION OF VARIOUS EMBODIMENTS
[0010] Reference in the specification to "one embodiment" or "an
embodiment" means that a particular feature, structure, or
characteristic described in connection with the embodiment is
included in at least one embodiment of the teaching. The
appearances of the phrase "in one embodiment" in various places in
the specification are not necessarily all referring to the same
embodiment.
[0011] It should be understood that the individual steps of the
methods of the present teachings may be performed in any order
and/or simultaneously as long as the teaching remains operable.
Furthermore, it should be understood that the apparatus and methods
of the present teachings can include any number or all of the
described embodiments as long as the teaching remains operable.
[0012] The present teaching will now be described in more detail
with reference to exemplary embodiments thereof as shown in the
accompanying drawings. While the present teachings are described in
conjunction with various embodiments and examples, it is not
intended that the present teachings be limited to such embodiments.
On the contrary, the present teachings encompass various
alternatives, modifications and equivalents, as will be appreciated
by those of skill in the art. Those of ordinary skill in the art
having access to the teaching herein will recognize additional
implementations, modifications, and embodiments, as well as other
fields of use, which are within the scope of the present disclosure
as described herein.
[0013] FIG. 1 is a block diagram of a known signal canceling system
100 for cancelling or suppressing undesired electrical signals. The
apparatus shown in FIG. 1 is typical of a system platform, such as
an aircraft or ship, where one or more transmitting antennas are
positioned in relatively close proximity to reception or
transceiver antennas that receive electrical signals with
relatively low power levels. In the system shown in FIG. 1, a
transmitter 102 is coupled to a transmission antenna 104 that
radiates an electrical transmission signal with a relatively high
power level compared with typical reception signals. A reception
antenna 106 is positioned to receive the desired reception signal.
However, in practice the reception antenna 106 receives both the
desired reception signal and a portion of the undesirable
electrical transmission signal that is delayed by a signal path
delay delta 108 as shown in FIG. 1.
[0014] The canceling system 100 includes a subtractor 110. A
subtractor is defined herein as any component or system that
cancels the undesirable transmission signal from a reception signal
that includes a combination of the desired reception signal and an
undesirable transmission signal. The subtractor 110 shown in FIG. 1
includes a coupler 112 that is positioned to couple a sample or
small portion of the undesirable transmission signal. The output of
the coupler 112 is electrically connected to a signal input of a
controller 114. A second coupler 116 is used to couple a sample or
small portion of the output signal generated by the subtractor 110.
The output of the second coupler 116 is electrically connected to
an error signal input of the controller 114.
[0015] The controller 114 processes the sample of the undesirable
transmission signal from the subtractor 110 and then adjusts the
magnitude and the phase of the sample of the undesired transmission
signal to substantially equal the magnitude and phase of the actual
undesired transmission signal received at the reception antenna
106. Ideally, the controller 114 generates a signal that when
subtracted from the desired receive signal Rx in the subtractor 110
results in the elimination of the undesired signal. However, there
are typically several factors that contribute to less than perfect
signal cancellation of the undesired transmission signal in the
subtractor 110.
[0016] One of the factors that contribute to less than perfect
signal cancellation of the undesired transmission signal is the
signal path delay delta 108 between the transmission antenna 104
and the reception antenna 106. Compensating for the signal path
delay delta 108 is difficult because the signal path delay 108
depends upon the particular location of the equipment, which may
not always be a fixed location. The reception equipment must then
be modified to compensate for the particular signal path delay 108.
Furthermore, many practical systems have multiple signal path
delays. In such systems, it is not usually possible to totally
compensate for all the signal path delays.
