The present invention relates, in general, to generating communication signals. More specifically, the present invention relates to a system and method of generating single sideband, constant envelope, spread spectrum signals.
As an example of modern communication spread spectrum signals, the following is a description of known signals broadcast by Global Positioning System (GPS), which includes 24 satellites orbiting the Earth.
In GPS, each satellite broadcasts carrier signals on the same frequencies. Navigational data is spread by a clear acquisition (C/A) code and modulated on the L1 (1575.42 MHZ) in-phase channel. The navigational data is further spread by a P(Y) code and modulated on both the L1 quadrature and L2 (1227.60 MHZ) in-phase channels.
As both military and civilian requirements for GPS change, a condition which will likely continue into the 21st century, operational modifications become increasingly necessary. Many of these modifications revolve around the waveform structure of GPS.
One of the requirements that has changed since awarding of a contract for the next generation GPS satellites (Block IIF) is a requirement for an additional military signal on the same L band carrier as the C/A and P(Y) signals. An Interplex modulation technique is used to combine the three signals.
Interplex modulation is a technique for combining three or more signals to generate a constant envelope composite signal. A constant envelope composite signal is highly desirable, because it allows a highly efficient power amplifier to be utilized.
As an example, for three signals, S1, S2 and S3, Interplex modulation allows combining these signals into a phase modulated composite signal that maintains a constant envelope, thereby allowing the use of a high power amplifier without signal distortion. Taking these three signals, S1, S2 and S3, an Interplex modulator generates a composite signal that includes three desired components plus an unwanted cross-product.
Signals generated by Interplex modulation are single-carrier, double sideband signals, which have a serious shortcoming and restriction. It is often desired to generate, amplify, and transmit spread-spectrum signals having multiple carriers, with each carrier modulated by one or more spreading codes.
The present invention addresses this shortcoming by providing a composite signal that includes multiple carriers, with each carrier modulated by one or more spreading codes. Moreover, the present invention provides this composite signal as a constant-envelope, single-sideband signal, thereby resulting in systems with high power and spectral efficiency.
To meet this and other needs, and in view of its purposes, the present invention provides a method of generating a composite signal having the following steps: (a) generating a plurality of sub-carriers, each sub-carrier having a different frequency position in a frequency spectrum; (b) generating a plurality of codes; (c) forming a plurality of code combinations from the plurality of codes generated in step (b), wherein a code combination is comprised of at least one code from the plurality of codes; (d) first modulating each sub-carrier using a respective one of the code combinations formed in step (c) to form a plurality of modulated sub-carriers; and (e) second modulating in-phase and quadrature components of a base carrier using the plurality of modulated sub-carriers to form the composite signal having multiple carriers.
The composite signal of the method of the invention is a constant envelope signal. The composite signal is also a single sideband signal.
Step (a) of the method may include generating the plurality of sub-carriers at frequency positions of ƒm1, ƒm2, ƒm3, . . . ƒm
The method of the invention in step (c) may include forming the following code combinations: CC1(t), CC2(t), CC3(t) . . . CCN(t), where N is the number of code combinations, and CCi(t) is a code combination at frequency position ƒo+ƒi.
The code combinations of the method of the invention have to satisfy the following condition:
The composite signal produced by the method of the invention may have the following form:
Another embodiment of the present invention is a system for generating a composite signal of constant envelope having multiple carriers, each carrier including at least one spreading code. The system includes at least one signal generator for providing a plurality of individual sub-carriers, at least one code generator for forming a plurality of spreading codes and outputting combinations of the spreading codes as code combinations, and a base generator for forming in-phase and quadrature components of a base carrier. The system may also include a plurality of first mixers for, respectively, multiplying the plurality of sub-carriers with the code combinations to form a plurality of modulated sub-carriers, and second mixers for, respectively, multiplying the in-phase and quadrature components of the base carrier with the plurality of modulated sub-carriers. A combiner combines the multiplied in-phase and quadrature components of the base carrier to form the composite signal.
Yet another embodiment of the present invention is a system for generating a composite signal of constant envelope having multiple carriers. The system includes at least one signal generator for providing a plurality of in-phase carrier signals and quadrature carrier signals, and at least one code generator for forming a first set of code combinations and a second set of code combinations. The system may also include a first set of mixers for mixing the in-phase carrier signals with the first set of code combinations, and a second set of mixers for mixing the quadrature carrier signals with the second set of code combinations. A combiner combines output signals from the first set of mixers and the second set of mixers to form the composite signal. Each of the in-phase carrier signals have the form of cos(ω0+ωi)t, and each of the quadrature carrier signals have the form of sin(ω0+ωi)t, and ω0 corresponds to a base frequency and ωi corresponds to a sub-carrier frequency.
