This application claims the benefit of Italian Patent Application No. 102019000016871, filed on Sep. 20, 2019, which application is hereby incorporated herein by reference.
The present invention relates to an electronic circuit, and in particular embodiment, to an electronic circuit for tripling frequency.
As is known, communications at millimeter-wave (mm-wave) range have drawn a lot of attention in recent years due to the wide available bandwidth yielding higher data transmission capacity. Thus, current systems use transceivers that convert the exchanged signals from the base frequency to the selected communication frequency and vice versa. To this end, the transceivers use circuitry to generate a local oscillation (LO). Design of the local oscillation transceivers is critical because many conflicting parameters, i.e., tuning range, phase noise, output power and level of spurious tones, affect the performances. Differently from what is commonly pursued at other radio frequencies, local oscillation generation with a PLL (Phase Locked Loop) circuit comprising a VCO (Voltage Controlled Oscillator) at the desired output frequency is not viable at mm-wave range. In fact, the severe impact of parasitic structures and effects in silicon technology and the low quality factor of passive components (mostly, variable capacitors) impair the achievable tuning range and phase noise. Moreover, traditional frequency dividers in the PLL cause excessive power consumption.
A more promising approach consists in providing a PLL in a lower range (e.g., in the 10-20 GHz range), where the silicon VCO features the best figure of merit, followed by a frequency multiplier chain.
For example,
The frequency multiplier system 1 has to provide a good suppression of the driving signal and of undesired harmonics in order not to impair the transceiver performance. In particular, in the frequency multiplier system 1, it is desired that the first stage (frequency tripler 3) features the highest suppression, because its spurious tones are shifted close to the final LO frequencies by the intermodulation of the cascaded stages. Moreover, this issue is more critical for odd-order multipliers, because even-order multipliers (here, the frequency doubler 5) may exploit push-push transistors for suppression of signal components at undesired frequencies.
Odd-order multipliers, such as the frequency tripler 3 of the frequency multiplier system 1, typically comprise a transistor with low conduction angle (e.g., class-C biased transistor) that generates a harmonic-rich current and the desired component is selected with a band-pass filter or an injection-locked oscillator.
For example,
Vin=A sin(2πfot)
through an input capacitor 12 and coupled to a bias voltage Vb through a resistor 13. The transistor 11 has an emitter terminal E grounded, and a collector terminal C coupled to an output terminal 14 and to a supply voltage VCC through an LC resonant circuit 15 tuned at 3fo.
In a per se known manner, the class-C tripler circuit 10 conducts a current Io whose harmonic content is set by the conduction angle θ determined by the bias voltage Vb and shown in the simulations of
In detail,
As may be seen in
Class-C tripler circuits may be improved, in principle, by using a more complex filter topology or by cascading multiple filtering stages, but at the cost of a high design complexity, big area, bandwidth limitation and higher consumption.
Also the injection-locked oscillator solution (see, e.g., N. Mazor et al., “A high suppression frequency tripler for 60-GHz transceivers,” in 2015 IEEE MTT-S International Microwave Symposium, 2015, pp. 1-4), although providing a better suppression (up to about 30 dB), does not satisfactorily solve the problem.
Some embodiments provide a frequency tripler that improves the suppression of the driving signal frequency at the output.
Some embodiments relate to tripling frequency, in particular for radiofrequency applications in the millimeter-wave range.
Some embodiments relate to an electronic circuit for tripling frequency. Some embodiments related to a corresponding method.
For the understanding of the present invention, embodiments thereof are now described, purely as a non-limitative example, with reference to the drawings, wherein:
The tripler circuit 20 represents an implementation of an ideal transistor-based tripler circuit having a polynomial trans-characteristic f(Vin) (later on also called ideal polynomial trans-characteristic) according to the following equation (1):
where gm is the transconductance of the transistor in the tripler circuit (at a specific DC biasing condition).
In particular, as may be demonstrated with some calculation, the above ideal trans-characteristics allows a tripler circuit, receiving at its input a sinusoidal driving voltage:
Vin=A sin(2πf0t)=A sin(ω0t)
having amplitude A and base frequency fo is able to generate an output current Io:
Io=f(Vin)=gm sin(32πf0t)=gm sin(3ω0t)
having only the third harmonic (3fo).
In detail, with reference to
In detail, the first and second transistors Q1, Q2 have emitter terminals coupled to each other and to a common node 21, base terminals coupled to a first and, respectively, a second input node 22, 23 and collector terminals coupled to a first and, respectively, a second output node 24, 25 supplying a first and, respectively, a second single-ended current Io− and Io+.
