The present disclosure relates generally to wireless communications and more specifically to a phase-reconfigurable circuit with dynamic phase modulation for wideband dual-input power amplifiers.
The orthogonal frequency division modulation (OFDM) used in modern telecommunication systems such as 5G efficiently use bandwidth but at the price of a relatively high peak-to-average power ratio (PAPR). The high PAPR complicates the power amplifier design for such systems. For example, if the power amplifier is biased for good efficiency at the average power of the transmitted signal, the power amplifier may then clip or saturate during the moments of peak power so as to cause non-linearities. Conversely, if the power amplifier is biased for good efficiency at the peak power, the power amplifier is then inefficient at the average power level. A traditional power amplifier for OFDM signals would thus have to choose between good linearity but poor efficiency or high efficiency but poor linearity.
To have both high efficiency and high linearity in the same system, dual-input amplifiers such as Doherty amplifiers have been developed that include both a carrier amplifier and a peaking amplifier. Doherty amplifiers require a phase-reconfigurable circuit for splitting and phase shifting the input signal to drive the peaking and carrier amplifiers and also an output network to combine the output signals from the peaking and carrier amplifiers. In a traditional Doherty amplifier, the phase-reconfigurable circuit phase shifts the input signal to the peaking amplifier by −90° as compared to the input signal to the carrier amplifier. To enhance performance, generalized Doherty amplifiers have been developed in which the phase shift is no longer set to −90° but instead may be tuned to any suitable value.
The following summary discusses some aspects of the present disclosure to provide a basic understanding of the discussed technology. This summary is not an extensive overview of all contemplated features of the disclosure and is intended neither to identify key or critical elements of all aspects of the disclosure nor to delineate the scope of any or all aspects of the disclosure. Its sole purpose is to present some concepts of one or more aspects of the disclosure in summary form as a prelude to the more detailed description that is presented later.
In accordance with an aspect of the disclosure, a dual-input amplifier with dynamic phase modulation is provided that includes: an envelope detector configured to process an envelope of an RF input signal to form an envelope signal; a single-ended-to-differential converter configured to convert a version of the RF input signal into a differential RF input signal; an I/Q generator circuit configured to convert the differential RF input signal into a differential in-phase signal and into a differential quadrature-phase signal; a first vector-sum phase-shifter; a second vector-sum phase-shifter; a first pair of output terminals; and a second pair of output terminals, wherein the first vector-sum phase-shifter and the second vector-sum phase shifter are configured to process the differential in-phase signal and the differential quadrature-phase signal to form a first differential output signal at the first pair of output terminals and to form a second differential output signal at the second pair of output terminals and to adjust a phase difference between the first differential output signal and the second differential output signal responsive to the envelope signal.
In accordance with another aspect of the disclosure, a dual-input amplifier method is provided that includes: converting an RF input signal into a differential in-phase signal and a differential quadrature-phase signal; processing the differential in-phase signal and the differential quadrature-phase signal to form a first differential output signal and a second differential output signal, wherein the first differential output signal has a phase difference with respect to the second differential output signal; and adjusting the phase difference responsive to a power of the RF input signal.
In accordance with yet another aspect of the disclosure, a dual-input amplifier is provided that includes: a pair of vector-sum phase-shifters configured to dynamically modulate a phase difference between a first differential output signal and a second differential output signal responsive to a power of an input RF signal; a first differential-to-single-ended converter configured to convert the first differential output signal into a first single-ended output signal; a first driver amplifier configured to amplify the first single-ended output signal to form a first driver output signal; and a first power amplifier configured to amplify the first driver output signal to form a first power amplifier output signal.
