Analog Filter Design: Current Design Techniques and Trends Edgar Sánchez-Sinencio Distinguished and TI J. Kilby Chair Professor Educational Session ES2-2 Analog Active Filters: Introduction and motivation • Analog Filters are used in a host of applications and are key building blocks in a number of applications. • The main components in active filters are Op Amp (VCVS) or Transconductance Amplifier (VCCS), resistors and capacitors. • In this presentation we discuss different implementations of non- conventional Amplifiers and their strengths and weakness. • Also we present different non-conventional filter topologies in different domains and/or their implementations. • Linearity of amplifiers/filters* is still an important active research area, not discussed here for lack of time. * M. Mobarak, M. Onabajo, J. Silva-Martinez and E. Sanchez-Sinencio, "Attenuation-Predistortion Linearization of CMOS OTAs With Digital Correction of Process Variations in OTA-C Filter Applications," in IEEE Journal of Solid-State Circuits, vol. 45, no. 2, pp. 351-367, Feb. 2010 2 Analog Active Filters: Outline • Continuous-Time Filters – Active-R – Switched-R – Ring Oscillator Based – PWM Based – Inverter Based OTA-C – Hybrid Filter CT + DT 3 Analog Active Filters: Outline • Continuous-Time Filters – Active-R Why? – The Gm-C filters are operated in open loop and thus have modest linearity. οGm-C filter depend on the transconductance gain Gm and are PVT sensitive but a good tuning technique has solved those problems. ο Active-R deserves an opportunity to challenge conventional Gm-C filters 4 Active-R: Basic concept • Uses the low-pass characteristics of transistors instead of capacitors to implement lossy integrators. π3ππ΅ = πΊπ΅π π 1+ 2 π 1 [1] Brand, J.R.; Schaumann, R., "Active R filters: review of theory and practice,“ IEEE Journal on Electronic Circuits and Systems, vol.2, no.4, pp.89,, July 1978 5 Active-R filters: Tradeoffs ο ω0 in the order of magnitude of GBW ο No need for feedback capacitors ο Can compete with Gm-C filters ο Sensitive to PVT ο Load resistance affecting DC gain ο Take into account higher-order poles i.e. πΊπ΅π −π π πΊπ΅π π΄ π = π ≅ (1 − π π) π π 6 Active-R: Basic concept Uses the low-pass characteristics of Op Amps instead of capacitors to implement integrators. Lossy Integrator αR Vi R - Building blocks Lossless Integrator Vi Vo A(s) R αR -A(s) + Vo + π΄(π ) = πΌ π 1+ (1 + πΌ) πΊπ΅π α α′ = α+1 πΊπ΅πα′ π΄(π ) = π [1] Brand, J.R.; Schaumann, R., "Active R filters: review of theory and practice,“ IEEE Journal on Electronic Circuits and Systems, vol.2, no.4, pp.89,, July 1978 7 8 9 10 Comparison First-Order Gm-C vs. Active-R 11 Bandpass – 2nd order Active-R filter 2R3 R4 Vi 2R3 -A (s) R2 + 1 + VoLP A2(s) VoBP R1 - π€βππ π‘βπ πππ΄ππ πππππ : ππ1 βͺ πΊπ΅π1 & ππ2 βͺ πΊπ΅π2 π»π΅π π ≈ π0 = π0 π + ππ2 π π π 2 + 0 π + π02 π −π»0 πΊπ΅π1 ⋅ πΊπ΅π2 ⋅ πΌ ⋅ π /π 1 πΌ= π= π 42 πΊπ΅π2 ⋅ πΌ ⋅ πΊπ΅π1 ⋅ π ⋅ 2π 3 π 1 π 1 + π 2 π = π 4 ||π 3 π΄π π = πΊπ΅π π + ππ [2] Venkateswaran, S., "Multifunction active R filter with two operational amplifiers," Electronics Letters , vol.14, no.23, pp.741,742, November 9 1978 [3] Rao, K.R.; Srinivasan, S., "A bandpass filter using the operational amplifier pole," Solid-State Circuits, IEEE Journal of , vol.8, no.3, pp.245,246, June 1973 12 13 14 Remarks on comparison Gm-C vs. Active-R filters 15 Analog Active Filters: Outline • Continuous-Time Filters – Active-R - Switched-R - Ring Oscillator Based - PWM Based - Inverter Based OTA-C - Hybrid Filter CT + DT 16 Why switched-R? • Switched-R (SW-R) filters employ switches to adjust the time constant of the filter by changing the duty cycle of the clock controlling the switches. ο Allows for continuously tunable filters that can offer a flexible solution for wide ranges of adjustable bandwidth 17 What are switched-R? Φ(t) periodic with “TS” and ON period “TON” • Duty-cycle controlled switches are used to control the amount of charge transferred through a resistor to a capacitive element. πππ πππ π·= = ππ πππ + πππΉπΉ π= π πΆ π· • The overall effective resistance is defined as the ratio of applied voltage to average current which flows to the branch over one clock period: π ππ π = π· 0<π·≤1 [1] Kaehler, J.A., "Periodic-switching filter networks-a means of amplifying and varying transfer functions," IEEE Journal of Solid-State Circuits, vol.4, no.4, pp.225,230, Aug 1969 [2] Kurahashi, P.; Hanumolu, P.K.; Temes, G.C.; Un-Ku Moon, "Design of Low-Voltage Highly Linear Switched-R-MOSFET-C Filters,“ IEEE Journal of Solid-State Circuits, vol.42, no.8, pp.1699,1709, Aug. 2007 18 First-order filter example Charging phase • The complementary switch (SWc) stirs current to ground when SW is off such that the current loading through the resistor branches is consistent over both clock phases. Vo Hold phase ππππ π 1 πΆ1 = π· Continuous (100% duty-cycle) 75% duty-cycle 50% duty-cycle 25% duty-cycle For a step input: πππππ = 1 − π·π‘ − π π 1πΆ π’(π‘) 19 First-order filter example • Switched-R filter can allow the realization of continuously tunable filters by controlling the duty cycle. S-1R π − π 2 1 π» π = π 1+π 3ππ΅ π3ππ΅π −1π R2=R1 π· = π 2 πΆ [2] 20 Issues on switches for SW-R vs. SC Filters • SW-R filters do not contain floating switches on large signal nodes, which can result in switching limitations on low voltage operation when implementing SC filters. May require clock bootstrapping [3]. [3] S. Xiao, J. Silva, Un-Ku Moon and G. Temes, "A tunable duty-cycle-controlled switched-R-MOSFET-C CMOS filter for low-voltage and high-linearity applications," ISCAS '04. Proceedings of the 2004 International Symposium on Circuits and Systems, 2004, pp. I-433-6 Vol.1. 21 S-2R architecture π2 + π1 π» π =− π 1+π 3ππ΅π−2π π3ππ΅π −2π = • There are two paths that charge the cap. • Each path is associated with a different time constant. • There is no hold period unlike S-1R. • S-2R networks are less sensitive to slew rate limitation, relaxing the requirements of the amplifier and reducing the clock harmonic distortion at the output. 1 1 π· 1−π· + = + π1 π2 π1 π 1 π2 π 2 1 1+ π₯−1 π· 1 = πΆ π₯π1 π 1 πΆ k2R2 π₯= π1 R1 [4] Jiraseree-amornkun, A.; Worapishet, A.; Klumperink, E.; Nauta, B.; Surakampontorn, W., "Theoretical Analysis of Highly Linear Tunable Filters Using Switched-Resistor Techniques," IEEE Transactions on Circuits and Systems I: Regular Papers, vol.55, 22 no.11, pp.3641,3654, Dec. 2008 S-2R – Tuning range and distortion trade-off The S-2R topology reduces the maximum slope at the output of the filter, reducing the clock harmonic distortion at the output (HDclk) with respect to the signal component (Hdin). • Resistor ratio trade-off: ο Tuning Range increases with x. ο Clock harmonic distortion also increases with x. Δπ3ππ΅π−1π % = 2 π·πππ₯/πππ − 0.5 100% 0.5 Δπ3ππ΅π−2π % = 2 (π₯ − 1) π·πππ₯/πππ − 0.5 1 + (π₯ − 1)0.5 where π₯ = π 2 π 1 S-2R tuning and distortion trade-off 58 100% 100 56 80 54 60 52 40 50 20 