It is understood that the foregoing general description and the following detailed description are exemplary, but are not restrictive, of the invention.
The invention is best understood from the following detailed description when read in connection with the accompanying drawing. Included in the drawing are the following figures:
a is a plot of power versus frequency, illustrating a single carrier having a center carrier frequency of ƒo+ƒm, modulated by a particular code combination, in accordance with an embodiment of the present invention;
b is a plot of amplitude versus time of the signal whose spectrum is shown in
a is a plot of power versus frequency, illustrating two carrier signals, each modulated by a different code combination, in accordance with an embodiment of the present invention;
b is a plot of amplitude versus time, illustrating that the two carrier signal of
a is a plot of power versus frequency, illustrating four carrier signals, each modulated by a different code combination, in accordance with an embodiment of the present invention;
b is a plot of amplitude versus time showing that the four carrier signal of
When generating spread-spectrum signals, constant-envelope is a desirable property, because it allows operation of a high-power amplifier (HPA) in a transmitter that is performing in a most efficient mode. That is, the operating point of the HPA may be placed close to the 1-dB saturation point, instead of further backing away from the saturation point. Backing away from the saturation point is necessary for non-constant amplitude input signals, because the higher powered signals may saturate the amplifier.
The next generation of GPS satellites, for example, will use Interplex modulation as a combining technique for the modulating (or spreading) code signals. Interplex modulation is efficient for combinations of up to three code signals, and for some combinations of more than three code signals having particular power ratios.
A general form of an N-channel Interplex signal is
where sn(t)=dn(t)sq(ωnt)=±1 are code signals, and θn are phase modulation indices used to adjust power relationships among various codes. Furthermore, when a binary data stream dn(t)=±1 phase shift keys a unit amplitude square wave sq(ωnt)=±1 of frequency ωn, the result is again a binary wave.
In an exemplary implementation, for three codes that have equal power, the Interplex signal takes the following form:
z(t)=√{square root over (2P)}[P(t)+M(t)]cos2πƒot−√{square root over (2P)}[C(t)−C(t)P(t)M(t)]sin2πƒot (2)
where P(t), C(t), and M(t) are the GPS P-code, C/A-code, and M-code signals, respectively.
It will be appreciated that Interplex modulation makes the envelope of the signal in equation (2) a constant, through the introduction of a cross-product term, C(t)P(t)M(t). The signal envelope of (2) is as follows:
In deriving equation (3), the fact that the code powers are unity is used, as follows:
C2(t)=P2(t)=M2(t)=1 (4)
This follows because the amplitudes of the codes take on two values:
C(t)=±1, P(t)=±1, and M(t)=±1.
Signals generated by the Interplex method, using equation (1) are single-carrier, double sideband signals, which is a serious shortcoming. The present invention, as will be explained, overcomes this shortcoming by generating, amplifying, and transmitting spread-spectrum signals having multiple carriers, with each carrier modulated by one or more spreading codes. In addition, the present invention provides a constant-envelope signal having a single-sideband. Accordingly, the present invention advantageously results in systems having high power and spectral efficiency.
Using GPS as an example, the present invention may generate signals for the L2, L5, GLONASS, and Galileo band simultaneously (as shown in
As previously described, the Interplex method produces a single-carrier, double-sideband, constant envelope signal, but cannot generate multiple-carrier signals and cannot generate single sideband signals. The present invention, on the other hand, can generate a composite signal of multiple-carriers as a sideband in the single-sideband, suppressed carrier modulation scheme.
An exemplary embodiment of the present invention will now be described. The invention provides for the generation of a composite signal that may have an arbitrary number of carriers; that may have single-sideband frequency spectra; and may have a constant envelope. An underlying requirement of the invention is that code signals and sub-carrier signals, constituting the modulating signals, do not have overlapping spectra. Once this condition is fulfilled, a method of the invention arranges codes and cross-products of codes to modulate the sub-carriers, in a manner that produces a constant composite envelope signal.
It will be understood that multi-carrier as used by the present invention does not imply any relationship between carrier frequencies. In OFDM, for example, carriers have to be orthogonal, and in some MC-CDMA systems, carrier frequencies have to be integer multiples. In the present invention, however, carrier frequency values may be completely arbitrary, as they do not affect the operation.