Finally, in accordance with another aspect of the disclosure, a transmitter is provided that includes: a delay and impedance matching circuit configured to delay an RF input signal into a delayed matched signal; a pre-amplifier configured to amplify the delayed matched signal to form an amplified input signal; a single-ended-to-differential conversion circuit configured to convert the amplified input signal into a differential input signal; a polyphase filter configured to convert the differential input signal into a differential in-phase signal and a differential quadrature-phase signal; a first vector-sum phase-shifter and a second vector-sum phase shifter both configured to process the differential in-phase signal and the differential quadrature-phase signal to form a first differential output signal and a second differential output signal and to dynamically modulate a phase difference between the first differential output signal and the second differential output signal responsive to a power of the RF input signal; a first differential-to-single-ended conversion circuit configured to convert the first differential output signal to form a first single-ended output signal; a second differential-to-single-ended conversion circuit configured to convert the second differential output signal to form a second single-ended output signal; one or more first amplifiers configured to amplify the first single-ended output signal to form a first amplified RF signal; one or more second amplifiers configured to amplify the second single-ended output signal to form a second amplified RF signal; and a combiner configured to combine the first amplified RF signal and the second amplified RF signal to form a combined RF output signal.
Other aspects, features, and implementations of the present disclosure will become apparent to those of ordinary skill in the art, upon reviewing the following description of specific, exemplary implementations of the present disclosure in conjunction with the accompanying figures. While features of the present disclosure may be discussed relative to certain implementations and figures below, all implementations of the present disclosure can include one or more of the advantageous features discussed herein. In other words, while one or more implementations may be discussed as having certain advantageous features, one or more of such features may also be used in accordance with the various implementations of the disclosure discussed herein. In similar fashion, while exemplary implementations may be discussed below as device, system, or method implementations it should be understood that such exemplary implementations can be implemented in various devices, systems, and methods.
The accompanying figures, where like reference numerals refer to identical or functionally similar elements throughout the separate views and which together with the detailed description below are incorporated in and form part of the specification, serve to further illustrate various implementations and to explain various principles and advantages in accordance with the present disclosure.
Implementations of the present disclosure and their advantages are best understood by referring to the detailed description that follows. It should be appreciated that like reference numerals are used to identify like elements illustrated in one or more of the figures.
To improve the efficiency and linearity of Doherty amplifiers, phase-reconfigurable circuits has been developed in which the phase difference between the input signal to the carrier amplifier and the input signal to the peaking amplifier may be set to an arbitrary value. Although such a variable input phase difference is beneficial, challenges remain with respect to the linearity of a Doherty amplifier. The linearity of a Doherty power amplifier may be characterized in a number of ways. For example, a first measure of linearity is known as an AM-AM measurement, where AM denotes amplitude modulation. In an AM-AM characterization of an amplifier, the input signal is an unmodulated sinusoid. The output sinusoid should have a linear relationship to this input sinusoid but as the input signal power is increased, eventually the output sinusoid will have a non-linear distortion with respect to the input sinusoid. An AM-AM measurement characterizes this non-linear distortion. Another measure of linearity is known as an AM-PM measurement, where PM denotes phase modulation. A sinusoid is again input to the power amplifier and the input power gradually increased. A phase of the output signal should stay steady but will inevitably begin to change as the input power is increased. The AM-PM measurement characterizes the linearity of the output phase as a function of the input signal power.
Load modulation perturbs the desired flatness of the AM-AM and AM-PM performance of a Doherty amplifier despite the use of a phase-reconfigurable input circuit providing an arbitrary phase difference between the carrier and peaking input signals. In addition, the instantaneous peak power of a Doherty amplifier is lowered by the class C biasing of the peaking amplifier to facilitate load modulation. A Doherty amplifier is thus disclosed herein with an improved phase-reconfigurable input circuit to provide enhanced linearity. The phase-reconfigurable input circuit disclosed herein will be referred to simply as an “input circuit” in the following discussion for brevity. To provide improved linearity, the input circuit not only introduces an arbitrary static phase difference between the carrier and peak input signals but also dynamically modulates the phase difference responsive to a power of the input signal. The resulting dynamic modulation of the phase difference improves the linearity of the Doherty amplifier. Although the following discussion will be directed to a Doherty amplifier implementation, it will be appreciated that the input circuit disclosed herein is readily applicable to any suitable dual-input power amplifier such as a balanced amplifier or a load-modulated balanced amplifier.