48 1 2 3 4 5 6 7 Resistor ratio - x 8 9 Tuning range (%) • The frequency tuning range is defined as the range of variation of the cut-off frequency from the nominal case (D=50%). HDin/HDclk (dB) • 0 10 23 Topology comparison: S-1R VS S-2R The reduction on clock harmonic distortion at the output requires the use of a small scaling factor x, this greatly reduces the frequency tuning range of the filter, which is always smaller than the tuning range of the S-1R architecture. X=2 πΉπΌπ = 100πΎπ»π§ πΉπΆπΏπΎ = 16ππ»π§ Clock to signal freq. ratio: πΉπΆπΏπΎ πΉπΌπ = 160 24 fin=2kHz fs=128MHz Op-Amp GBW=20MHz Higher-order filters • Higher order filters using switched-R can be realized using the Switching-R topologies, like the biquad structure proposed in [3]. Rb1 and Rb2 resistors are added to bias the input of the Op-Amps (PMOS input) near ground, allowing low voltage operation. [5] Kurahashi, P.; Hanumolu, P.K.; Temes, G.; Un-Ku Moon, "A 0.6V Highly Linear Switched-R-MOSFET-C Filter," CICC '06. IEEE 25 Custom Integrated Circuits Conference, 2006, vol., no., pp.833,836, 10-13 Sept. 2006 Linearity of Switched-R filters • The harmonics of the clock appear on the output spectrum of the filter. • Using high frequency clocks can alleviate this problem. οPush the clock harmonics to higher frequencies, which can be easily filter out. οHowever, this increases power consumption, makes the control of the duty cycle challenging and can result in additional distortion from slewrate limited operation. 26 How can we reduce clock harmonic distortion without compromising tuning range? One solution: Clock’s spurious tone cancellation (1/2) • In order to avoid using high frequency clock signals a harmonic cancellation technique [5] can be employed to cancel out the spurious tones coming from the clock. πππ’π‘ • 1 ππ = − [π ππ ∗ πππ πΆ ππ 4π −3πππ 4 cos ππ ππ cos 2 4 ππππ ππ , π = π/ππππ Multiple paths are introduced with a delay (phase shift), which cancel harmonic components of the clock without affecting the fundamental. e-s3T/4 -s3T/4 e Vclk(s) e-sT/2 Vclk(s) 1/R e-sT/2 1/R e-sT/4 -sT/4 e 1/R 1/R 1/R 1/R 1/R 1/R Vin(s) OA 1/R 1/R Vo(s) Vin(s) OA 1/R Vo(s) 1/R Lossless integrator First order low-pass filter [6] Soto-Aguilar S., Alagappan, A., Sanchez-Sinencio, E., “Clock Harmonic Distortion Reduction Technique for Full Tunable Range in Switched-R-MOSFET-C 27 Filters“, Journal of Analog Integrated Circuits and Signal Processing, to be published. [5] Clock’s spurious tone cancellation (2/2) ο The technique employs 4 phases to cancel the first tree harmonics while still maintaining 100% frequency tuning range, unlike S-2R. ο Cancellation is sensitive to mismatch between the multi-phase paths First clock harmonic appears at 4πΉπππ 28 COMPARISON SUMMARY Topology S-1R S-2R Multi-phase S-1R Harmonic distortion 1st order active filter 47dB Tow-Thomas biquad 45dB 1st order active filter 57dB Tow-Thomas biquad 55dB 1st order active filter 98dB Tow-Thomas biquad 88dB Tuning range 100% 34% 100% [6] Switches Ron = 36.59Ω OTA: ADC = 49.9dB, UGB = 102.33MHz 29 Analog Active Filters: Outline • Continuous-Time Filters - Active-R Switched-R Ring Oscillator Based PWM Based Inverter Based OTA-C Hybrid Filter CT + DT 30 Ring Oscillators as Integrators • A ring VCO is an integrator with voltage input and phase output πππ’π‘ πΎππΆπ = π£ππ π π • Advantages: οInfinite DC gain οProcess scalable οCan operate with low supply voltages • • M. Park, et al., "A multiphase PWM RF modulator using a VCO-based opamp in 45nm CMOS,”, IEEE RFIC, 2010, pp.39-42. 