The third and fourth transistor Q3, Q4 have emitter terminals coupled to each other and to the common node 21, base terminals coupled to a third and, respectively, a fourth input node 27, 28, and collector terminals coupled to the second and, respectively, the first output node 25, 24.
A biasing current source 26, configured to generate bias current Ib, is coupled between the common node 21 and ground.
The first and the second input nodes 22, 23 receive each a fraction equal to ½ of the input voltage Vin, in counter-phase, both reduced by a DC voltage (offset voltage Vos). The third and the fourth input nodes 27, 28 receive each an attenuation α/2 of the input voltage, in counter-phase, the attenuation α being selected so that, during operation, at low values of the input voltage Vin and considering also the offset voltage Vos, the first pair of transistors Q1, Q2 is still off, while the second pair of transistors Q3, Q4 are on, as discussed in detail below.
Specifically, the first input node 22 receives first voltage V1:
V1=Vin/2−Vos;
the second input node 23 receives voltage V2:
V2=−Vin/2−Vos;
the third input node 27 receives voltage V3:
V3=αVin/2; and
the fourth input node 28 receives voltage V4:
V4=−αVin/2
where Vos is the DC offset voltage and α is the attenuation, as indicated above.
The tripler circuit 20 of
The trans-characteristic of the tripler circuit 20 of
In particular, the normalized output current Ion is the differential current Io+−Io+, normalized with respect to its maximum amplitude (equal to Ib).
The values of attenuation α and offset voltage Vos are selected so that the trans-characteristic of the tripler circuit 20 tracks the ideal polynomial trans-characteristic of equation (1), that is so that the trans-characteristic of the tripler circuit 20 is null at Vin=0, then increases with a similar slope as the ideal polynomial trans-characteristic, then decreases again to zero and to negative values, following the ideal trans-characteristic. The opposite happens for negative values of Vin.
In particular, the zero-crossings (besides of that at Vin=0) of the trans-characteristic of the tripler circuit 20 occur when the voltage at the base terminal of the third transistor Q3 (at the third input node 27) equals the voltage at the base terminal of the first transistor Q1 (at the first input node 22) as well as when the voltage at the base terminal of the fourth transistor Q4 (at the fourth input node 28) equals the voltage at the base terminal of the second transistor Q2 (at the second input node 23), that is when condition (2) is satisfied:
The zero-crossings occur thus at the following values of the input voltage Vin:
On the other hand, the zero-crossings of the trans-characteristics (1) (besides of that at Vin=0) occur at the following values of the input voltage Vin:
It follows that the trans-characteristic of the tripler circuit 20 and the ideal trans-characteristic have same zero-crossings when attenuation α and offset voltage Vos satisfy the following condition:
Analysis of the derivatives of the ideal polynomial trans-characteristic (i) shows that its slope at the zero crossings at Vin=±√{square root over (3)} A/2 is ±2 times that of the origin. Further circuit analysis proves that it is enough to design attenuation α=0.2 to have the slopes of the two trans-characteristics identical at zero crossings, such that the shape of the actual trans-characteristic of the tripler circuit 20 keeps as close as possible to the ideal one (see
By fixing the value of attenuation α, the value of the offset voltage Vos is obtained as a linear function of the amplitude A of the input voltage Vin, based on condition (5).
In this case, also a non-optimal value of the attenuation α may be set, and the envelope detector operates as an open loop able to compensate and maintain the linear desired relationship of condition (5).
For example,
In
A voltage divider 40, of capacitive type, is coupled between the input nodes 22, 23 of the tripler circuit 20 and comprises a first branch 41 and a second branch 42.
The first branch 41 of the voltage divider 40 comprises a first capacitor 45, a first resistor 46, a second resistor 47 and a second capacitor 48 connected in series. The first and second capacitors 45, 48 have same capacitance C1; the first and second resistors 46, 47 have same resistance R.
The first branch 41 has a central tap between the first and second resistors 46, 47 coupled to a second output 50 of the envelope detector 38, which generates a second biasing voltage Vb2. The first branch 41 also has a first intermediate node 51 between the first capacitor 45 and the first resistor 46 and a second intermediate node 52 between the second resistor 47 and the second capacitor 48. The voltage difference Vb2-Vb1 forms the offset voltage Vos of the tripler 20 of
The second branch 42 of the voltage divider 40 comprises a third capacitor 54 coupled between the first and second intermediate nodes 51, 52. The third capacitor 54 has a capacitance C2. First and second intermediate nodes 51, 52 are also coupled to the third and, respectively, the fourth input node 27, 28 of the tripler circuit 20.