[0017] For many systems of practical interest that have undesirable
signals at significant powers levels, it is possible to avoid the
limitations caused by the true time delay between the transmission
antenna 104 and the reception antenna 106 by converting the true
time delay to a phase change. It is known in the RF art that one
can substitute a phase change for the true time delay if the signal
bandwidth is small enough. In the system shown in FIG. 1, a vector
modulator 118 is used to adjust the phase and magnitude of the
undesired transmission signal to compensate for the true time
delay. However, as the bandwidth of the undesired transmission
signals increases, the degree of cancellation will degrade with
phase shift and it will become necessary to compensate for the true
time delay. Current state-of-the art ultra-broadband transmissions
will require at least some compensation for the true time
delay.
[0018] In addition, as the bandwidth of the undesired transmission
signal increases, the bandwidth of the subtractor 110 becomes a
significant limitation and consequently the subtractor 110 is not
able to fully cancel the undesirable transmission signal. The
subtractor 110 is often implemented as a directional coupler. Such
directional couplers have bandwidths that are limited to about a
decade of bandwidth. In many state-of-the art systems, signal
cancellation needs to be performed over two, three, or even more
decades of bandwidth.
[0019] One aspect of the present teaching relates to using an
electro-optical modulator and various signal processing algorithms
executing on signal processor hardware to cancel or suppress
undesired electrical signals over a wide signal bandwidth. One
feature of the methods and apparatus of the present teaching is
that cancelation can be accomplished even when the undesirable
signals overlap with the desired signal in time and/or frequency
and without the need for a physical time delay. In one aspect of
the present teaching, a dual-drive electro-optic modulator is used
to achieve wide-bandwidth signal cancelation.
[0020] FIG. 2 is a block diagram of one embodiment of a photonic
subtractor 200 according to the present teaching. In one
embodiment, the photonic subtractor 200 includes a dual-drive
electro-optic modulator 202. A laser 204 is optically coupled to an
optical input of the dual-drive electro-optic modulator 202. In
some embodiments, an optical detector 206 is optically coupled to
the output coupler 208 of the dual-drive electro-optic modulator
202 to convert the modulated optical output signal to an electrical
signal. The dual-drive electro-optic modulator 202 includes a first
electrode 210 that is coupled to a signal comprising the
combination of the desired and the undesired electrical signal. In
addition, the dual-drive electro-optic modulator 202 includes a
second electrode 212 that is coupled to only the undesired
electrical signal.
[0021] Dual-drive electro-optic modulators are well known in the
electro-optic art. Dual-drive electro-optic modulators are
sometimes configured so that a single modulation signal is applied
to both of the dual-drive electrodes. The conventional
configuration of a dual-drive electro-optic modulator includes a
180 degree phase shifter coupled to one of the dual-drive
electrodes so that the electrical modulation experienced by a
modulation signal applied to one of the dual-modulation drive
electrodes is the negative of the electrical modulation experienced
by a modulation signal applied to the other one of the dual-drive
electrodes. The output coupler of the dual-drive electro-optic
modulator takes the difference between the modulated light from the
two branches of the modulator. The dual-drive electro-optic
modulator can also be designed to impart differential modulation on
the first electrode 210 relative to the second electrode 212. In
such a design, the output coupler 208 takes the difference between
the modulated light from the two branches of the modulator, which
is effectively the sum of the modulated light from the two branches
of the modulator. Thus, the output modulation signal is the sum of
the modulation signals applied to the dual-drive electrodes.
[0022] The photonic subtractor 200 does not include the 180 degree
phase shifter that is typically used in dual-drive electro-optic
modulators. Thus, the desired signal together with the undesired
signal is applied to one of the dual-drive modulator electrode,
while the undesired signal alone is applied to the other dual-drive
electrode. Therefore, the same phase of the undesired electrical
signal is applied to both of the dual-drive electrodes. The output
coupler 208 of the photonic subtractor 200 takes the difference
between the modulation on the two branches of the optical modulator
202, thus cancelling out the undesired signal and leaving only the
desired signal to propagate to the optical detector 206.
