The present invention relates generally to phase-locked loop systems, and more particularly, to phase-locked loop systems that utilize charge pump circuits.
Phase-locked loops (PLL) find widespread use in frequency synthesizers, clock recovery circuits, phase modulators, and frequency demodulators. Generally, a PLL consists of a voltage-controlled oscillator (VCO), counter, phase/frequency detector (P/FD), charge pump (CP), and RC integration filter.
The phase-locked loop relies on feedback to drive the frequency difference and phase offset between a reference signal and the output of the counter towards zero. Its operation depends on the circuits that comprise the system; and as such, variations in circuit parameters alter the response of the system, lower the stability of the feedback loop, and introduce distortion. The charge pump and integration filter are circuits that are especially sensitive.
It is therefore desirable to improve the performance of the charge pump so that the PLL can better adapt to parameter changes.
In one or more embodiments, a PLL system is provided that includes an improved charge pump (CP) circuit that operates linearly and compensates for parameter variations. The improved CP circuit produces fast and symmetric current pulses with reduced ringing and overshoot.
In one embodiment, a charge pump circuit is provided that comprises a replica circuit that provides a current difference between charge (UP) and discharge (DN) currents, and a buffer coupled to the replica circuit to buffer a received control voltage.
In one embodiment, a charge pump circuit is provided for use in a phase-lock loop circuit. The charge pump circuit comprises a charge pump core circuit that outputs a control voltage. The charge pump circuit also comprises a replica circuit that is coupled to the charge pump core circuit, wherein the replica circuit receives the control voltage and produces one or more bias signals that are coupled to the charge pump core circuit to minimize the difference between charge up and charge down currents generated by the charge pump core circuit.
In one embodiment, a method is provided for operating a charge pump circuit in a phase-lock loop circuit. The method comprises generating an output control voltage at a charge pump core circuit, generating one or more bias signals based on the control voltage, and adjusting the operation of the core circuit based on the one or more bias signals so as to minimize a difference between charge up and charge down currents.
In one embodiment, a charge pump circuit is provided for use in a phase-lock loop circuit. The charge pump circuit comprises a charge pump core circuit means for outputting a control voltage. The charge pump circuit also comprises a replica circuit means for receiving the control voltage and producing one or more bias signals that are coupled to the charge pump core circuit means to minimize the difference between charge up and charge down currents generated by the charge pump core circuit means.
The foregoing aspects and the attendant advantages of the embodiments described herein will become more readily apparent by reference to the following detailed description when taken in conjunction with the accompanying drawings wherein:
In one or more embodiments, a PLL system is provided that includes an improved charge pump (CP) circuit that operates linearly and compensates for parameter variations.
Vout(t)=Ac cos (ωfreet+KVCO∫vctrl(t)dt)
where ωfree is the free-running frequency of the oscillator and Kvco is its gain function. The gain function Kvco describes the relationship between the excess phase of the carrier Φout(s) and the control voltage vctrl, i.e.
The Div-by-N counter simply divides the output phase Φout(s) by N. When the PLL is locked, the phase/frequency detector and CP combination generate an output signal (iCP(t)) that is proportional to the phase difference (error Δθ) between the two periodic signals input to the phase detector. The CP output signal can be expressed as;
A simple RC integration filter, consisting of resistor R and capacitor C, transforms the CP output signal to the control voltage Vctrl, which can be expressed as;
Combining the above transfer functions yields the composite transfer function;
where a zero (at 1/RC) has been added to the second order system to stabilize it.
The phase/frequency detector and CP define the parameter KPD. These circuits compare the output of the feedback N-counter to the reference signal Φin and generate the output signal Icp(t) representing their phase difference.