The first and second input nodes 22, 23 of the tripler circuit 20 are also coupled to a first, respectively a second input 55, 56 of the envelope detector 38 through respective capacitors 57, 58.
The tripler circuit 30 also comprises an output transformer T2 having a primary winding 61 coupled between the first and second output nods 24, 25 of the tripler 20 and a second winding 62 coupled between a first and second circuit outputs 64, 65; and an LC network 66 formed by a shunt capacitor 67 and a tail inductor 68 is coupled between the common node 21 of the tripler 20 and ground.
The first and second circuit outputs 64, 65 may be connected to an output buffer similar to the first buffer 4 of frequency multiplier system 1 of
In the tripler circuit 30 of
The tail inductor 68 resonates with shunt equivalent capacitance existing at the common node 21 and the shunt capacitance 67 is sized sufficiently large to act as an AC-short at the operating frequency of common node 21, which is 2fo. In fact, LC network 66 allows the shunt parasitic capacitances at common node 21 to charge-discharge at high frequency using the current being exchanged with the tail inductor 68, hence not to lag behind the base voltages of the input transistors Q1-Q4 when operating at high input frequency.
In the specific implementation shown in
A supply voltage VCC is applied to the collector terminals of the fifth and sixth transistors Q5 and Q6 and to supply nodes of the first and second voltage generating networks 75, 81. Supply voltage VCC is also applied to a central tap of the second transformer T2.
All transistors Q5-Q10 in the envelope detector 38 share a same bias voltage VCM. In this way, transistors Q5-Q6 (driven by |Vin(t)|) and Q7, cause the voltage VRE on averaging resistor 73 to be equal to the average value of |Vin(t)|. Since Vin(t)=A sin(2πfot), voltage on the averaging resistor 73 is VRE=(4/π)A and the current through it is IRE=(4/π)A/RE. MOSFET transistors M1, M2 in the first voltage generating network 75 mirror current IREF+IRE into a first output resistor 85 (coupled to the first output 37 of the envelope detector 38) with resistance while MOSFET transistors M3, M4 in the second voltage generating network 81 mirror current IREF into a second output resistor 86 with resistance R2 (coupled to the second output 50 of the envelope detector 38). Thus:
Vb1=VCC−(IREF+IRE)·R1,
Vb2=VCC−IREF·R2.
Assuming R1=R2,
Vos=Vb2−Vb1=R1·IRE=(4/π)(R1/RE)A.
The ratio R1/RE is designed such that Vos satisfies condition (5), thus allowing to maintain good suppression of the fundamental frequency component independently from the amplitude of the input signal.
Measurements made by the Applicant confirm that the tripler circuit 20 suppresses almost completely the component at fundamental frequency fo in the output current Io. For example,
The improvement of the tripler circuit 20 with respect to a conventional tripler using class-C operating transistors is also visible from
Advantages of embodiments of the present invention are clear from the above. For example, it is underlined that, in some embodiments, the tripler circuit is advantageously able to suppress undesired fundamental and harmonics in a much better way than with conventional circuits.
In some embodiments, the tripler circuit advantageously operates at low power compared with conventional designs exploiting class-C transistors and filters.
Finally, it is clear that numerous variations and modifications may be made to the frequency tripling electronic circuit described and illustrated herein, all falling within the scope of the invention as defined in the attached claims.
For example, the bipolar transistors Q1-Q10 could be replaced by MOSFET transistors; the transistors may be made in any technology, such as silicon, gallium arsenide (GaAs), indium phosphide (InP), etc.; the structure of the envelope detector may be any other, provided it performs the functionalities depicted above, specifically it gets Vb2−Vb1=Vos satisfying relation (5).
Number | Date | Country | Kind |
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102019000016871 | Sep 2019 | IT | national |
Number | Name | Date | Kind |
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5552734 | Kimura | Sep 1996 | A |
5576653 | Kimura | Nov 1996 | A |
5581210 | Kimura | Dec 1996 | A |
20090160502 | Lu | Jun 2009 | A1 |
Number | Date | Country |
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2283347 | May 1995 | GB |
H1093399 | Apr 1998 | JP |
2015042814 | Apr 2015 | WO |
Number | Date | Country | |
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20210091757 A1 | Mar 2021 | US |