[0023] The present teachings are described in connection with
cancelling a transmission signal that has leaked into the receive
signal path. However, one skilled in the art will appreciate that
the apparatus and methods of the present teaching can be used in
any application where an undesirable signal is present in the
receive signal path. For example, there are many transceiver
systems where a portion of a transmission signal leaks into the
receive signal path. The magnitude of the transmission leakage
signal is typically much less than the full power transmit signal.
However, the magnitude of the transmission leakage is often much
larger than the desired receive signal.
[0024] A common platform where such transmit and receive signal
levels are present is an aircraft or ship. On aircrafts and ships,
there are often several transmitters and receivers located in close
proximity to each other. Even though the transmit antenna of one
system might have a directional radiation pattern that is aimed in
a different direction from the receive antenna of another system,
such a configuration typically would provide only about 30 to 40 dB
of isolation between the transmitter and receiver systems. For
example, if the transmitter is radiating 10 W, a transmit signal
with a power of 1 mW (or 0 dBm) is leaking into the receive path.
For a receiver with a minimum sensitivity on order of -170 dBm, the
undesired transmit leakage signal is very much larger than the
desired receive signal.
[0025] FIG. 3 is a block diagram of a co-site canceller 300
including a photonic subtractor according to the present teaching
that is configured to cancel transmitter signal leakage in the
receive signal path. The co-site canceller 300 includes a
dual-drive electro-optic modulator 302. A laser 304 is optically
coupled to an optical input of the dual-drive electro-optic
modulator 302. The laser 304 generates an optical carrier signal.
An optical detector 306 is optically coupled to the output coupler
308 of the dual-drive electro-optic modulator 302. The optical
detector 306 generates an electrical signal related to the output
of the dual-drive electro-optic modulator 302.
[0026] A receive antenna 310 is coupled to an electrode 312 of the
dual-drive electro-optic modulator 302. A transmitter 314 having an
output coupled to a transmission antenna 316 is positioned
proximate to the receive antenna 310. A coupler 318 is positioned
proximate to the output of the transmitter 314 to couple a first
portion of a first electrical signal, which in this example is a
sample of the transmitter signal Tx.sub.T. The output of the
coupler 318 is electrically connected to an electrode 320 of the
dual-drive electro-optic modulator 302. When the two modulated
signals combine at the modulator output coupler 308, the receive
signal Rx and the combination of the receive signal and the sample
of the transmit signal Tx.sub.T are modulated onto the optical
carrier. Total cancellation of the undesired signal will occur when
both the magnitude and phase of Tx.sub.R equal the magnitude and
phase of Tx.sub.T.
[0027] The receive antenna 310 is intended to pick up the desired
receive signal Rx, which in this example is a second electrical
signal. However, in practice the receive antenna 310 also picks up
some of the undesired transmit signal Tx.sub.R from the transmitter
314 located proximate to the receive antenna 310, which in this
example is a second portion of the first electrical signal. In some
systems, the undesired transmit signal Tx.sub.R (second portion of
the first electrical signal) has the same or nearly the same
frequency as the desired receive signal Rx (second electrical
signal). The power of the desired receive signal Rx (second
electrical signal) is often much less than the power of the
undesired transmit signal Tx.sub.R (second portion of the first
electrical signal). Therefore, there is a need to cancel the
undesired transmit signal Tx.sub.R (second portion of the first
electrical signal) received by the receive antenna 310. One skilled
in the art will appreciate that although only one path between the
transmission antenna 316 and receive antenna 310 is shown and
described in connection with FIG. 3, in practical systems there can
be numerous paths between the transmission antenna 316 and receive
antenna 310.
[0028] A general method of cancelling a signal according to the
present teaching includes coupling a first portion of a first
electrical signal into a first electrical input of a dual-drive
electro-optic modulator. A second portion of a first electrical
signal and a second electrical signal is coupled into a second
electrical input of the dual-drive electro-optic modulator. In the
example described in connection with FIG. 3, the first portion of a
first electrical signal is the sample of the transmit signal
Tx.sub.T, the second portion of a first electrical signal is the
transmit leakage signal Tx.sub.R, and the second electrical signal
is the receive signal Rx.