An example input circuit 100 is shown in
To determine the input signal power for the dynamic phase modulation, an envelope detecting and processing circuit 120 detects the envelope of the input signal and processes the envelope into a differential envelope signal that is a function of the input signal envelope. For illustration clarity, the differential envelope signal is also illustrated as a single-ended signal in
Referring again to the input circuit 100, the differential peaking branch signal is transformed to single-ended form in a second differential-to-single-ended converter circuit such as a transformer and impedance matching circuit 155 to drive a second driver amplifier 161 in portion 105. In turn, the second driver amplifier 161 drives a peaking amplifier 165. The amplified output signals from the carrier amplifier 160 and the peaking amplifier 165 are combined in a combiner 170 to produce a combined output signal. A combined duplexer, filter, and antenna switch 175 processes the combined output signal to drive one or more antennas 180. A received signal from the antenna(s) 180 couples through the duplexer 175 before being amplified by a low-noise amplifier (LNA) (not illustrated).
To provide a better appreciation of the dynamic phase modulation provided by the input circuit 100, some basic concepts will now be discussed, followed by a more detailed discussion of the input circuit's various components. Recall that a traditional phase-reconfigurable circuit may introduce an arbitrary static phase difference between the carrier and peaking input signals. This phase difference may be expressed using a phasor representation of the carrier and peaking input signals produced. It may be shown that the carrier input signal (for example, the carrier input signal voltage) may be represented in phasor form by (1+j)exp(+j φ/2) whereas the peaking input signal may be represented by (1+j)exp(−j φ/2), where j is the imaginary number equaling the square root of −1. These phasors are illustrated using a unit circle as shown in
Regardless of the value of the static phase difference φ between the carrier and peaking input signals, the dynamic phase modulation disclosed herein may either increase the phase difference or decrease it depending upon the power of the input signal. In that regard, the dependency of the phase modulation on the input signal power may be characterized by a factor x, where x is a function of the input signal power. Depending upon how it is applied, the factor x may represent either a phase divergence (an increase over the static phase difference φ) or a phase convergence (a decrease from the static phase difference φ) between the carrier and peaking input signals. For example, suppose that x is applied so as to cause a phase divergence. In a phasor representation with phase divergence as a function x of the input signal power, it may be shown that the carrier input signal voltage may be represented in phasor form by (1+j)exp((+j φ/2+x). Assuming that x is small compared to φ/2, this phasor form may be expanded as shown in the following Equation (1):
where Vcarrier is the carrier input signal voltage waveform. Similarly, after expansion the peaking input signal voltage may be represented by the following Equation (2):
where Vpeaking is the peaking input signal voltage waveform.
With regard to these expanded expressions for the carrier and peaking input signals, it may be shown that the phase difference between the carrier and peaking input signals may be either increased (a diverging phase modulation) or decreased (a converging phase modulation) depending upon how the envelope modulation signal is derived from the envelope detection and processing circuit 120. Examples of the carrier and peak input signals with a diverging phase modulation and also with a converging phase modulation are also shown in
The pair of vector-sum phase shifters 140 and 145 are shown in conceptual form in
In the vector-sum phase shifter 140, a variable transconductance amplifier 305 transconducts the differential in-phase signals I+ and I− with a gain of cos(φ/2) to produce a differential output signal. A circuit 325 mixes the differential output signal from the variable transconductance amplifier 305 with the differential envelope signal so as to multiply the differential output signal with a factor of (1−x). Circuit 325 thus produces a differential version of cos(φ/2)(1−x) from Equation (1). This signal drives the transformer and impedance matching circuit 150, which will be discussed further below.
