A Fully-Differential Zero-Crossing-Based 1.2V 10b 26MS/s Pipelined ADC in 65nm CMOS Soon-Kyun Shin, Yong-Sang You, Seung-Hoon Lee, Kyoung-Ho Moon, Jae-Whui Kim, Lane Brooks*1, and Hae-Seung Lee*1, *2 Samsung Electronics, Yongin, Korea *1 MIT, Cambridge, MA *2 Cambridge Analog Technologies, Inc. Bedford, MA TEL : +82-31-209-4815, FAX:+82-31-209-1973, E-mail: [email protected] Abstract A fully-differential zero-crossing-based 10b 26MS/s pipelined ADC in a 65 nm CMOS process is presented. Switched-capacitor overshoot correction is compatible with the differential topology and allows faster operation. A CMFB is engaged in the coarse phase for constant common-mode. The 0.33mm2 ADC achieves 54.3dB SNDR with a FOM of 161fJ/step. ADC Implementation Comparator-based switched-capacitor (CBSC) circuits were introduced as an alternative way to achieve low power and to overcome the design bottlenecks of op-amps [1]. Subsequently, a zero-crossing-based circuit (ZCBC) [2], in which comparators are replaced by dynamic zero-crossing detectors, achieved higher power efficiency and speed. These approaches, however, used single-ended architectures that were sensitive to supply and substrate noise. In this paper, a fully-differential zero-crossing based pipelined ADC is described. This differential architecture offers similar benefits to op-amp based differential ADCs. The architecture of the proposed ADC based on fully-differential ZCBC is similar to the conventional ADC [3], consisting of Flash ADCs, MDACs, and digital correction logic (DCL). A load of replica MDAC is employed at the last stage to produce the same ramp rate as in other stages, because the ramp rate is a function of capacitive load. To avoid current consumption in the reference ladder in flash ADCs, a switched capacitor comparators [4] are used instead. The ADC is composed of 9 pipelined 1.5 bit stages. For simplicity of the design, Stages 2 through 9 are made identical. Stage 1 is made twice as large for lower noise. The schematics of the fully-differential ZCBC pipeline stages are shown in Fig. 1. It uses dual phase differential ramps for virtual ground detection by a zero-crossing detector (ZCD). Current sources I1 and I2 are for the coarse and the fine phases, respectively. Each current source is biased by a separate diode-connected current reference in order to maximize testability, at the cost of increased power consumption by a large factor. The timing diagram is shown in Fig. 2. The input voltage is sampled on C1, C2, C3, and C4 prior to the beginning of charge-transfer phase (the rising edge of Q1). A short preset signal P sets OUTT to GND and OUTC to VDD through SW1 and SW2. This ensures that the differential input to the ZCD is always negative at the start of the coarse phase. After the preset, the coarse charge-transfer phase E1 begins. The coarse current I1 charges OUTT and discharges OUTC at a fast rate until the inputs Vx and Vy cross each other. At this point, the

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Fig. 1. Implementation of 2 stages of the fully differential ZCBC 1.5b/stage ADC.

ZCD makes its first decision. Because the ZCD has a finite delay, I1 turns off shortly after Vx crosses Vy. The fast ramp rate and the finite delay in the ZCD causes overshoot during the coarse phase. In the previous work, an overshoot correction circuit with variable comparator threshold was used to reduce the overshoot voltage [1]. Fig. 2. Timing diagram. Since it is not straightforward to change the switching threshold of the fully-differential ZCD, a switched-capacitor overshoot correction circuit (OCC) has been implemented. CO1-2 are charged during the coarse phase, and the charge on CO1-2 is subtracted from C1, C2, C3, and C4 at the end of the coarse phase. This reduces the coarse phase overshoot, and maximizes the time for the fine phase for higher power efficiency without affecting the accuracy of the charge transfer at the end of the fine phase. During the coarse phase, a switched-capacitor common-mode feedback (CMFB) shown in the inset of Fig. 1 is engaged to maintain a constant output common-mode. The CMFB is used only during the coarse phase because the output voltage changes are very small in the fine phase causing negligible common-mode variation. After I1 turns off

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Fig. 4. Chip micrograph.

