This disclosure relates to phase locked loops (PLLs).
Rapid advances in electronics and communication technologies, driven by immense customer demand, have resulted in the widespread adoption of an extensive variety of electronic devices. These devices often rely for proper operation on sophisticated frequency synthesizers, clock recovery circuits, jitter and noise reduction circuits and other types of circuits that are sometimes implemented with phase locked loops (PLLs). Improvements in PLLs will further enhance the performance of electronic devices.
The PLL 100 and its component parts may be implemented in other ways and may vary in performance characteristics from implementation to implementation. For example,
The PLL 100 includes a fine resolution (FineRes) encoder 106 for encoding the ΔΣ ADC output. The fine resolution encoding facilitates true multi-bit phase/frequency error digitization with drastically reduced ΔΣ quantization noise. A phase/frequency detector charge pump (CP) 108 front-end drives the ADC 104, and a multi-modulus divider (MMD) 110 is present in the feedback path from the digital loop filter.
The PLL 100 also includes coarse and fine resolution detection modes that facilitate fast acquisition and spur-free tracking operation. A fully digital loop filter 112 may be implemented in the PLL 100 and may control the digitally controlled oscillator (DCO) 114. Note that the PLL 100 has a bandwidth determined by the loop filter coefficients independent of the ΔΣ phase/frequency detector parameters (e.g., CP current Icp and the 1st-order ΔΣ ADC integrating capacitor Cint).
The PLL 100 operates on the differential phase/frequency error of its output clock signal Fout with respect to the input reference clock signal 122, Fref. The output frequency of the PLL output clock 124, Fout, reflects the targeted channel frequency upon phase/frequency lock. The detector 102 provides a digital estimate of the PLL output frequency the PLL 100 may compare to a digital word (e.g., a channel indicator 116) that specifies the targeted channel frequency for the PLL 100 to produce. The digital frequency error information (Δfe) 118 is accumulated (e.g., integrated) to provide the digital phase error information (Δphie) 120. The PLL 100 controls the phase/frequency of the DCO 114 responsive to the digital frequency error information, e.g., to try to eliminate the error. A phase lock enable signal 126 may be provided to selectively enable or disable the operation of the accumulation and filter operations of the PLL 100.
Note that the loop filter configuration is independent of the fine resolution encoder 106. Without the fine resolution encoder 106, loop filter may instead be characterized by a low bandwidth and high rejection (that may result in less stable output) so that distortion due to the coarse resolution quantization is adequately filtered. The fine resolution encoder 106 thus allows for more flexible PLL dynamic control.
An accumulator 164 accumulates the digital frequency error information (Δfe) 162 (e.g., by integration) to provide the digital phase error information (Δphie) 166. The loop filter 168 filters the digital phase error information. The second example architecture 152 controls the phase/frequency of the DCO 170 responsive to the digital frequency error information, e.g., to try to eliminate the error. A phase lock enable signal 172 may be provided to selectively enable or disable the operation of the accumulation and filter operations of the PLL. The DCO 170 generates a frequency output 174.
The flash ADC 204 and current-mode DAC 206 of the ADC 104 is digitally reconfigurable to support single-bit or multi-bit resolution via dynamic control of the number of active quantization levels, allowing for fast frequency acquisition and spur-free tracking operation. In that regard, the PLL 100 may include a resolution control input 208 that specifies, e.g., the number of quantization levels that the ADC 104 will generate. As a specific example, the resolution control input 208 may be provided to both the flash ADC 204 and the current-mode DAC 206 to configure them for the number of quantization levels desired. A controller may use the resolution control input 208 to place the PLL 100 into single-bit or three level quantization mode for coarse resolution operation of the PLL 100, while the controller may cause multi-bit quantization for fine resolution operation of the PLL 100. The controller may switch to fine resolution operation on an application specific basis, and as one example the switch to fine resolution may depend upon the time for the frequency error to settle to within a predefined margin. To the extent that there are mismatches in the flash ADC 204 and current-mode DAC 206 characteristics, those mismatches may be randomized via the closed-loop noise shaping functionality of the detector 200, thereby alleviating any need for dynamic element matching (DEM). However, as noted below with respect to
Nint+{ . . . , −1, 0, 1, . . . }
and thereby achieves a long-term average fractional N value, where:
N=N
int
+N
frac
=F
LO
/F
ref and Nfrac∈[0,1) or [−½, ½).
The mean value of the detector output Bout 302 is preferably Nfrac in order to minimize the frequency error between Fref and Fmmd=FLO/(Nint+Nfrac). The fractional division control results in Nfrac cycle-to-cycle period variations of Fmmd, which entail a Nfrac LO cycles normalized differential frequency Delta fin input 304 to the ΔΣ detector.
Delta fin (Nfrac) 304 and the induced 1st-order ΔΣ ADC quantization noise Qn 306 are transferred to the detector output 302 as:
B
out
=Δf
in+(1−z−1)2Qn=Nfrac+(1−z−1)2Qn
Note that the induced quantization noise undergoes 2nd-order highpass shaping.
