a 12-bit self-calibrating sar adc achieving a nyquist 90.4-db sfdr
TRANSCRIPT
A 12-bit self-calibrating SAR ADC achieving a Nyquist 90.4-dBSFDR
Hua Fan • Xue Han • Qi Wei • Huazhong Yang
Received: 10 March 2012 / Revised: 24 June 2012 / Accepted: 3 October 2012 / Published online: 25 October 2012
� Springer Science+Business Media New York 2012
Abstract This paper describes a 10 or 12 bit program-
mable successive approximation register ADC for bridge
stress monitoring systems requiring high-resolution, high
linearity, low power and small size. Its sampling rate is
scalable, from 0 to 200 kS/s. The proposed ADC employs a
novel time-domain comparator with offset cancellation.
Prototyped in a 0.18-lm, 6MIP CMOS process, the ADC,
at 12 bit, 100 kS/s, achieves a Nyquist SNDR of 68.74 dB
(11.13), an SFDR of 90.36 dB, while dissipating 579.6 lW
from a 1.8-V supply. The on-chip calibration improves the
DNL from ?0.2/-0.74 LSB to ?0.23/-0.25 LSB and INL
from ?1.27/-0.97 LSB to ?0.41/-0.4 LSB.
Keywords Analog-to-digital converter (ADC) �Self-calibrating � Successive approximation register (SAR)
1 Introduction
With the advance of ubiquitous sensor networks focusing
on the technologies for bridge stress monitoring, industrial
monitoring, environmental control and prevention of
disasters or accidents, on-chip analog-to-digital converters
(ADCs) have been becoming essential for the development
of highly sensitive, stable, and robust sensor interfaces.
Successive approximation register (SAR) ADC is known
for its prominent energy efficiency these years [7–9, 20, 31,
27]; simple and OPAMP-less architecture also render it
more amenable to sensor network applications than other
Nyquist ADC architectures such as pipeline.
This work is aimed for general wireless sensor network
applications, in particular for bridge stress monitoring
systems. In these systems, high linearity, low power, and
low cost ADCs have been essential for the development of
highly sensitive, stable, and robust sensor networks. The
performance of the ADC, in terms of the required resolu-
tion and linearity, is important because the detectable sig-
nal amplitude is very small, and the ADC will introduce the
quantization noise and distortion to the signal, the resolu-
tion should be chosen high enough to provide the adequate
signal-to-noise-plus-distortion ratio (SNDR) and spurious
free dynamic range (SFDR). As a result, resolution and
linearity are paramount design objectives. Moreover, re-
configurability in sample rate and resolution is desirable to
allow for flexibility in the detectable signal amplitude
range. However, the linearity of SAR ADCs is usually
limited to around 10 bits due to process limitation [22]. The
main factors limiting the accuracy and linearity of the SAR
ADC are: comparator offset and capacitor mismatch (*10
bit in 0.18 lm).
In [30] at first, comparator offset is cancelled by using
all of the following three techniques: (1) two preamp stages
which achieve an overall gain of about 30 dB; (2) input
offset cancellation with auxiliary calibration capacitive
digital-to-analog converter (DAC); and (3) chopping to
remove comparator offset and reduce the 1/f noise [29].
Then, capacitor mismatch is cancelled by using another
auxiliary calibration capacitive DAC which injects a cor-
recting charge into the charge balance node for each bit
decision. The capacitor mismatch calibration makes pos-
sible the implementation of SAR ADCs with resolution
beyond the matching limit.
H. Fan (&) � X. Han � Q. Wei � H. Yang
Department of Electronic Engineering, TNList, Tsinghua
University, Haidian, China
e-mail: [email protected]
H. Yang
e-mail: [email protected]
123
Analog Integr Circ Sig Process (2013) 74:239–254
DOI 10.1007/s10470-012-9977-6
Another similar self-calibrating SAR ADC was reported
in [15]. In [15], the comparator offset is cancelled by using:
(1) preamp; (2) input offset cancellation with auxiliary cal-
ibration capacitive DAC; and (3) output offset cancellation.
It must be noted that, different from [30], where two cali-
bration DACs are introduced into the system for comparator
offset cancellation and capacitor mismatch calibration,
respectively, here, the capacitor mismatch calibration and
the comparator offset calibration make use of the same
auxiliary calibration capacitive DAC, this greatly decreases
the die area and complexity of layout. Smaller area in turn
contributes to smaller power consumption, since the smaller
parasitic capacitance reduces the required drive power.