31 B. Drost, et al., "Analog Filter Design Using Ring Oscillator Integrators,” IEEE JSSC, Dec. 2012, pp.3120-3129. RO Integrator with Current Input and Current Output π»πΌππ π πΌπππ πΎπΆπ πΎπΆπΆπ πΎππ· = = πΌπΌπ π • Use PD+CP for phase-to-voltage/current conversion to interface with other building blocks • IOUT is PWM current signal • • M. Park, et al., "A multiphase PWM RF modulator using a VCO-based opamp in 45nm CMOS,”, IEEE RFIC, 2010, pp.39-42. 32 B. Drost, et al., "Analog Filter Design Using Ring Oscillator Integrators,” IEEE JSSC, Dec. 2012, pp.3120-3129. RO Integrator Non-Idealities -1 • Spurious Tones – Increase FOSC ο Push out harmonics ο Higher power consumption ο Poor linearity as on/off time of the PWM signal gets comparable with rise/fall time of PD and CP • • M. Park, et al., "A multiphase PWM RF modulator using a VCO-based opamp in 45nm CMOS,”, IEEE RFIC, 2010, pp.39-42. 33 B. Drost, et al., "Analog Filter Design Using Ring Oscillator Integrators,” IEEE JSSC, Dec. 2012, pp.3120-3129. RO Integrator Non-Idealities -2 • Spurious Tones – Multiphase PWM ο Cancel all tones up to MFOSC ο Prone to mismatch • • M. Park, et al., "A multiphase PWM RF modulator using a VCO-based opamp in 45nm CMOS,”, IEEE RFIC, 2010, pp.39-42. 34 B. Drost, et al., "Analog Filter Design Using Ring Oscillator Integrators,” IEEE JSSC, Dec. 2012, pp.3120-3129. RO Integrator Non-Idealities -3 • Non-Linearity – VCO: Non-linear voltage/current-to-frequency conversion • Pseudo-differential architecture ο Cancel even order harmonics – PD+CP: Non-linear behavior when on/off time of the PWM signal becomes comparable to rise/fall times. • Limit max duty cycle to be less than 90% • B. Drost, et al., "Analog Filter Design Using Ring Oscillator Integrators,” IEEE JSSC, Dec. 2012, pp.3120-3129. 35 RO Integrator Non-Idealities -4 • Integrator Parasitic Poles – Parasitic pole at VCO supply node • Add linear resistance RC at supply node ο Pushes parasitic pole to higher frequency ππππ = 1 π ππΆπ π πΆ πΆπ π π < π ππΆπ ο Improve VCO linearity because it appears in parallel with non-linear RVCO ο Reduce loop gain when ROI is utilized in feedback system • B. Drost, et al., "Analog Filter Design Using Ring Oscillator Integrators,” IEEE JSSC, Dec. 2012, pp.3120-3129. 36 First-Order LPF Using RO Integrator • 3-db bandwidth tuning by varying feedback CP current π»πΏππΉ π = 1 π πΌπ πΎπΆππΉπ΅ 1 + 1 π πΎπΆππΉπ΅ πΎπΆπΆπ πΎππ· πΎπΆππΉπ΅ = π × πΌπΆπ • B. Drost, et al., "Analog Filter Design Using Ring Oscillator Integrators,” IEEE JSSC, Dec. 2012, pp.3120-3129. 37 Tow-Thomas Biquad Using RO Integrator • Frequency tuning by changing CP bias currents π»πΏππΉ π = • 1 π πΌπ πΎπΆππΉ 1 π 2 πΎπΆπΆπ1 πΎπΆπΆπ2 πΎππ·1 πΎππ·2 πΎπΆπ1 πΎπΆππΉ πΎπΆπ2 π +1 πΆπΆπ1 πΎππ·1 πΎπΆπ1 πΎπΆππΉ +πΎ B. Drost, et al., "Analog Filter Design Using Ring Oscillator Integrators,” IEEE JSSC, Dec. 2012, pp.3120-3129. 38 Tow-Thomas Biquad Using RO Integrator • Frequency tuning and Q tuning by changing CP bias currents Q=1.5 Q=1 Q=0.7 KCP1=KCPF=108 µA Q=0.7 fo=1-20 MHz Q=0.7-1.5 fo=20 MHz 39 ROI-based Filter Design: An Example • ROI-based LPF with BW=100kHz π»πΏππΉ π = 1 π πΌπ πΎπΆππΉπ΅ 1 + 1 π πΎπΆππΉπ΅ πΎπΆπΆπ πΎππ· Parameter Value fCCO 100 MHz KCCO 400 MHz/A KPD 1/π KCPFB 392.7 µA RIN 1 kΩ 40 Simulation Results – Frequency Response 41 Simulation Results – Output Waveforms M=2 M=1 M=8 42 Simulation Results – Spectral Purity ππΌπ = 100 