In
In the loop filters 500, the HDPLL loop gain may be normalized via the gain normalization (Gnorm) factor 508. The gain normalization factor 508 may decouple the HDPLL dynamic operation from process, voltage, temperature (PVT) dependent parameters such as the DCO gain. The PLL 100 may implement filter coefficients (e.g., 504, 506) that are powers of two, and therefore facilitate digital hardware implementation, e.g., as digital bit-shifting operations. None of the factors, including the gain normalization factor Gnorm 508, need to be a power of two, however. The digitally intensive HDPLL dynamic control facilitates on-demand bandwidth control, sometimes referred to as gear shifting. The digital dynamic control also facilitates effective addressing of parasitic spurious noise, e.g., injected via the power supplies or coupling between the DCO and the crystal (Xtal) reference.
The hybrid delta sigma phase/frequency detector (ΔΣ PFD) of PLL 100 may be implemented with other optional features. For instance, it may include digital re-quantization, adaptive noise filtering, or both. In some implementations, the hybrid ΔΣ PFD may include a multiple bit flash ADC, with a corresponding DAC that operates on fewer bits facilitating less complex DEM for the DAC and with a low complexity dither DSP that has relaxed digital noise performance. The reduction in the complexity of the DAC and dither DSP facilitates implementation in less silicon area with lower latency digital hardware.
In some implementations, a high flash ADC resolution enhances the performance of the hybrid ΔΣ PFD, and as a result, the PLL uses a high resolution current mode DAC in the feedback path of the ΔΣ ADC. To address negative effects that may be associated with analog component mismatches in the feedback DAC, the PLL may include dynamic element matching (DEM) to noise shape mismatch errors. Increasing the number of DAC quantization levels (e.g., beyond five) may result in considerable increases to the complexity of the DEM algorithm, and impose latency constraints.
To reduce the feedback DAC and related DEM algorithm complexity to up to several quantization levels (e.g., up to five), the fine M-level flash ADC output is temporarily re-quantized to a coarser K-level grid to drive the feedback DAC. The resulting re-quantization error is properly recombined with the flash ADC output to restore M-level resolution. A digital noise shaping requantizer is utilized so that the re-quantization error does not mask the noise shaping performance of the ΔΣ ADC (e.g., 1st-order).
The adaptive filter 1304 provides adaptive cancellation of known noise affecting the dither DSP 1310 and hybrid ΔΣ PFD. The adaptive cancellation helps to achieve wide PLL bandwidth. In turn, a wide PLL bandwidth provides more stable tracking and higher rejection of the DCO phase noise which allows for relaxed DCO power consumption. The adaptive filter 1304 may be implemented as described below with regard to
Note that in fine resolution (FineRes) detection mode, the ADC 204 is configured to produce multi-bit phase/frequency error digitization with drastically reduced ΔΣ quantization noise, according to its resolution (Δ<1). The dither DSP 402 interfaces the high-resolution ADC output to the lower-resolution grid of the MMD control (e.g., through a digital ΔΣ modulator). Detector linearity requirements often calls for small valued integer MMD control span (e.g., in the range [−3, +3]), which in turn may limit the available choices of low-complexity noise-shaping dither DSP topologies. In such cases a low-order dither DSP may be used (e.g., a dither DSP with 3rd-order ΔΣ noise shaping characteristics). The adaptive filter 1402 may cancel out the noise contribution from the dither DSP to the hybrid ΔΣ PFD output Bout by utilizing the readily available digital quantization noise signal Qn,dth 1404.
As another benefit, the adaptively configured filter 1406 captures the dynamic performance of the hybrid ΔΣ PFD as seen by the dither DSP induced quantization noise Qn,dth to the detector output Bout. In other words, the adaptation of the filter 1406 reveals additional information about the dynamic performance of the hybrid ΔΣ PFD. The information may be used in other systems to understand and make further adaptations to the performance of the hybrid ΔΣ PFD.
where Hs is the signal transfer function of the 1st-order ΔΣ ADC and gn the normalized integrator gain.
A typical bandwidth configuration of the ΔΣ ADC (e.g., several MHz range for gn>0.5) may exceed the PLL loop bandwidth (e.g., a few hundreds of kHz range) and for those frequencies Hs is approximately 1. This allows the cancellation filter to be safely replaced by a delay element and the residual high frequency noise-shaped re- quantization error be rejected by the PLL loop filter.
Various implementations of the PLL 100 have been specifically described. However, many other implementations are also possible.
Fine resolution encoding may generally refer to a quantization step Δ less than 1. The PLL 100 uses quantization steps less than one (Δ<1) together with the fine resolution encoder 106 to interface the fractional valued ΔΣ ADC output with the MMD 110. The quantization step may be set according to a targeted PLL performance. Accordingly, even low-level fractional quantization may be sufficient for a target performance level, and finer grained fractional quantization may be implemented to reach higher target performance levels.
This application claims the benefit of and is a continuation in part of U.S. Non-provisional application Ser. No. 13/966,515, filed 14-Aug.-2013, which claims the benefit of priority to U.S. Provisional Application No. 61/828,108, filed 28-May- 2013 and the benefit of priority to U.S. Provisional Application No. 61/856,278, filed 19-Jul.-2013, all of which are entirely incorporated by reference.
Number | Date | Country | |
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61856278 | Jul 2013 | US | |
61828108 | May 2013 | US |
Number | Date | Country | |
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Parent | 13966515 | Aug 2013 | US |
Child | 14283652 | US |