Referring again to
The P/FD drives the CP, which comprises a pair of switches S1 and S2 that connect current sources IUP and IDN to the integration filter (R1, C1). An UP pulse closes switch S1 and directs charge to the integration filter, raising the control voltage vctrl. Similarly, a DN pulse closes switch S2 and removes charge from the integration filter, lowering the control voltage vctrl. The control voltage vctrl, in turn, sets the frequency of the voltage-controlled oscillator (VCO in
Ideally, the CP circuit is both symmetrical and insensitive to the level of the control voltage vctrl. The net charge (ΔQ) transferred or removed from the integration filter is proportional to the time difference (Δt) between the active edges of the N-counter's output signal (DIV) and the reference signal (REF), and can be expressed as;
ΔQ=KPDIΔt
where KPD is the associated scaling factor and I is the current level—either IUP or IDN. It may also be important that these currents be equal and therefore cancel during the overlap of the UP and DN pulses, otherwise, an error occurs.
In one embodiment, the current sources IUP and IDN and the switches S1 and S2 are implemented using CMOS transistors. In one embodiment, the current source transistors operate in the saturation region with VDS≧VGS−VT. In this region, the applied gate-source voltage VGS sets the drain current ID as expressed by;
where the μ is the carrier mobility, COX is the oxide capacitance, W and L are the device dimensions, VT is the threshold voltage, and λ is the channel-length modulation coefficient. The voltage difference VGS-VT is oftentimes noted as the overdrive or effective voltage Veff. In other applications, VDS<VGS−VT and the transistor operates in the linear region with ID given by;
Therefore, to operate the transistor in saturation mode, the minimum drain-source VDS(sat) is approximated by;
where κ is the intrinsic gain of the device
and λ is assumed to be small.
Phase-locked loops may target a specific frequency or range of frequencies. The feedback system adapts to different device parameters and circuit responses through changes in the control voltage vctrl. Supporting a wide control voltage range provides for lower VCO sensitivity (KVCO) and improved noise immunity. Unfortunately, this may also mean dramatic changes in the operating bias for the transistors in the CP circuit. As a result, the symmetry, matching, and overall performance of the CP circuit may suffer.
VUP+<V+−+VDS(sat)
Increasing voltage VUP+, collapses the drain-source voltage available to the current-source transistor P1 and thereby prevents any charge transfer.
Similarly, to remove an accurate charge from the integration filter and to operate devices N1, N3 in the saturation mode, the following two conditions should be met;
VDN+>VGS
Lowering voltage VDN+ prevents any charge transfer. This means that the drain-source voltage applied to current-source transistors P1 and N1 actually switches, charging and discharging any associated device capacitances.
Ideally, the differential pair switch maintains a fixed voltage at the drain of transistor P1. In practice, this voltage may change due to voltage and impedance differences seen at the drain of transistors P2 and P3.
The current source transistors P1, N1 generally have long-channel geometries and high effective gate-source bias voltages (Veff) to reduce channel-length modulation effects, minimize parasitic capacitance, and improve matching. The effective voltage also corresponds to the minimum drain-source voltage for operation in saturation mode VDS(sat) since;
and as a result;
VDS(Sat)
The effective voltage is typically several hundred millivolts.
An ideal charge pump circuit generates matching charge (IUP) and discharge (IDN) currents so that these currents cancel each other when the UP and DN pulses overlap. In practice, this is challenging because the current sources are implemented using complimentary devices—PMOS and NMOS transistors—and therefore may be dependent upon different parameters.
Any output current Δi is sensed by resistor R2 and amplified by error amplifiers GM1 and GM2. In one embodiment, the amplifiers GM1 and GM2 are transconductance amplifiers that convert an input differential voltage to an output current. The output currents from error amplifiers GM1 and GM2 adjust bias currents IB2 and IB4, which are mirrored to the replica circuit and the CP core current sources (transistors P1 and N1). The two error amplifiers (GM1 and GM2) are part of feedback loops that reduce the current Δi, and thus the difference in the replica circuit's as well as the charge pump's currents (IUP and IDN).
Δi=IN6−IP6≈IDN−IUP
and develops a proportional voltage across resistor R2 equal to ΔiR2.