However, the actual calibration was done via off-chip FPGA.
This paper presents a 10 or 12 bit programmable SAR
ADC that utilizes an improved capacitor–resistor network
with on-chip digital calibration technique to correct com-
parator offset and capacitor mismatch based on [30] and
[15]. There are three major differences between the
improved capacitor–resistor network and that in [30]: (1) In
[30] capacitive DAC in capacitor–resistor network is based
on two’s complement architecture. The total capacitance of
the DAC in two’s complement architecture is 2N 9 Cu,
here, N is the resolution of main DAC, Cu is the unit
capacitor in DAC. In this work, the tri-level based capaci-
tive DAC proposed in [5] is used to take the place of con-
ventional capacitive DAC in capacitor–resistor network.
This improves conventional capacitor–resistor network in
the following two aspects: first, the total capacitance of the
main DAC is 2N-1 9 Cu, only half of the conventional
capacitive DAC, so the area reduction of main DAC is
about twice. Secondly, simulation results show that the total
power consumption of 10 bit tri-level based SAR ADC is
44.8 % of the conventional SAR ADC; (2) Bottom-plates of
capacitors are used to sample the input rather than top-
plates, so there is no signal-dependent charge injection; and
(3) Tri-level based capacitor mismatch calibration method
is proposed. In Sect. 3.2, we will discuss the tri-level based
capacitor mismatch calibration in detail. In addition, a novel
digital differential time-domain comparator based on [2]
with improved offset is proposed, which, instead of oper-
ating in the voltage domain, transforms the differential
inputs into pulses and compares their arrival times. The
time-domain comparator only dissipates dynamic power by
eliminating the preamplifier in conventional voltage com-
parator. Note that the proposed time-domain comparator
can be applied to both single-ended and differential SAR
ADCs, whereas the time-domain comparator in [2] can only
be applied to single-ended SAR ADC. Furthermore, the
digital time-domain comparator has eliminated the only
analog part of SAR ADC, meaning that entire SAR opera-
tion is moved to digital-domain, which enables the SAR
ADC more amenable to technology scaling than other
Nyquist ADC architectures. This paper is organized as
follows: Section 2 describes the design and architecture of
the proposed SAR ADC. Section 3 presents the error cor-
rection and calibration process using the correction capac-
itive DAC. Section 4 shows the experimental results.
Finally, Sect. 5 provides a short conclusion.
2 Circuit design
2.1 ADC architecture
Figure 1 shows the block diagram of the 10 or 12 bit pro-
grammable differential SAR ADC. It comprises combined
capacitor–resistor network, a calibration DAC, a novel
digital time-domain comparator, and the control logic. The
combined capacitor–resistor network is composed by 10-bit
capacitive main DAC and 2-bit resistor-string sub DAC
without digital decoding [11], which provides the ADC the
flexibility to switch between 10- and 12-bit resolution if
necessary. The 10 bit main DAC is based on tri-level charge
redistribution architecture to improve the switching energy
efficiency and simplify the SAR control logic circuits.
Furthermore, the tri-level based DAC has intrinsically one
more bit resolution than the conventional DAC [5], so the
total capacitors to realize a 10-bit DAC using this approach
are halved compared with the conventional one using ‘‘trial-
and-error’’ switching procedure. The metal-insulator-metal
(MIM) capacitors in the 0.18 lm CMOS process only
match to about 10 bits; in order to achieve the desired 12-bit
resolution, a 10-bit capacitive DAC is introduced into the
system to correct the mismatches of the upper 8 bits. The
conversion plans for the 10-bit and 12-bit modes of this
ADC are shown in Fig. 2. In 10-bit 100 kS/s mode, the
main clock frequency fclk is 1.1 MHz, the conversion
requires 11 clock periods of the main clock: the first one for
the input sampling, ten periods for the bit cycles. In 10-bit
200 kS/s mode, fclk is 2.2 MHz. No calibration for com-
parator offset or capacitor mismatch calibration is imple-
mented in 10-bit mode. In 12-bit mode, the accuracy of the
SAR ADC and capacitor mismatch measurement both
heavily rely on the accuracy of the comparator, so the
comparator offset cancellation is implemented prior to the
main DAC linearity calibration; otherwise, it will result in a
linearity error. In 12-bit 100 kS/s mode, fclk is 1.3 MHz.