[0029] An optical beam is generated that propagates from the
optical input to an optical output of the electro-optic modulator.
The optical beam is modulated with the first and second portions of
the first signal and with the second signal. The modulation at
least partially cancels the first and second portions of the first
electrical signal, thereby generating a modulation signal with
reduced first signal modulation.
[0030] One limitation of the co-site canceller 300 is that it
requires applying the undesired signal alone without any of the
desired signal to one of the dual-drive electrodes. Fortunately, in
many practical applications of wide-bandwidth signal cancellers,
such as transceivers and co-located transmitters and receivers, it
is possible to isolate the undesired electrical signal from other
signals.
[0031] Another limitation of the co-site canceller 300 is that it
requires that the modulation of the optical signal by the
combination of the desired electrical signal and the undesired
electrical signal on one dual-drive electrode and the modulation of
the optical signal by the undesired electrical signal alone on the
other dual-drive electrode be equal to achieve compete or near
complete signal cancelation. Thus, cancellation of the undesired
signal at the optical output coupler 308 of the co-site canceller
300 requires that one of the electrodes of the optical modulator
302 receive an accurate copy of the undesired signal with the same
temporal characteristics as the undesired signal applied to the
receiving antenna 310. However, the exact amplitude, phase, and
time delay of the undesired electrical signal Tx.sub.R at the
receiving antenna 310 is not typically known.
[0032] Another limitation of the co-site canceller 300 is that
there may be multiple paths of the undesired signal caused by
reflections or caused by the distributed nature of the antennas
themselves, which results in delays or echoes in the second portion
of a first electrical signal which changes the second portion of a
first electrical signal relative to the first portion of the
electrical signal. For example, there are often multiple paths of
reflections between the transmitter antenna 316 and the receiver
antenna 310 that changes the transmit leakage signal Tx.sub.R
relative to the sampled transmitter signal Tx.sub.T. In addition,
there are sometimes changes in the signal path length or
propagation medium between the transmitter antenna 316 and the
receiver antenna 310 that can result in amplitude and/or phase
variations, which is sometimes referred to in the art as channel
fading.
[0033] Another limitation of the co-site canceller 300 is that the
degree of modulation that each of the dual-drive electrodes imparts
on the optical signal is different for different electrodes. For
example, the degree of modulation that each of the dual-drive
electrodes imparts on the optical signal is a function of the
overlap integral of the RF modulation and the optical mode. Each
particular modulator has a unique overlap integral for each of the
dual-drive electrode and these overlap integrals are not exactly
the same. Furthermore, the overlap integrals are fixed when the
modulator is fabricated and cannot be changed to balance the degree
of modulation. In addition, the electrical loss in the cables
connecting to the dual-drive electrodes is not exactly equal
because of difference in length and/or manufacturing. Therefore,
there are differences in the degree of modulation that each of the
dual-drive electrodes imparts on the optical signal because of
differences in the electrical characteristics of the cables
connecting each of the dual-drive electrodes.
[0034] Consequently, there is a need to improve the co-site
canceller 300 so that it cancels not just one undesired signal of
fixed amplitude and phase but multiple undesired signals each with
a different amplitude and phase that is not known and not
necessarily fixed over time. In addition, there is a need to
improve the co-site canceller 300 so that it compensates for
different degrees of modulation that each of the dual-drive
electrodes imparts on the optical signal.
[0035] One aspect of the present teaching is to use a signal
processor, such as an adaptive signal processor, to adjust the
signal parameters of the sample of the transmit signal Tx.sub.T to
achieve more complete signal cancellation. For example, signal
processing can be used to adjust the amplitude, phase and/or time
delay of the undesired modulation signal to achieve more complete
signal cancellation.