A single sideband (SSB), amplitude modulated signal may be expressed as follows:
s(t)=√{square root over (2P)}m(t)cos2πƒot−√{square root over (2P)}{circumflex over (m)}(t)sin2πƒot (5)
where P is the total signal power, ƒo is the carrier frequency, and {circumflex over (m)}(t) is the Hilbert transform of the modulating signal m(t), and
where P.V. is a principle value (equation (6) has a discontinuity at t=s).
If m(t) and {circumflex over (m)}(t) are chosen in a manner that results in
m2(t)+{circumflex over (m)}2(t)=const (7)
then s(t) from equation (5) is a constant-envelope signal, and a SSB signal.
To illustrate a method of the invention, consider generating a modulated carrier at frequency ƒo+ƒm. The modulating signal then is a product of the sub-carrier signal of frequency
and a spreading code (or combination of codes), CC(t), resulting in
m(t)=CC(t)cosωmt (8)
According to Bedrosian's theorem, the Hilbert transform of m(t) from equation (8) is
{circumflex over (m)}(t)=CC(t)sinωmt (9)
with a condition that frequency ƒm (a sub-carrier) is greater than the highest component in the spectrum of the code signal CC(t).
Although, theoretically, this is not possible, since any spreading code (or combination of codes) has an infinite number of sidelobes in its spectrum, in a practical implementation it is sufficient that ƒm is greater than the code bandwidth. The bandwidth definition, as used herein, is the width of the signal spectrum's main lobe. In such definition, the GPS C/A code has 2-MHz bandwidth, and the P(Y) code has 20-MHz bandwidth.
Therefore, a single-carrier, SSB, constant-envelope composite signal has the following form:
s(t)=√{square root over (2P)}CC(t)cos(2πƒmt)cos(2πƒ0t)−√{square root over (2P)}CC(t)sin(2πƒot)=√{square root over (2P)}CC(t)cos2π(ƒo+ƒm)t (10)
As an example for CC(t), the invention may use a code combination similar to the code combination in equation (2) to obtain
s(t)=√{square root over (2P)}[C(t)−C(t)P(t)M(t)+P(t)+M(t)]cos(ωo+ωm)t (11)
The composite signal from equation (11) is single sideband, because it has no frequency components below ωo. The composite signal from equation (11) also has a constant envelope considering that
[C(t)−C(t)P(t)M(t)+P(t)+M(t)]2=4=const (12)
where the unity power property of code signals from equation (4) is used. The signal from equation (11) and its spectrum are shown in
It is important to understand that the code combination used in equation (11) is not the only combination of spreading codes and their cross-product terms that produces a constant-envelope signal. On the contrary, there are many combinations of codes and combinations of cross products that would produce the same result.
Obviously, the previous example is not a very interesting application of the method of the present invention, because the same result may be achieved using the Interplex method, by specifying ƒo+ƒm as the carrier frequency, instead of ƒo. However, a more interesting method of the present invention is developed next.
Another method of the present invention may be illustrated by using two or more carriers. The result of this method cannot be achieved by the Interplex method or any other known method. That is, the present invention forms an amplitude-modulated, single sideband, multi-carrier signal, where each of the carriers may be independently modulated with different spreading codes to produce a constant envelope composite signal.
A two-carrier signal implemented according to the method of this invention, has the following form:
s(t)=√{square root over (2P)}CC1(t)cosωm1t×CC2(t)cosωm2t]cosωot−√{square root over (2P)}[CC1(t)sinωm1t+CC2(t)sinωm2t]sinωot (13)
where CC1(t) and CC2(t) are two different code combinations. The signal in equation (13) is single sideband, because the amplitudes of the in-phase and quadrature carriers, namely,
[CC1(t)cosωm1t+CC2(t)cosωm2t]
and
[CC1(t)sinωm1t+CC2(t)sinωm2t]
respectively, are a Hilbert transform pair, considering equations (8) and (9). The single-sideband property is evident, when the expression in equation (13) is simplified, as follows:
s(t)=√{square root over (2P)}CC1(t)cos(ωo+ωm1)t+√{square root over (2P)}329 CC2(t)cos(ωo+ωm2)t (14)
It will be appreciated that the signal of equation (14) has no spectral components below ƒo.