First, 11 clock periods are used for the comparator offset
cancellation through 10-bit calibration DAC. Then, the
capactior mismatch calibration begins by measuring the
nonlinearity due to the MSB capacitor. 13 clock periods are
required to store the digital representation of the mismatch
of the MSB capacitor. The 8 MSB capacitors are calibrated.
Thus, 104 clock periods are needed for the capacitor mis-
match calibration. In 12-bit 200 kS/s mode, fclk is 2.6 MHz.
240 Analog Integr Circ Sig Process (2013) 74:239–254
123
It is worth noting that the ADC is allowed to re-run cali-
bration any time in order to capture the temperature
dependent change in both offset and mismatch. Once the
interrupt signal for recalibration is enabled, the normal
conversion of the ADC is interrupted and calibration is
performed again.
2.2 Tri-level based capacitor–resistor network DAC
The DAC capacitor array is the basic structure of the SAR
ADC and it serves both to sample the analog input voltage
and as a DAC for generating an error voltage between the
input and the current digital representation of the analog
input value via a binary search algorithm. The DAC choice
is combined capacitor–resistor network [30]. The alterna-
tive split DAC or C-2C ladder structures are not of interest
here owing to floating nodes which strongly influence the
accuracy and linearity [32]. This capacitor array in com-
bined capacitor–resistor network, however, uses charge
inefficiently during a conversion, so the tri-level based
DAC can take place of the conventional capacitive DAC in
capacitor–resistor network.
Figures 3 and 4 detail the differences between the con-
ventional and the tri-level based switching scheme using a
3-bit SAR ADC [5]. Since the ADC is fully differential, the
operation of the positive and negative sides is complemen-
tary. For simplicity, only the positive side of the ADC
operation is described below. During sampling, shown in
Fig. 3, the top-plates of the differential capacitor arrays are
shorted to common-mode voltage VCM, and the entire
capacitor array stores the voltage VCM–VIN. Note that
VCM does not need to be exactly at the center of the full
reference range in a fully differential circuit, because it is a
common level and will be cancelled out. During the MSB
decision phase, since the MSB notifies whether the input is
larger or smaller than 0, the MSB can be determined directly
by placing the sampled differential inputs at the comparator;
in the meantime, all the capacitors’ bottom plates are
switching to the common-mode voltage VCM, resulting in
the equivalent output voltage -Vin at the inputs of com-
parator; thus, the comparator compares the input voltage
with 0 and decides the MSB code (Fig. 4(a)). Hence, the
MSB behaves like a sign bit, which reduces the capacitors by
half. If -Vin[0, 2C is switched to VREFN while the other
capacitors remain connected to VCM, dropping the voltage
at inputs of comparator to -Vin-VREF/2. If -Vin\0, 2C
is switched to VREFP, raising the voltage at inputs of com-
parator to -Vin?VREF/2. All of the remaining decisions
follow the same switching scheme, proceeding to smaller
capacitors. Finally, Vxp and Vxn converge towards VCM.
Note that the tri-level based DAC produces a proper
reference level without the largest capacitor, (4C), owing to
the additional common-mode voltage VCM. In addition,
since the DAC needs no ‘‘trial and error’’, switch-back
operations exist in the conventional design are not required.
Therefore, the MSB capacitor can be removed from the
3-bit DAC array, leading to a reduction by half of the
number of capacitors used in the ADC, and avoiding
the mismatch error at the conventional MSB transition. The
only additional cost of this method is that it uses n more
switches to initially reset all the capacitors to VCM, here, n
is the resolution of the ADC.
C C
256C CC
D0
D1
D11
VREFP
VCMVINP
VCM
VREFN
VINNVCM
Vxp
Vxn
256C
512C
VREFN
VREFP
Main DAC
SubDAC
Con
trol
lerCc
Cc
CALDAC
512C
Tri-level based architecture removesthe MSB capacitor in DAC
10
2
10
Fig. 1 10 or 12 bit programmable and digitally calibrated SAR ADC block diagram
Analog Integr Circ Sig Process (2013) 74:239–254 241
123
2.3 A novel time-domain comparator
Figure 5 shows the circuit schematic of the proposed dig-
ital time-domain comparator. It consists of an improved
voltage-to-time converter (VTC) based on [2] and a time-
to-digital converter (TDC) [19]. The VTC proposed in [2]
is shown in Fig. 6. There are two major differences
between the proposed VTC and the one proposed by
ADC power on
Normal OperationComp.