A variable transconductance amplifier 310 transconducts the differential in-phase signals I+ and I− with a gain of sin(φ/2) to produce a differential output signal. A circuit 340 mixes the differential output signal from the variable transconductance amplifier 310 with the differential envelope signal so as to multiply the pair of differential output signals with a factor of (1+x). Circuit 340 thus produces a differential version of sin(φ/2)(1+x). This differential version of sin(φ/2)(1+x) couples in a complementary fashion to the transformer and impedance matching circuit 150 to drive circuit 150 with a differential version of −sin(φ/2)(1+x) from Equation (1).
In the vector-sum phase shifter 145, a variable transconductance amplifier 315 transconducts the differential in-phase signals Q+ and Q− with a gain of sin(φ/2) to produce a differential output signal. A circuit 350 mixes the differential output signal from the variable transconductance amplifier 315 with the differential envelope signal so as to multiply the differential output signal with a factor of (1−x). Circuit 350 thus produces a differential version of j sin(φ/2)(1−x). This differential version of j sin(φ/2)(1−x) couples to the transformer and impedance matching circuit 150 to drive circuit 150 with a differential version of j sin(φ/2)(1−x) from Equation (1).
To complete Equation (1), a variable transconductance amplifier 320 in the vector-sum phase shifter 145 transconducts the differential in-phase signals Q+ and Q− with a gain of cos(φ/2) to produce a differential output signal. A circuit 355 mixes the differential output signal from the variable transconductance amplifier 320 with the differential envelope signal so as to multiply the differential output signal with a factor of (1+x). Circuit 350 thus produces a differential version of j cos(φ/2)(1+x). This differential version of j cos(φ/2)(1+x) couples to the transformer and impedance matching circuit 150 to drive circuit 150 with a differential version of j cos(φ/2)(1+x) from Equation (1). The vector-sum phase shifters 140 and 150 thus drive circuit 150 with a differential version of the carrier input signal as defined by Equation (1).
The vector-sum phase shifters 140 and 145 are constructed analogously so that the transformer and impedance matching circuit 155 is driven with a differential version (which may also be denoted herein as a second differential output signal) of the peaking input signal as defined by Equation (2). The vector-sum phase shifters 140 and 145 thus couple to a second pair of output terminals 148 to drive the transformer and impedance matching circuit 150 with the second differential output signal. In particular, a circuit 330 mixes the differential output signal from the variable transconductance amplifier 305 with the differential envelope signal so as to multiply the differential output signal with a factor of (1+x). Circuit 330 thus produces a differential version of cos(φ/2)(1+x). This differential version of cos(φ/2)(1+x) couples to the transformer and impedance matching circuit 155 to drive circuit 155 with a differential version of cos(φ/2)(1+x) from Equation (2).
A circuit 335 mixes the differential output signal from the variable transconductance amplifier 310 with the differential envelope signal so as to multiply the differential output signal with a factor of (1−x). Circuit 335 thus produces a differential version of sin(φ/2)(1−x). This differential version of sin(φ/2)(1−x) couples to the transformer and impedance matching circuit 155 to drive circuit 155 with a differential version of sin(φ/2)(1−x) from Equation (2).
In addition, a circuit 345 mixes the differential output signal from the variable transconductance amplifier 315 with the differential envelope signal so as to multiply the differential output signal with a factor of (1+x). Circuit 345 thus produces a differential version of j sin(φ/2)(1+x). This differential version of j sin(φ/2)(1+x) couples to the transformer and impedance matching circuit 155 in a complementary fashion to drive circuit 155 with a differential version of −j sin(φ/2)(1+x) from Equation (2).
Finally, a circuit 360 mixes the differential output signal from the variable transconductance amplifier 320 with the differential envelope signal so as to multiply the differential output signal with a factor of (1−x). Circuit 360 thus produces a differential version of j cos(φ/2)(1−x). This differential version of j cos(φ/2)(1−x) couples to the transformer and impedance matching circuit 155 to drive circuit 155 with a differential version of j cos(φ/2)(1−x) from Equation (2). The vector-sum phase shifters 140 and 150 thus drive circuit 155 with a differential version of the peaking input signal as defined by Equation (2).