The square of the envelope of the signal of equation (14) may be expressed as follows:
2P[CC1(t)cosωm1t+CC2(t)cosωm2t]2+2P[CC1(t)sinωm1t+CC2(t)sinωm2t]2=2P[CC12(t)+CC22(t)+CC1(t)CC2(t)cos(ωm1−ωm2)t] (15)
The envelope of this signal is a constant, if the following conditions are met:
CC12(t)+CC22(t)=const
CC1(t)CC2(t)=0 (16)
Next an example implementation will be described, where GPS spreading codes (for example) are desired. In this example, the C/A code is to be placed in a band with center frequency ƒo+ƒm1, and the P(Y) and M codes are to be placed in a band with center frequency ƒo+ƒm2. (As described previously, these center frequencies may be set independently to any desired value). The method of the invention may next form the following code combinations from the GPS spreading codes:
CC1(t)=C(t)−C(t)P(t)M(t)
CC2(t)=P(t)+M(t) (17)
Expression (13) may then be written, as follows:
s(t)=√{square root over (2P)}{[C(t)−C(t)P(t)M(t)]cosωm1t+[P(t)+M(t)]cosωm2t}cosωot−√{square root over (2P)}{[C(t)−C(t)P(t)M(t)]sinωm1t+[P(t)+M(t)]sinωm2t}sinωot (18)
The envelope of the signal of equation (18) is a constant, considering the derivation in equation (3). A method of the invention, in this example, introduced a cross-product of C(t)P(t)M(t) into CC1(t) to achieve necessary cancellations.
The signal of equation (18) and its spectrum are shown in
Before generalizing a method for the present invention, another example will now be provided that used four-carriers. For this example, the constant-envelope signal has the following form:
s(t)=√{square root over (2P)}[CC1(t)cosωm1t+CC2(t)cosωm2t+CC3(t)cosωm3t+CC4(t)cosωm4t]cosωot−√{square root over (2P)}[CC1(t)sinωm1t+CC2(t)sinωm2t+CC3(t)sinωm3t+CC4(t)sinωm4t]sinωot (19)
where CC1(t), CC2(t), CC3(t) and CC4(t) are code combinations that are desired at frequency positions ƒo+ƒm1, ƒo+ƒm2, ƒo+ƒm3 and ƒo+ƒm4 in the spectrum. The structure of this signal provides the single sideband property. After performing a calculation similar to the one in equation (15), it may be observed that in order to maintain the signal envelope constant, the following conditions have to be met:
CC12(t)+CC22(t)+CC32(t)+CC42(t)=const
CC1(t)CC2(t)=0
CC1(t)CC3(t)=0
CC1(t)CC4(t)=0
CC2(t)CC3(t)=0
CC2(t)CC4(t)=0
CC3(t)CC4(t)=0 (20)
a (spectrum) and 4b (composite constant envelope signal) show this four-carrier example with one possible arrangement of code combinations, as follows:
CC1(t)=C1(t)[1−C2(t)C3(t)][1−C4(t)C5(t)]
CC2(t)=[C2(t)+C3(t)][1−C4(t)C5(t)]
CC3(t)=[C4(t)+C5(t)][1−C2(t)C3(t)]
CC4(t)=C6(t)[1+C2(t)C3(t)][1+C4(t)C5(t)]
where C1(t), C2(t), C4(t) and C6(t) are C/A codes; C3(t) is a P(Y) code; and C5(t) is an M code. Instead of C/A, P(Y), and M, other codes may be used as well, such as codes to be implemented in the next generation GPS. It will be understood that this is just one of many possible arrangements, depending on a desired mixture of codes at a specific position in the spectrum. It is also possible to produce a new code using a majority vote. (Majority voting is a process of forming a resulting signal from an odd number of original code signals, which take values of +1 or −1, by taking a majority vote of the signals in every chip interval to determine the sign of the resulting signal.)
The carriers may be arbitrarily positioned in the spectrum. As an example of an arbitrary selection of four carriers,
Finally, as a general case, the present invention produces a single sideband, constant envelope, composite signal comprised of N carriers, having the following form:
where CCi(t) are code combinations at respective center frequency positions ƒo+ƒi. As defined herein, ƒo+ƒi is a carrier at center frequency position ƒo+ƒi, where ƒo is a base carrier and ƒi is a sub-carrier.
It will be appreciated that this generalized method of the present invention is completely backward compatible with the existing GPS system. In this manner, any standard receiver may receive signals generated by the present invention. Modifications of the GPS receiver or any GPS receiver updates are not necessary.
In general, the signal structure that provides the SSB property and the constant envelope signal are as follows:
Conditions shown in equation (22) do not restrict placement of any number of code signals, in any combination, on any of the carrier frequencies. These conditions just determine the type and number of additional cross-product terms necessary for term cancellations to provide a constant modulated signal envelope.