ππ»π§ 43 Ring Oscillator Based Amplifier (ROA) • Another approach is to use the ring oscillator as an infinite DC gain Opamp in an active-RC filter topology. Zero Compensation • Spurs at VCO oscillation frequency are filtered out if the oscillation frequency is greater than the desired signal bandwidth • Effect of non-linearity is improved because of the feedback loop • C. W. Hsu and P. R. Kinget, "A 40MHz 4th-order active-UGB-RC filter using VCO-based amplifiers with zero compensation," ESSCIRC 2014 - 40th, Venice Lido, 2014, pp. 359-362. 44 Ring Oscillator Based Amplifier (ROA) • 3rd-order Chebyshev active-RS filter using amplifiers with different DC gains and the ROA • C. W. Hsu and P. R. Kinget, "A 40MHz 4th-order active-UGB-RC filter using VCO-based amplifiers with zero compensation," ESSCIRC 2014 - 40th, Venice Lido, 2014, pp. 359-362. 45 Open Challenges ο§How to improve linearity of the ROI-based filter •Linearity of the filter is limited by the non-linear current/voltage-tofrequency conversion of the RO since it operates in open loop. ο§How to utilize ROI in discrete time filters •So far ROI is only used in continuous time filters. ο§How to cancel spurious tones effectively •Multiphase technique is prone to mismatch 46 Analog Active Filters: Outline • Continuous-Time Filters - Active-R Switched-R Ring Oscillator Based PWM Based Inverter Based OTA-C Hybrid Filter CT + DT 47 PWM Filter Design • The basic idea of Pulse-Width Modulation (PWM) filters is to replace the linear output stage (Class-A or ClassAB) with a non-linear stage (Class-D). 48 PWM Filter Design • Advantages ο Building blocks are less sensitive to voltage supply reduction ο It takes advantage of higher fT as technology scales ο Theoretical rail-to-rail output swing • Disadvantages ο Strong out of band harmonic components due to the switching frequency ο Complex implementation compared to standard filter architectures ο The modulators consume a significant amount of the power in the system 49 PWM First-Order Filter • A Fully-Differential lossy integrator is used to illustrate VA+ VA- VS+ VS- Parameter Value VDD 1V R2, R1 10 kΩ C 4 pF F-3dB 4 MHz LPF 80 MHz CLPF 2 pF RLPF 1 kΩ FS 200 MHz Vtri 550 mVpk-pk A0 35 dB THDVA+-VA- -45 dB 50 Simulation Results of First-Order Filter Vout = Vout+-Vout- Parameter Value VDD 1V fin 100 kHz Vin,Diff 800 mVpk THD -45.2dB (0.55 %) HD2 -62.5 dB (0.01%) HD3 -48 dB (0.29%) HD5 -48.5 dB (0.25%) BW = 4 MHz 51 Simulation Results for one and four phases PWM filter After filter Before filter THD =-14 dB Before filter THD =-24 dB After filter THD =-14 dB THD =-36 dB Vout Diff. Parameter Single Phase 4-Phase VDD 1V 1V fin 100 kHz 100 kHz FS 200 MHz 200 MHz Vtri 550 mVpk-pk 550 mVpk-pk MHighest Spur 400 MHz 1.6 GHz Comparators 2 8 Out-of-Band THD ~ 7.31 % 52% ~ 1.86 PWM Filter Design • Current State-of-the-art: Multi-Phases to push out harmonics Fs,eff = 2.4 GHz FBW = 70 MHz Fs,eff / FBW = 34 • Vigraham, B.; Kuppambatti, J.; Kinget, P.R., "Switched-Mode Operational Amplifiers and Their Application to Continuous-Time 53 Filters in Nanoscale CMOS," IEEE Journal of Solid-State Circuits, vol. 49, no. 12, pp. 2758-2772, Dec. 2014 PWM Filter Design • Current Challenges 1. To effectively remove the modulation frequency at the output of the OpAmp 2. To determine the trade-offs between power, filter bandwidth and linearity 3. To explore more PWM filter architectures 54 Analog Active Filters: Outline • Continuous-Time Filters - Active-R Switched-R