CAL DAC
Conversion ModeADC
Outputs
Normal Operation
RST
Idle
Idle
Idle
Does not work
Idle Conversion Mode
CLK
11 clock cycles 11 clock cycles
11 1 11 11 1 111
fclk=1.1M @100kS/s
(a)
ADC power on
OffsetCancel
Normal Operation
Normal Operation
Comp.
For Offset Cancel
Conversion Mode
ADCOutputs
Calibration Mode(ADC outputs are invalid)
For MismatchCal.
RST
IdleIdle
Idle
CAL DAC
CLK1 11 1 104 1 13 1 13
Idle Idle
Idle
11 clock cycles 104 clock cycles 13 clock cycles fclk=1.3MS/s@100kS/s
(b)
1
Fig. 2 ADC conversion
waveforms showing a 10-bit
100 kS/s conversion plans and
b 12-bit 100 kS/s conversion
plans
C C
2C CC
VREFP
VCMVINP
VCM
VREFN
VINNVCM
Vxp
Vxn
2C
VREFN
VREFP
VREFN
VREFP
C
2C C
VREFPVINP
VCM
VREFN
VINN
Vxp
Vxn
2C4C
4C
C
C
(a) (b)
Fig. 3 DAC during sampling
phase: a tri-level based
b conventional
242 Analog Integr Circ Sig Process (2013) 74:239–254
123
Agnes. The most important one is that the proposed VTC
achieves smaller offset by combining two discharge bran-
ches into one, as shown in Fig. 5(a), then the input-referred
offset caused by the deviation of resistors RD in Fig. 6 can
be avoided. Moreover, the proposed time-domain com-
parator can be applied to both single-ended and differential
SAR ADC, while the time-domain comparator in [2] can
only be applied to single-ended SAR ADC. TDC detects
phase difference between Outp and Outn, and manifests
this result in Out, which is also the output of the compar-
ator. TDC with symmetrical input paths proposed in [19] is
adopted in this work. However, the simple back-to-back
NAND SR-latch in [19] suffers from asymmetrical delays
between rising and falling edges. This latch can be further
replaced by a more symmetrical and faster one presented in
[25]. The operation of the time-domain comparator is as
follows: When the signal CLK is high, the nominally equal
capacitors C1 and C2 will be charged to VDD through
transistors M5 and M6, while node A is discharged to
remove any residual charge. The nodes Outp and Outn,
which are the outputs of voltage to time converter as well
as the inputs of binary phase detector, are reset to 0. The
nodes B, C, D and E are initially set to high. When CLK
makes transition to low, transistors M1 and M2 become
constant current generators and discharge capacitors C1
and C2 at a constant rate, the VTC generate a pulse delay
difference proportional to the input voltage difference. The
time-domain comparator obviates the need of preamplifier
that dissipates static power and the highly digital con-
struction of comparator offers all the benefits of the digital
CMOS technology.
The accuracy of the comparator is mainly determined by
KT/C noise voltage across C1, C2 and the latch time
margin DT .