It will be further understood that the method of the invention is not restricted to the generation of GPS signals. Its theoretical basis is completely general and, therefore, its applicability is very broad. It may be used for generating spread-spectrum and non-spread-spectrum signals, in all circumstances where single sideband, constant envelope, multi-carrier signals are desired. Their use is advantageous in combination with high-power amplifiers, but their use is not restricted to such applications. The generalized method of the present invention is also applicable to both wireless and wired communications. GPS code signals have been used herein for illustrative purposes only, and codes other than the ones specified may be readily used by this method.
Referring now to
From the multiple individual codes generated by step 52, the method forms multiple code combinations by way of step 53. These multiple code combinations include at least one or more of the individual codes generated in step 52. For example, the code combinations may include CC1(t), CC2(t), . . . CCN(t).
Each of the code combinations formed in step 53 may now modulate, by way of step 54, a respective sub-carrier generated in step 51. For example, code combination CC1(t) may modulate sub-carrier cos(ω1t) and sin(ω1t). It will be appreciated that cos(ω1t) is the in-phase sub-carrier signal and sin(ω1t) is the quadrature sub-carrier signal. Both, however, have the same frequency.
As known, the in-phase sub-carrier signal and the quadrature sub-carrier signal are out-of-phase with respect to each other by 90 degrees.
As another example, code combination CC2(t) may modulate another sub-carrier of cos(ω2t) and sin(ω2t). It will be understood that sin(ω2t) is 90 degrees out-of-phase with respect to cos(ω2t). Both have the same frequency.
Each of the resulting modulated sub-carriers may next modulate, in step 55, a base carrier of ƒo to form multiple modulated carriers. Each of the multiple modulated carriers are formed at a center frequency position of ƒo+ƒmi. Similar to step 54, step 55 modulates the base carrier at cos(ωot) and sin(ωot). The base carrier of cos(ωot) and sin(ωot) are 90 degrees out-of-phase with respect to each other.
The method next combines the multiple modulated carriers to form a composite signal in step 56. It will be appreciated that (as best shown in
Referring next to
The in-phase modulated sub-carriers output from adder 67 are mixed with the in-phase base carrier at ƒo of cos(ω0t). This mixing, or modulating, is performed by mixer 69. Similarly, the quadrature modulated sub-carriers output from adder 68 are mixed, or modulated, with sin(ω0t) by way of mixer 70.
The output from mixer 69 and the output from mixer 70 are combined by adder 71 to form the composite signal of s(t).
Other embodiments of the invention will now be described with reference to
As an example of the embodiments shown in
s(t)=√{square root over (P)}CCI1(t)cos(ωo+ωm1)t+√{square root over (P)}CCQ1sin(ωo+ωm1)t+√{square root over (P)}CCI2cos(ωo+ωm2)t+√{square root over (P)}CCQ2sin(ωo+ωm2)t (23)
where CCI1(t) and CCI2(t) are code combinations modulating the in-phase carriers, and CCQ1(t) and CCQ2(t) are code combinations modulating the quadrature carriers.
After expanding the sine and cosine functions in equation (23) and grouping the terms, the following may be derived:
s(t)=√{square root over (2P)}[CCI1(t)cosωm1t+CCI2(t)cosωm2t+CCQ1(t)sinωm1t+CCQ2(t)sinωm2t]cosωot−√{square root over (2P)}[CCI1(t)sinωm1t+CCI2(t)sinωm2t−CCQ1(t)cosωm1t−CCQ2(t)cosωm2t]sinωot (24)
This composite signal is single-sideband, since the in-phase carrier amplitude of
[CCI1(t)cosωm1t+CCI2(t)cosωm2t+CCQ1(t)sinωm1t+CCQ2(t)sinωm2t] (25)
and the quadrature carrier amplitude of
[CCI1(t)sinωm1t+CCI2(t)sinωm2t−CCQ1(t)cosωm1t−CCQ2(t)cosωm2t] (26)
are Hilbert transform pairs, following the development from equations (8) and (9).