Ring Oscillator Based PWM Based Inverter Based OTA-C Hybrid Filter CT + DT 55 Basic Concepts ο§Motivations •High data rate communication applications need filters with several 100s MHz bandwidth οΌHard disk drive, UWB communications •Technology/Power supply voltage scaling makes typical analog design such as OTAs more difficult οΌReduced headroom/dynamic range/intrinsic gain ο§Inverter-based OTA •Good for low voltage low power high speed applications οΌOnly one high impedance node at the output οΌClass AB operation ο§Bram Nauta, “A CMOS transconductance-C filter technique for very high frequencies,” in IEEE J. Solid-State Circuits, vol. 27, no. 2, pp.142-153, 56 Feb. 1992 Inverter as a transconductor (Gm) I OUT ο½ ο g mp οVin NEXT I OUT ο½ ο g mn οVin I OUT ο½ ο( g mn ο« g mp ) οVin ? ο§ One MOSFET transistor is essentially the simplest Gm cell ο§ Inverter is a current-reused Gm cell consisting of complementary PMOS and NMOS ο§It sounds good, but there are several design issues for OTA applications •How to stabilize output common mode •How to increase output resistance (DC gain) •How to enhance linearity 57 Class AB Inverter PMOS OFF NMOS OFF ο§VDD =1V, VOCM = 0.5V 58 Class AB Inverter as a high speed Gm GM Z OUT _ CM ο½ g m _ red 1 ο« g m _ blue ο§Inverter-based OTA’s class AB operation 1 Z ο½ OUT _ DM VTHN ο« VTHP οΌ VDD g m _ red ο g m _ blue ο§Green inverters ο Main GM cell ο§Red inverters ο Common mode control/Q tuning using supply ο§Blue inverters ο Negative gm for DC gain enhancement ο§Balanced configuration for linearity improvement ο§Bram Nauta, “A CMOS transconductance-C filter technique for very high frequencies,” in IEEE J. Solid-State Circuits, vol. 27, no. 2, pp.142-153, 59 Feb. 1992 Inverter-based vs. Conv. OTA-based ο§Power supply voltage determines inverter-based OTA’s class and the optimal design point ο§Class AB inverter-based OTA is good for high speed and low power ο§Class C inverter-based OTA is used in SC filter applications ο§Youngcheol Chae and Gunhee Han, “Low voltage, low power inverter-based switched-capacitor delta-sigma modulator,” in IEEE J. Solid-State 60 Circuits, vol. 44, no. 2, pp.458-472, Feb. 2009 Class AB Inverter-based Gm-C first order LPF ο§VDD=1V, GM= 4.6mS, CINT=50fF ο§DC gain = 30dB, fu=6.3GHz Parasitic cap degrades fu Vid=10mV fin=10MHz THD=2% 61 Linearity Enhancement ο§Joeri Lechevallier, Remko Struiksma, Hani Sherry, Andreia Cathelin, Eric Klumperink, and Bram Nauta, “A Forward-Body-Bias Tuned 450MHz Gm-C 3rd-Order Low-Pass Filter in 28nm UTBB FD-SOI with >1dBVp IIP3 over a 0.7-to-1V Supply,” in ISSCC Dig. Tech. Papers, pp.96-97, Feb. 62 2015 Open Challenges ο§How to enhance inverter’s DC gain •Cascode and Gain-boosting makes DC gain traded off with output swing (SFDR) ο§Tuning without an LDO regulator •Dropout voltage is bad for low supply voltage ο§How to deal with PVT variation •Mismatch leads to PSRR/CMRR aggravation in pseudo-differential topologies ο§MHz~GHz frequency tunable filter design for high data rate communication applications ο§Hao Luo, Yan Han, Ray C.C. Cheung, Xiaopeng Liu, and Tianlin Cao, “A 0.8-V 230-uW 98-dB DR Inverter-Based SD Modulator for Audio Applications,” in IEEE J. Solid-State Circuits, vol. 48, no. 10, pp.2430-2441, Oct. 2013 ο§Fawzi Houfaf, Mathieu Egot, Andreas Kaiser, Andreia Cathelin, and Bram Nauta, “A 65nm CMOS 1-to-10GHz Tunable Continuous-Time Lowpass Filter for High-Data-Rate Communications,” in ISSCC Dig. Tech. Papers, pp.362-363, Feb. 2012 