Fig. 3. Schematic of zero-crossing detector and timing diagram.

at the end of the coarse phase, current source I2 turns on to begin the fine charge-transfer phase E2. The current I2 is much smaller than I1 resulting in a slower ramp that generates much smaller overshoot [1]. When the inputs Vx and Vy cross again during the fine phase, the sampling signal S falls to open the sampling switches. The accurate output voltage is sampled on the next stage capacitors C1‫׳‬,C2‫׳‬,C3‫ ׳‬and C4‫ ׳‬at that instant. The final overshoot in the fine phase is constant and contributes a constant input referred offset in the ADC. A single differential ZCD is used for both the fine phase and the coarse phase to reduce power consumption. The ZCD has two stages of differential amplifiers A1 and A2 followed by dynamic inverters DI1 and DI2 as shown in Fig. 3. The differential amplifier stages provide voltage gain and common-mode and power supply rejection. The first stage A1 is a band-limited stage in order to control noise. The diode-connected loads M3-4 are used to avoid explicit common-mode feedback. M1-2 reduce the drain current of M3-4 to increase gain. Since a dynamic inverter can detect only a negative-going change of the input signal, DI1 and DI2 are used during the coarse and fine phases, respectively. Da and Db are pre-charging signals for dynamic inverters DI1 and DI2. They make their decisions when their inputs Oy and Ox fall below their switching threshold. The switching threshold of DI1 and DI2 are maintained constant because their input waveforms Oy and Ox are invariant. The signals S, E1, and E2 are generated from the ZCDs’ outputs COMP1-2 and signals P and Q1 by combinational logic. When Oy falls below DI1’s threshold, the COMP1 rises rapidly, finishing the coarse phase. At the start of the fine phase, Db goes low and finishes precharging DI2. MP2 waits until Ox falls below DI2’s threshold. After the output of DI2 COMP2 rises, the sampling signal S falls to take the sample of the output. E2 turns off shortly after S goes down, turning off the fine phase current source. This ensures the linearity of the ramp until after the sample of the output is taken. Experimental Results A prototype fully-differential ZCBC pipeline ADC is fabricated in a 65nm 1.2V CMOS process. The active die area of the ADC excluding bias block and test circuits is 0.33mm2 as shown in Fig. 4. The measured results of the ADC are shown in Fig. 5. The DNL and INL are +0.16/-0.22LSB and

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Fig. 5. Measured output spectrum, DNL, and INL.

+0.45/-1.21LSB, respectively. The SNDR with a 12.9MHz input tone, is 54.3dB (8.73 ENOB), and the SFDR is 70.4dB. Table I shows the performance summary. The core ADC power consumption excluding the bias block and test circuits is 1.78mW, resulting in a 161fJ/step FOM. As explained previously, the bias block is designed for maximum test flexibility at the cost of substantial increase in power consumption. The power consumption of the bias block is 3.73mW, which can be significantly reduced by not synthesizing the bias voltages individually for the various stages and by employing bypass capacitors at the bias nodes. Even when the excessively high power consumption of the bias block is included, the resulting FOM is 499fJ/step. References [1] John K. Fiorenza, Todd Sepke, Peter Holloway, Charles G. Sodini, and Hae-Seung Lee, “Comparator-Based Switched-Capacitor Circuits for Scaled CMOS Technologies,” IEEE J. Solid-State Circuits, vol.41, pp.2658-2668, Dec., 2006. [2] Lane Brooks, Hae-Seung Lee, “A Zero-Crossing-Based 8b 200MS/s Pipelined ADC,” ISSCC Dig. Tech. Papers, pp. 460-461, Feb., 2007. [3] S. H. Lewis, H.S.Fetterman, G. F. Gross, R. Ramachandran, and T. R. Viswanathan,“A 10-b 20-Msample/s Analog-to-Digital Converter,” IEEE J. Solid-State Circuits, vol.27, pp.351-358, Mar., 1992. [4] A. M. Abo, P. R. Gray, “A 1.5-V, 10-bit, 14.3-MS/s CMOS Pipeline Analog-to-Digital Converter,” IEEE J. Solid-State Circuits, vol.34, pp.599-606, May, 1999. TABLE I. Performance Summary Technology 65nm CMOS 1-Poly 6-Metal Supply voltage 1.2V Resolution 10b Sampling frequency 26MS/s Full-scale analog 1.0Vpp Die area 0.33*1mm2 / 0.56*2mm2 Power consumption 1.78*1mW / 5.51*2mW DNL +0.16 / -0.22LSB INL +0.45 / -1.21LSB ENOB 8.73b FOM 0.161*1pJ/step / 0.499*2pJ/step *1 : ADC Core only *2 : Including bias and test blocks

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22.2 A Fully-Differential Zero-Crossing-Based 1.2V 10b ...

which comparators are replaced by dynamic zero-crossing detectors, achieved .... of the ADC excluding bias block and test circuits is 0.33mm2 as shown in Fig.

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