The minimum input voltage error DVin caused by the
time error DT can be calculated as follows. When inputs of
the VTC approach to 0 (i.e. VINN & VINP = VCM),
according to iDt ¼ CDVth;INV (C1 = C2 = C), here
DVth;INV is the voltage drop across the capacitor, we can get
VINP � Vgs1
2RDDt1 ¼ CDVth;INVA ð1Þ
VINN � Vgs2
2RDDt2 ¼ CDVth;INVB ð2Þ
here VINN & VINP = VCM, we can get DVth;INVA �DVth;INVB ¼ DVth;INV )
Dt1 ¼ 2RDCDVth;INV
VINP � Vgs1
ð3Þ
Dt2 ¼ 2RDCDVth;INV
VINN � Vgs2
ð4Þ
According to (3) and (4), we can get
DT ¼ Dt1� Dt2 � 2RDCDVth;INVDVin
ðVCM � Vgs1;2Þ2ð5Þ
So the error voltage DVin caused by time error DT is equal
to:
DVin ¼ DTðVCM � Vgs1;2Þ2
2RDCDVth;INVð6Þ
The KT/C error voltage caused by charging and
discharging capacitance is equal to
VC;noise ¼ffiffiffiffiffiffiffi
KT
C
r
ð7Þ
Which is referred to the input, we can get
(a) (b)
C C
2C CC
VREFP
VCMVINP
VCM
VREFN
VINNVCM
Vxp
Vxn
2C
VREFN
VREFP
C
2C C
VREFPVINP
VCM
VREFN
VINN
Vxp
Vxn
2C4C
4C
VREFN
VREFP
C
C
0 0
Fig. 4 DAC during MSB
decision phase: a tri-level based
b conventional
Analog Integr Circ Sig Process (2013) 74:239–254 243
123
VC;noise in ¼
ffiffiffiffiffi
KTC
q
Gain¼
ffiffiffiffiffiffiffi
KT
C
r
IRDRD
Vth;INV¼
ffiffiffiffiffiffiffi
KT
C
r
VRD
Vth;INVð8Þ
Then, the accuracy of the comparator Vaccu comp can be
estimated according to (6) and (8)
Vaccu comp ¼ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi
ðVc;noise inÞ2 þ ðDVinÞ2
q
ð9Þ
In conclusion, the accuracy of the comparator can be improved
by changing the value of C and RD. What should be mentioned
is that, a possible mismatch between the two discharge bran-
ches causes an input-referred offset, which is identical to that
of the conventional voltage comparator; offset cancellation of
this comparator is described in a later subsection.
3 Digital calibration
3.1 Comparator offset cancellation
The offset in the comparator of the SAR ADC limit the
system’s performance because any input signal that is
smaller than the input offset leads to unpredictable ADC
output. Capacitor mismatch measurement also heavily
relies on the accuracy of the comparator. So the comparator
offset cancellation becomes critical. Various comparator
offset cancellation techniques have been published. One
common solution for suppressing the offset of the com-
parators is adding a preamplifier but suffers from static
power dissipation and offset from itself, which leads to the
CLK
M1VINP
VDD
C2
CLK
C1
M2
RD
VINN
Outp
M3 M4
M6M5
M7
A
INVA INVB Outn
(a)
IRD
OutOut
VDD VDD
VDD VDD
B C
M9 M8
M10 M11
D E
OutpOutn
Outn
(b)
Outp
Fig. 5 Schematic of proposed
differential time-domain
comparator a voltage-to-time
converter and b time-to-digital
converter
244 Analog Integr Circ Sig Process (2013) 74:239–254
123
limited performance of the comparator [28]. Instead of
using preamplifier, the error tolerant 1.5-bit-per-stage
conversion scheme in pipelined ADCs is a feasible method,
where wrong decisions made in earlier stages can be
compensated as long as they are within the error tolerance
range. Redundant 1.5-bit-per-stage allows large offset
calibration range, but it doubles the number of comparators
and the structure of ADC must be altered, leading to
increase in design complexity and die area [10]. Another
offset cancellation technique [8] adjusts capacitance of the
output nodes of comparator to balance the output current,
which dissipates no static power; the minimum offset step
is controlled by unit capacitance of the output nodes;
however, to keep the calibrated offset resolution, the
smallest variable step of capacitance is always smaller than
1fF [8], which is hard to realize using high precision MIM
capacitors, so it can only be implemented with voltage-
controlled variable capacitor, such as PMOS transistor. It is
difficult to control the small capacitance under process
variations, so this method is usually applied to SAR ADC
with resolution smaller than 10 bits [24].
Offset cancellation techniques that are more suitable for
low voltage and high resolution design are expected for this
SAR ADC design. An open loop successive approximation
based offset cancellation method can be used to cancel the
offset of the time-domain comparator. The offset cancel-
lation is done by shorting all capacitors at the comparator
input to the common level VCM for offset storage
(Fig. 7(a)); once the offset is known, the 10 bit calibration
DAC generates a voltage successively converging to the
stored offset through capacitive coupling (Fig. 7(b)). The
final input word of the DAC is then stored as the digital
representation of the input referred offset of the compara-
tor. Eq. (10) indicates how DAC’s outputs converge to the
stored offset, where, Vos is the offset voltage of the time-
domain comparator, DOFF is the final input word of the
DAC. VREF is difference of VREFP and VREFN, Ctotal
represents the total capacitance of the main DAC, Ccal
represents the total capacitance of the calibration DAC and
Cc is the coupling capacitor. It is clear that the maximum
offset voltage that the cancellation technique can accom-
modate is proportional to the size of the coupling capacitor
Cc. To maximize the calibration efficiency, the coupling
capacitor Cc is adjustable in order to change the calibration
range, which prevents the unexpectedly poor matching due
to limited production properties; proper value of Cc was
chosen to guarantee the offset cancellation is capable of
flexibly handling any case of comparator input offset.