ο§Joeri Lechevallier, Remko Struiksma, Hani Sherry, Andreia Cathelin, Eric Klumperink, and Bram Nauta, “A Forward-Body-Bias Tuned 450MHz Gm-C 3rd-Order Low-Pass Filter in 28nm UTBB FD-SOI with >1dBVp IIP3 over a 0.7-to-1V Supply,” in ISSCC Dig. Tech. Papers, pp.96-97, Feb. 63 2015 A New Look: Digital-based Op-Amp ο§Motivations • A step towards Analog Design Automation • Reduced layout design cycle via commercially available synthesis tools ο§Digital Standard Cell-based Op-amp • Extended concept of an inverter-based OTA • Programmability with respect to required amplifier specifications • Fully synthesizable ο§Jun Liu, Ahmed Fahmy, Taewook Kim, and Nima Maghari, “A Fully Synthesized 0.4V 77dB SFDR Reprogrammable SRMC Filter Using Digital 64 Standard Cells,” in IEEE Custom Integr. Circuits Conf., vol. 27, no. 2, pp.142-153, Sep. 2015 Mapping to NAND/NOR-based Amplifier ο§Inverters are replaced with NAND/NOR gates for common mode feedback implementation ο§Jun Liu, Ahmed Fahmy, Taewook Kim, and Nima Maghari, “A Fully Synthesized 0.4V 77dB SFDR Reprogrammable SRMC Filter Using Digital 65 Standard Cells,” in IEEE Custom Integr. Circuits Conf., vol. 27, no. 2, pp.142-153, Sep. 2015 NAND/NOR-based Amplifier uOP A0=23dB, BW=16MHz CMOS 180nm ο§ NAND/NOR-based unit amplifier can be used in the pseudo differential amplifier ο§Common mode feedback employs an inverter chain ο§A single stage has low gainο BAD 66 Towards a Higher Gain Amplifier Negative resistance to enhance output resistance Feedforward compensation ο§Cascade the unit amplifiers with feed-forward compensation for stability ο§Use negative resistance (cross-coupled tri-state inverters) to increase voltage gain 67 1st Order LPF using digital gates GAIN=1 BW=1MHz R1=100k RF=100k CF=1.59p Lossy Integrator Freq. Response BW=1MHz at VDD=0.8 mOP Freq. Response VDD=0.8 68 2nd Order LPF using digital gates GAIN=1 f0=1MHz Q=0.7 R1=R2=100k RF1=70k CF1=CF2=1.59p Q=0.65 f0=1MHz at VDD=0.8 69 69 Open Challenges ο§Placement & Routing automation considering small mismatch and parasitics ο§How to design a stable amplifier with high gain from digital gates • Frequency compensation ο§How to deal with PVT variation • uOP’s bandwidth is sensitive to VDD 70 Analog Active Filters: Outline • Continuous-Time Filters – Active-R – Switched-R – Ring Oscillator Based – PWM Based – Inverter Based OTA-C – Hybrid Filter CT + DT 71 CT+DT Hybrid Baseband Filter • DT (Discrete-Time) Filter • Pros: good channel selectivity & stopband attenuation ο • Cons: poor passband flatness ο • Solution: add a CT filter to pre-distort the input signal * S.H. Shin, et al., “A 0.7-MHz–10-MHz Hybrid Baseband Chain With Improved Passband Flatness for LTE Application,” TCAS-I, Vol. 62, No. 1, pp. 244—253, Jan. 2015 72 CT+DT Hybrid Baseband Filter 10 Normalized Gain (dB) 0 -10 -20 -30 -40 -50 -60 -70 CT (2nd order LPF) Sinc Filter (sampling) MA-32 DT Filter CT+DT Response -1 0 10 10 Normalized Frequency (f ) s 73 Classical Moving Average FIR Sinc filter comes from the sampling behavior 1 1+z-1+z-2+z-3 z-1 z-2 z-3 The output sampling rate (fs.out) is not the same as the input sampling rate (fs.in) ο can’t CASCADE the same filter to obtain higher order Solution: Multi-phase Operation 74 6 phases MA-32 DT Filter Charge Sharing delayed by clock 75 Thanks to my Ph. D students in the preparation of this material: Fernando Lavalle, Adriana Sanabria Borbon, Hatem Osman, Kyoohyun Noh, Sergio Soto-Aguilar, Congying Shi and Minglei Zhang 76