In the following discussion it will be assumed that the antenna(s) such as antenna 180 of
The vector-sum phase shifters 140 and 145 may each be implemented using a suitable circuit having a mixer-like topology. The following discussion will thus be directed to mixer-like implementations of the vector-sum phase shifters 140 and 145 without loss of generality. As defined herein, a circuit is deemed to be a “mixer-like” circuit when the circuit has the topology of a mixer but does not frequency translate its output signal(s). Note that each of Equations (1) and (2) has four terms each, with two cosine terms and two sine terms. Each term may be formed by a corresponding plurality of mixer-like circuits. An example plurality of N mixer-like circuits 400 is shown in
With respect to activating individual circuits in the plurality of circuits 400, an N-bit wide digital control word cos_mag controls which ones of the circuits are active. The N circuits are arranged from a first circuit 405 to an Nth circuit 410. A first bit cos_mag(1) of the digital control word controls a switch 415 for the first circuit 405. Should switch 415 be closed, it gates the differential envelope signal Vg from being mixed in the circuit 405. But if the switch 415 is conducting, circuit 405 is active and mixes the envelope differential signal Vg with the in-phase differential signal. Similarly, a switch 420 controlled by an Nth bit cos_mag(N) of the digital control word controls whether the Nth circuit 410 is active or not. Each of the remaining circuits has its own corresponding switch analogous to switches 415 and 420. A combining network 425 combines the output signals from the active circuits to drive the peaking and carrier branches as will be explained further herein.
The mixer-like circuits disclosed herein may be constructed analogously to a Gilbert cell mixer. An example Gilbert-cell mixer-like circuit 500 is shown in more detail in
Circuit 500 also includes a differential pair of NMOS transistors M5 and M6 as well as another differential pair of NMOS transistors M7 and M8. The sources of transistors M5 and M6 couple to ground through an NMOS transistor M3. Similarly, the sources of transistors M7 and M8 couple to ground through an NMOS transistor M4. Depending upon the sinusoidal term being implemented, either the in-phase signal or the quadrature-phase signal from the I/Q signal generator 135 (
Assuming the circuit 500 is active, the positive component Vg+ of the envelope differential signal couples through transmission gate 510 to drive the gates of transistors M6 and M8. Similarly, the negative component Vg− of the envelope differential signal couples through the transmission gate 515 to drive the gates of transistors M5 and M8. The drains of transistors M5, M6, M7, and M8 couple to the combining network (not illustrated).
An example vector-sum phase shifter 600 is shown in
Referring again to the input circuit 100 of
The I/Q signal generator 135 functions to convert the differential signal from the transformer and impedance matching circuit 130 into the differential in-phase and quadrature-phase signals. In some implementations, the I/Q signal generator 135 may be formed by a two-stage polyphase filter. Each stage of the two-stage polyphase filter may be formed using either a transconductance-capacitance (gm-C) topology or a resistor-capacitor (RC) topology. An example RC two-stage polyphase filter 800 for implementing the I/Q signal generator 135 is shown in
An example two-stage gm-C polyphase filter 820 for implementing the I/Q signal generator 135 is shown in
A pre-amplifier may instead be inserted in between the vector-sum phase shifters 140 and 145 and the corresponding transformer and impedance matching circuits 150 and 155. In such an implementation, there may then be four single-ended pre-amplifiers such that the positive carrier branch input signal, the negative carrier branch input signal, the positive peaking branch input signal, and the negative peaking branch input signal are each pre-amplified by a corresponding pre-amplifier. Alternatively, such pre-amplifiers may be in addition to pre-amplifier 125. In other implementations, a pre-amplifier may instead be inserted between the transformer and the impedance matching portion in each of the transformer and impedance matching circuits 150 and 155. Note that these various pre-amplifier configurations may be in lieu of pre-amplifier 125 or may combined in part or in whole with pre-amplifier 125 in alternative implementations.