[0036] FIG. 4 is a block diagram of a co-site canceller 400 that
includes a signal processor according to the present teaching that
achieves more complete signal cancellation. The co-site canceller
400 is similar to the co-site canceller 300 that was described in
connection with FIG. 3. However, the co-site canceller 400 includes
a signal processor 402, such as an adaptive signal processor. A
coupler 404 is positioned proximate to the output of the
transmitter 406, which is coupled to a transmit antenna 405. The
output of the coupler 404 is electrically connected to an input of
the signal processor 402.
[0037] An optical coupler 408 is positioned proximate to the output
of an optical modulator 410. The output of the optical coupler 408
is optically coupled to an optical detector, such as a photodiode
409. The electrical output of the photodiode 409 is electrically
connected to a control input of the signal processor 402. A
receiving antenna 412 is coupled to a first electrode 414 of a
dual-drive electro-optic modulator 414. An output of the signal
processor 402 is electrically connected to a second electrode 416
of the dual-drive electro-optic modulator 410.
[0038] In operation, the signal processor 402 samples the
transmitter signal Tx.sub.T and the modulated optical signal and
uses an algorithm to derive a compensation signal which improves or
optimizes the cancellation performance of the co-site canceller
400. Enhanced signal cancellation is achieved because the adaptive
signal processor produces an output signal which rapidly converges
to a signal that is identical to or nearly identical to the
transmit leakage signal Tx.sub.R. In particular, the adaptive
signal processor estimates and corrects for any unknown amplitude,
phase, or delay variations between the undesired leakage signal at
the receiver Tx.sub.R and the sample of the transmitter signal
Tx.sub.T at the transmitter. Such discrepancies between the
transmitter and receiver signals would almost always occur in
practical systems and will result in less than perfect signal
cancelation.
[0039] A method according to the present teaching that includes
adaptive signal processing can include modifying the first portion
of the first electrical signal, which is the sample of the transmit
signal Tx.sub.T in the example described in connection with FIG. 3.
The step of modify the first portion of the first electrical signal
can include recursively estimating the first portion of the first
electrical signal using the output of the optical modulator 410. In
particular, the step of modify the first portion of the first
electrical signal can include generating a first portion of the
first electrical signal that has substantially the same amplitude
and phase variation as the second portion of the first signal that
is applied to the second electrical input. The step of modify the
first portion of the first electrical signal can also include
generating a first portion of the first electrical signal that has
substantially the same time delay as the second portion of the
first signal. The step of modify the first portion of the first
electrical signal can also include compensating for a signal path
delay in the first and second portions of the first signal. In
addition, the step of modify the first portion of the first
electrical signal can include modifying the first portion of the
first electrical signal so that the first and second portions of
the first electrical signal are substantially canceled in the
optical subtractor.
[0040] In one embodiment of the present teaching, the signal
processor 402 is implemented as an analog or a digital adaptive
signal processor. In one particular embodiment, the adaptive signal
processor is implemented as a digital filter as described herein.
However, one skilled in the art will appreciate that the adaptive
signal processor can be implemented with numerous types of
devices.
[0041] In one method of implementing the adaptive signal processor
402 as a digital filter, the adaptive signal processor 402 computes
a compensation signal {circumflex over (T)}x.sub.R[n] that is a
linear combination of the input signal samples, Tx.sub.T[n] at each
time sample n. Mathematically, {circumflex over (T)}{circumflex
over (x)}.sub.R[n] represents the output of a digital filter, which
is described by {circumflex over (T)}x.sub.R[n]=w.sup.HTx.sub.T[n],
where w denotes a vector of unknown filter weights to be estimated
and
Tx.sub.T[n]=[Tx.sub.T[n] Tx.sub.T[n-1] . . .
Tx.sub.T[n-P+1]].sup.T
denotes a vector of input transmit signal samples where the
variable P denotes the filter length. The operator "H" is the
Hermition transpose. The adaptive signal processor 402 implements
an algorithm that recursively estimates w in a way that minimizes
the error signal e[n]=Tx.sub.R[n]-{circumflex over (T)}x.sub.R[n]
at each time step, n. Note that the expression for the error signal
e[n] is a function of the unknown filter weights w since the output
signal {circumflex over (T)}x.sub.R[n] is a function of the filter
weight w.