To determine the conditions for having a constant envelope signal, the expressions in equations (25) and (26) are squared and added. After grouping the terms, the square of the signal envelope becomes
2P{CCI12(t)+CCI22(t)+CCQq2(t)+CCQ22(t)+[CCI1(t)CCI2(t)+CCQ1(t)CCQ2(t)]cos(ωm1−ωm2)t−[CCI1(t)CCQ2(t)−CCI2(t)CCQ1(t)]sin(ωm1−ωm2)t (27)
It is clear that the expression in equation (25) may be constant, if the following conditions are imposed:
CCI12(t)+CCI22(t)+CCQ12(t)+CCQ22(t)=const
CCI1(t)CCI2(t)+CCQ1(t)CCQ2(t)=0
CCI1(t)CCQ2(t)−CCI2(t)CCQ1(t)=0 (28)
This represents the conditions that a two-carrier spread spectrum signal, generated by the present invention, has to meet in order to have a constant envelope.
In a general case, for N carriers, the resulting composite signal has the following form:
where CCI(t) and CCQ(t) are code combinations for spreading the in-phase and quadrature carrier components, respectively. CCI(t) and CCQ(t), in addition to containing pure codes, in general, also contain terms that are products of pure codes (these are usually called cross-products.)
By expanding the trigonometric functions in equation (29) and collecting the terms, the following expression is obtained:
The square of the envelope of the composite signal, from equation (28) is
From considerations similar to the considerations of equations (27) and (28), the following conditions need to be fulfilled:
and
CCIi(t)CCIj(t)+CCQi(t)CCQj(t)=0 (i=1, . . . , N; j=1, . . . , N; i≠j)
CCIj(t)CCQi(t)−CCIi(t)CCQj(t)=0 (33)
If these conditions are met, then the multi-carrier composite signal from equation (29) forms a constant envelope.
As previously described, these methods are not restricted to the generation of GPS signals. These methods may be used for generating spread-spectrum and non-spread-spectrum signals, in all circumstances where single sideband, constant envelope, multi-carrier signals are described. These methods are also applicable to both wireless and wired combinations.
Referring now to
The method in step 74 generates multiple codes. For example, the spreading codes may include individual GPS codes of the C/A code, P(Y) code and M code.
The method next, in step 75, forms a first set of code combinations from the multiple codes generated in step 74. For example, the first set of multiple code combinations may be CCI1(t), CCI2(t), . . . CCIN(t). Step 75 also forms a second set of code combinations from the multiple codes generated in step 74. For example, the second set of code combinations may include CCQ1(t), CCQ2(t), . . . , CCQN(t).
The method then enters step 76 and modulates the in-phase carrier signals with the first set of code combinations. For example, code combination CCI1(t) modulates the in-phase carrier of cos(ω0+ω1)t, as shown.
The method also enters step 77 and modulates the quadrature carrier signals with the second set of code combinations. For example, code combination CCQ1(t) modulates the quadrature carrier of sin(ω0+ω2)t, as shown.
The method finally enters step 78 and combines the modulated in-phase carrier signals and the modulated quadrature carrier signals to form the composite signal of s(t).
Referring next to
System 80 includes mixers 81, 82, 83, 84, 85 and 86. Each of the mixers separately multiplies a respective code combination with either an in-phase carrier or a quadrature carrier. The in-phase carriers, as shown, are cos(ω0+ω1)t, cos(ω0+ω2)t, . . . and cos(ω0+ωN)t. The quadrature carriers, as shown, are sin(ω0+ω1)t, sin(ω0+ω2)t, . . . and sin(ω0+ωN)t.
The output from mixers 81-86 are provided, respectively, to adder 87 and adder 88. Each adder combines the output of the modulated quadrature carrier signals and the modulated in-phase carrier signals. A final adder, designated 89, combines the respective outputs of adder 87 and adder 88 to form the composite signal of s(t).
Although the invention is illustrated and described herein with reference to specific embodiments, the invention is not intended to be limited to the details shown. Rather, various modifications may be made in the details within the scope and range of equivalents of the claims and without departing from the invention.
For example, other embodiments of the present invention may be seen in
Referring first to
System 100 of
It will be appreciated that system 90 of
Number | Name | Date | Kind |
---|---|---|---|
5920237 | Park et al. | Jul 1999 | A |
6009074 | Kim et al. | Dec 1999 | A |
6307892 | Jones et al. | Oct 2001 | B1 |
6335951 | Cangiani et al. | Jan 2002 | B1 |
6563881 | Sakoda et al. | May 2003 | B1 |
7039122 | Dragonetti | May 2006 | B2 |
7046739 | Pilcher | May 2006 | B2 |
20020075907 | Cangiani et al. | Jun 2002 | A1 |
20020150068 | Orr et al. | Oct 2002 | A1 |
20030072385 | Dragonetti | Apr 2003 | A1 |