IP7=IB2+ΔIUP≈IUP
where current source IB1 (and thus ΔIUP) depends on the output of the operational amplifier 1102. That is to say that the current IB1 exists only when the voltage vctrl rises significantly above its lower limit, VDS(sat)N1. As a result, the difference current ΔIUP is generally positive.
With regards to GM2, transistors P10, P11, N7, and N10, N11, along with current sources IB3 and IB4 form a network similar to the one described above that adjusts current-source transistors N1 and N6. When the operational amplifier 1102 sinks current from the replica circuit, it indicates that IUP is larger than IDN. This creates a voltage across resistor R2 that steers more current through transistor P11 than transistor P10. As a result, a difference current ΔIDN is directed towards transistor N7, making;
IN7=IB4+ΔIDN≈IDN
where the bias current IB3 (and thus ΔIDN) depends on the output of the operational amplifier 1102. Although it operates similarly to bias current IB1, in this case, current IB3 exists only when the voltage vctrl falls significantly below its upper limit, V+−VDS(sat)P1. This generally makes ΔIDN positive.
VB1=V+−VDS(sat)
where mirror circuitry N7 and N12 establishes the proper current in transistors P12 and P13. Similarly, transistor P14 establishes the proper current density needed to set the gate-source voltage of transistor N13 and the drain-source voltage of transistor N14 with;
VB2=VGS
where the voltage VB2 serves as a reference to a feedback network shown in
VDN+=V+−(IN16+IN18)R5 and VDN−=V+−(IN16+IN18)R5+IN18R5
where R3=R4 and
which assures full switching of the differential pair N2, N3. In addition, the voltage VDN+ actually sets the drain voltage of the current source transistor N1 with
VDS(sat)
Note that VDS(sat) changes with both the drain current and the effective voltage Veff of the device. A similar switch driver can be used to control transistors P2 and P3.
VB2=VGS
which corresponds to the voltage needed for VDN+ to properly bias transistor N1. This assumes matching between transistors N2, N3 and N13 (to duplicate VGS(on)) and transistors N3 and N14 (to duplicate VDS(sat)). In turn, the servo loop circuit forces the maximum output level from the switch driver (equivalent to VDN+) to be equal to VB2, assuming transistors N15 and N16, N17 and N18, resistors R3 and R7, plus resistors R5 and R6 are matched. As a result,
(IN15+IN17)R6+IN17R7=(IN16+IN18)R5+IN18R4
which establishes the proper output levels from the driver switch.
The above circuit descriptions remain valid even when the currents in the replica and mirror structures are lowered as long as the current density in these structures is uniform. This minimizes the overall current consumption of the CP.
These innovative circuits generate the proper switch levels, minimize the difference between the charge and discharge currents of the CP circuit, and remove many of the design restrictions associated with current source transistors. The result is a circuit with improved performance, stable KPD, and extended control voltage range. The described circuits also allow the CP circuit to operate at lower supply voltages.
In one or more embodiments, an improved charge pump circuit is provided. Accordingly, while one or more embodiments of the charge pump circuit have been illustrated and described herein, it will be appreciated that various changes can be made to the embodiments without departing from their spirit or essential characteristics. Therefore, the disclosures and descriptions herein are intended to be illustrative, but not limiting, of the scope of the invention, which is set forth in the following claims.
This application claims the benefit of priority from a pending U.S. Provisional Patent Application entitled “IMPROVED CHARGE PUMP CIRCUIT” Ser. No. 60/405,669 filed on Aug. 24, 2002, the disclosure of which is incorporated by reference herein in its entirety for all purposes.
Number | Name | Date | Kind |
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5508660 | Gersbach et al. | Apr 1996 | A |
5945855 | Momtaz | Aug 1999 | A |
6781425 | Si | Aug 2004 | B2 |
Number | Date | Country | |
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60405669 | Aug 2002 | US |