This application is a continuation of pending Ser. No. 12/893,908 filed Sep. 29, 2010 now U.S. Pat. No. 8,253,473 issued Aug. 28, 2012, the entire disclosure of which is hereby incorporated herein by reference.
Numerous analog mixed-signal integrated circuits contain continuous-time filters based on elementary integrator cells that generally include a tunable transconductance amplifier (Gi) and a capacitor (Ci). Elementary integrator cells (Gi, Ci) are often building blocks of more complex circuits.
An exemplary integrator is shown in
The resistance Ri may be the finite output impedance of the transconductance amplifier Gi (due to the finite output impedance of the electronic components constituting the transconductance amplifier) or a resistive element (a resistor or an active device adapted to behave as a resistor) connected at the output of the transconductance amplifier, or a combination of the two.
The transfer function of the integrator of
The depicted circuit (Gi-Ci) nominally behaves like an integrator having its 0 dB crossing frequency at fi=Gi/2πCi, wherein the transconductance gain Gi may be fixed in a very large range of values.
The error amplifier Aio adjusts the gain of the transconductance amplifier Gi and of the matched transconductance amplifier Gmi in order to nullify the difference between the reference current output by the DAC and the current Gmi*Vr of the transconductance amplifier Gmi:
wherein GDAC is the programmable current gain of the digital-to-analog converter. Using the reference resistor Rr that may be an external resistor, or a resistor with a minimal dependence from process spread and/or supply voltage and temperature fluctuations, the transconductance gain Gmi is adjusted by the control loop for compensating such possible fluctuations, and is tunable by adjusting the gain of the DAC.
When the amplifiers Gi and Gmi are matched, their transconductance may substantially vary according to the same law. However, the transconductance gain Gi and the resistance Ri, and thus also the voltage gain (Gi Ri) of the integrator cell are influenced by process spread, supply voltage, and temperature fluctuations (PVT). This makes the phase of the transfer function of the integrator cell at the crossing frequency fi different from 90°, as it would be in an ideal integrator, and causes a PVT-dependent phase shift. This phase shift may affect the frequency response of filters based on integrator cells, especially if they function at high frequencies and are tunable over a wide frequency range.
An integrated architecture of an integrator that overcomes the above criticalnesses and inconveniences has been found. According to this disclosure, the output resistance of the input transconductance amplifier Gi of the integrator is made independently adjustable from the transconductance gain Gi through a dedicated control signal, and also includes a matched transconductance amplifier Gi2 having an adjustable gain and an output resistance matched with that of the first transconductance amplifier Gi, and adjusted by the same dedicated control signal. A reference current is forced through the matched output resistance, and the dedicated control signal is generated such to keep the output voltage of the matched transconductance amplifier relatively constant.
A method of stabilization against PVT variations of the integrated circuit of an integrator is also disclosed herein.
A single-end integrator according to a first embodiment is depicted in
This second control loop generates a voltage that varies with fluctuations of the matched resistance Rmi, subtracts it from a constant voltage kVr, and generates the control signal Vc as an amplified replica of the difference with the error voltage amplifier Avo. The output resistance Ri is adjusted by the same dedicated control signal.
The second error amplifier Avo has a gain designed to help ensure an adequate response of the second control loop, and adjusts the resistance Rmi to make
Gi2 Rmi=k Vr=constant (3)
even in case of PVT induced fluctuations. The matching between Gi2 and Gi and between Rmi and Ri fixes the phase of the integrator cell at the 0 dB crossing, independently from PVT induced fluctuations for a large range of frequencies, tunable through the DAC value.
The output resistance Rmi of the matched transconductance amplifier Gi may be the finite output impedance of the transconductor cell (due to the finite output impedance of the electronic devices making the transconductor cell), a resistive element placed at the output of the transconductor (a resistor or an active device behaving like a resistor), or a combination of the two.
The particular implementation of the two control loops in
In the example shown in
According to an alternative embodiment illustrated in
Rmi=k*Vr/Ir=constant (4)
An exemplary embodiment of the adjustable transconductance amplifier Gi and of the matched adjustable resistive element Rmi will now be described. In addition, an embodiment of the second control loop of the integrator cell realized in differential circuit form is depicted in
The transconductance amplifier Gi2 includes the devices M1-M8. The matched resistive element Rmi includes the devices M9-M11. The NMOS devices M1, M2 may be a differential pair, fed by the input signal Vin+/Vin− and by the tail current sources M7, M8.
The skilled person will immediately understand that it is not indispensable to realize tail current sources using the depicted MOSFETs M7, M8 and will be immediately capable of identifying in the relevant literature other usable architectures of tail current sources.
The transistors M5, M6 act as variable degenerating resistors to increase the linearity of the input differential pair. They may be replaced with a short circuit if no linearity improvement is desired, or substituted by other linearization circuitry.
The PMOS M3, M4 work as an active load. The current supplied by M3, M4 is set by a common-mode feedback amplifier CMFB that forces the common mode (Out++Out−)/2 to match a reference common mode Vcm. The active load M3-M4 and its relative common mode control may be substituted by any other kind of controlled active loads.
The finite output resistance of the transconductance amplifier Gmi of
The adjustable resistance Rmi is realized with the devices M9, M10, M11, that behave as a negative resistance. The value of this negative resistance is controlled by the proposed control loop by setting the voltage Vc, that fixes the current flowing through the devices M9, M10 and, as a result, their transconductance.
Alternative embodiments of variable resistances (either positive or negative) are possible. As an example, in
An exemplary embodiment of the circuit that adjusts the resistance is shown in
Exemplary application of the integrator cell to a 1st order LPF will now be discussed. In the following, the above circuit is applied, as an example, to a 1st order low pass filter.
and its group delay Tg(ω) is:
The LPF characteristics are similar or identical to those obtainable with an ideal integrator, provided that the capacitance Ci of the non ideal integrator may be multiplied by a factor (1+1/k), being k=GiRi.
If, by the two control loops and by layout matching, Gi=Gmi=Gi2=DAC/Rr and GiRi=k=constant, equations (5) and (6) are independent from any PVT variations, and the filter is tunable through the current converter DAC.
The 3 dB-frequency of the transfer function of equation (5) is:
that is clearly independent from PVT fluctuations and is tunable by setting the gain GDAC.
Number | Date | Country | Kind |
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VA2009A0061 | Oct 2009 | IT | national |
Number | Name | Date | Kind |
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20100141340 | Huang et al. | Jun 2010 | A1 |
Number | Date | Country |
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0365091 | Apr 1990 | EP |
1578013 | Sep 2005 | EP |
Number | Date | Country | |
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20120286870 A1 | Nov 2012 | US |
Number | Date | Country | |
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Parent | 12893908 | Sep 2010 | US |
Child | 13561355 | US |