[0042] One skilled in the art of adaptive signal processing will
recognize that the recursive least-squares solution for the filter
weight w that minimizes the error signal e[n] at each instant in
time is given by w[n]=w[n-1]+g[n]e*[n-1], where the symbol "*"
represents conjugation. The equation for the filter weight w
recites that the correction applied to the filter weights at each
instant in time is proportional to the measured error signal at the
previous time step e[n-1] multiplied by a gain vector g[n]. The
gain vector g[n] used here is similar to the "Kalman filter" gain
that is used to solve many recursive estimation problems. This gain
vector is computed recursively from the known transmit signal
vector Tx.sub.T[n] as follows.
g[n]=P[n-1]Tx.sub.T[n][.lamda.+Tx.sub.T.sup.H[n]P[n-1]Tx.sub.T[n]].sup.--
1
P[n]=.lamda..sup.-1P[n-1]-g[n]Tx.sub.T.sup.H[n].lamda..sup.-1P[n-1]
where P[n] is the covariance matrix associated with the current set
of adaptive filter weights w[n] and .lamda. is a tunable
"forgetting factor" parameter that weights new data relative to old
data and thus allows the filter to robustly adapt to changing input
signal conditions.
[0043] FIG. 5 illustrates results of a simulation 500 that
implements the co-site canceller 400 with an adaptive signal
processor according to the present teaching. The first waveform in
the simulation 500 is the desired received signal (or message) 502,
which is a simple sine wave. The second waveform in the simulation
500 is the transmitter leakage signal 504, which in the simulation
500 is a broadband noise waveform. The third waveform in the
simulation 500 is the actual received signal 506, which is a
combination of the desired signal and the received transmit leakage
and echo signals. The actual received signal 506 is assumed to
contain an echo of unknown amplitude and time delay. In the
simulation shown in FIG. 5, the actual received signal as a
function of time can be represented by the following equation:
Rx Signal(t)=Desired Signal(t)+Transmit Leakage(t)-0.5*Transmit
Leakage(t-.DELTA.t).
[0044] As described in connection with FIGS. 3 and 4, in order for
the photonic canceller to recover the desired signal, a copy of the
transmit leakage signal with the echo signals of unknown amplitude
and time delay needs to be applied to the second electrode 412 of
the dual-drive electro-optic modulator 410.
[0045] The adaptive signal processor 402 processes a sample of the
transmit signal that is available at the transmitter site and
accurately estimates the amplitude and time delay of the echo
signal present at the receiver antenna. After a brief transient,
the adaptive signal processor 402 generates a compensation signal
that is approximately represented by:
{circumflex over (T)}x.sub.R[n]=Transmit Leakage(t)-0.5*Transmit
Leakage(t-.DELTA.t).
When the compensation signal is applied to the second electrode of
the dual-drive electro-optic modulator, optical subtraction occurs
and consequently the desired message is cleanly recovered. The
fourth waveform 508 illustrates the recovered message.
[0046] Thus, the photonic canceller with the adaptive signal
processor according to the present teaching can automatically
compensate for any unknown delays, amplitude, or phase variations
between the transmitter and receiver signals. One skilled in the
art will appreciate that the adaptive signal processing described
in connection with FIGS. 4 and 5 is not limited to photonic signal
cancelling devices.
EQUIVALENTS
[0047] While the applicant's teaching are described in conjunction
with various embodiments, it is not intended that the applicant's
teaching be limited to such embodiments. On the contrary, the
applicant's teaching encompass various alternatives, modifications,
and equivalents, as will be appreciated by those of skill in the
art, which may be made therein without departing from the spirit
and scope of the teaching.
* * * * *