An example envelope detecting and processing circuit 120 is shown in more detail in
A dual-input amplifier method will now be discussed with regard to the flowchart of
The disclosure will now be summarized in the following example clauses:
Clause 1. A dual-input amplifier with dynamic phase modulation, comprising:
Clause 2. The dual-input amplifier of clause 1, wherein the I/Q generator circuit comprises a polyphase filter.
Clause 3. The dual-input amplifier of clause 2, wherein the polyphase filter comprises a transconductance-capacitor (gm-C) polyphase filter.
Clause 4. The dual-input amplifier of clause 2, wherein the polyphase filter comprises a resistor-capacitor (RC) polyphase filter.
Clause 5. The dual-input amplifier of clause 4, wherein the polyphase filter comprises a two-stage RC polyphase filter.
Clause 6. The dual-input amplifier of clause 3, wherein the gm-C polyphase filter comprises a two-stage gm-C polyphase filter.
Clause 7. The dual-input amplifier of any of clauses 1-6, wherein the envelope signal is a differential envelope signal, and wherein the dual-input amplifier further comprises:
Clause 8. The dual-input amplifier of clause 7, wherein the envelope signal is a differential envelope signal and the first vector-sum phase-shifter comprises:
Clause 9. The dual-input amplifier of clause 8, further comprising:
Clause 10. The dual-input amplifier of clause 8, wherein the second vector-sum phase-shifter also comprises four pluralities of mixer-like circuits.
Clause 11. The dual-input amplifier of any of clauses 1-10, wherein the phase-reconfigurable circuit is incorporated into a Doherty amplifier comprising:
Clause 12. The dual-input amplifier of clause 11, wherein the Doherty amplifier further comprises:
Clause 13. The dual-input amplifier of clause 12, further comprising:
Clause 14. The dual-input amplifier of any of clauses 1-13, further comprising:
Clause 15. The dual-input amplifier of any of clause 7, wherein the envelope detector further comprises a transconductance amplifier configured to form the differential envelope signal responsive to a difference between the envelope of the RF input signal and a reference voltage signal.
Clause 16. A dual-input amplifier method, comprising:
Clause 17. The dual-input amplifier method of clause 16, further comprising:
Clause 18. The dual-input amplifier method of claim 16, further comprising:
Clause 19. The dual-input amplifier method of clause 18, further comprising:
Clause 20. A dual-input amplifier, comprising:
Clause 21. The dual-input amplifier of clause 20, further comprising:
Clause 22. The dual-input amplifier of clause 21, further comprising:
Clause 23. The dual-input amplifier of clause 22, wherein the dual-input amplifier is integrated into a transmitter including at least one antenna configured to transmit the combined RF output signal.
Clause 24. The dual-input amplifier of clause 22, wherein the dual-input amplifier comprises a Doherty amplifier in which the first power amplifier is a carrier amplifier and in which the second power amplifier is a peaking amplifier.
Clause 25. A transmitter, comprising:
Clause 26. The transmitter of clause 25, wherein the one or more first amplifiers comprises a first series of a first driver amplifier and a first power amplifier, and wherein the one or more second amplifiers comprises a second series of a second driver amplifier and a second power amplifier.
Clause 27. The transmitter of clause 25, wherein the polyphase filter is a two-stage polyphase filter.
Clause 28. The transmitter of clause 27, wherein the two-stage polyphase filter is a two-stage transconductance-capacitor (gm-C) polyphase filter.
Clause 29. The transmitter of clause 27, wherein the two-stage polyphase filter is a two-stage resistor-capacitor (RC) polyphase filter.
Clause 30. The transmitter of any of clauses 25-30, wherein the one or more first amplifiers includes a carrier amplifier of a Doherty amplifier, and wherein the one or more second amplifiers includes a peaking amplifier of the Doherty amplifier.
The description herein is provided to enable a person skilled in the art to make or use the disclosure. Various modifications to the disclosure will be readily apparent to those skilled in the art, and the generic principles defined herein may be applied to other variations without departing from the scope of the disclosure. Thus, the disclosure is not limited to the examples and designs described herein but is to be accorded the broadest scope consistent with the principles and novel features disclosed herein.