Vxp� Vxn ¼ VosþCcalCc
CcalþCc VREF
Ctotalþ CcalCcCcalþCc
2DOFF;MSB � 1
21þ . . .þ 2DOFF;LSB � 1
210
� �
ð10Þ
During the capacitor mismatch measurement and ADC
normal conversion, the digital offset word is retrieved from
registers to cancel the comparator input referred offset.
Thanks to offset cancellation, device sizing of the
VDD
CLK
CLK
Vin
M5
M3
M1
M11 RD
C1
VDD
VB M2
M4
M12 RD
C2
CLK
CLK
M9
M8
M13
M7
VDD
CLK
VDD
M6
CLK
Outp
Outn
QD
CK
Out
Fig. 6 Schematic of time-
domain comparator proposed by
Agnes
Analog Integr Circ Sig Process (2013) 74:239–254 245
123
comparator is not constrained by any matching require-
ment. This is beneficial because the charge sharing between
the comparator input capacitance and the sampling
capacitor attenuates the sampled signal, so degrades the
SNR.
3.2 Capacitor mismatch calibration
The main DAC is composed of capacitors sized to produce
ratios in powers of 2, or binary ratios. Errors in these ratios
correspond to errors in conversion. Typically, the dominant
source of the largest ADC error is the DAC capacitor
mismatch error. The static linearity of SAR ADCs is usu-
ally limited to around 10 bits, so several techniques have
been reported in an attempt to improve the linearity of
ADC’s beyond the limit of matching to achieve intrinsic
linearity of 12 bits and beyond.
One approach is to simply size the capacitors large
enough and use complicated common centroid layout
technique to build a 12-bit accurate capacitor array [25].
However, as described in [12], this can impose severe die
area and power dissipation penalties.
(a)
(b)
C C
256C CC
VREFPVCMVINP
VCM
VREFN
VINNVCM
Vxp
Vxn
256C
VREFN
VREFP
Main DACP
Cc
Cc
CALDACP
CCALP
VOFFSET
CALDACN
Con
trol
ler
CCALN
Main DACN
C C
256C CC
VREFPVCMVINP
VCM
VREFN
VINNVCM
Vxp
Vxn
256C
VREFN
VREFP
Main DACP
Cc
Cc
CALDACP
CCALP
VOFFSET
CALDACN
Con
trol
ler
CCALN
Main DACN
Fig. 7 Comparator offset error
measurement
246 Analog Integr Circ Sig Process (2013) 74:239–254
123
Trimming is another technique, but it is costly in terms
of fabrication processing and chip area. Additionally, it
cannot track variations over time caused by component
aging, temperature variations, and supply voltage changes.
An example of foreground calibration is given in [23],
which requires a separate calibration reference source, and
the resistor ladder needs static current and consumes large
area and power.
Another example of foreground calibration was reported
[15] as a way to align the mismatch of capacitors using
capacitive calibration DAC, but the actual calibration was
done via off-chip FPGA.
An example of a background calibration is given in [21],
nonbinary design with radix = 1.86 can correct the mis-
match of the radix between each bit by using the pertur-
bation technique; however, in that structure, the non-
integer ratio of the capacitor significantly increases layout
complexity and needs sophisticated post-processing, and
the actual calibration was also done via off-chip software
approach.
To ease system complexity, and obviate the need of
complicated post-processing and maximally exploit the
architectural advantages of SAR, the foreground mismatch
self calibration based on tri-level DAC is introduced.
During the startup calibration, the mismatches of the
capacitor are measured by a calibration ADC after the
comparator offset cancellation is completed. The central
idea behind self-calibration is that the sum of all mis-
matching errors is 0 [17]. Each weighted capacitor Cn is
assumed to be off a factor of ð1þ enÞ from the ideal value
due to process variations. The total linearity error consists
of contributions from each capacitor ratio error [18].
It should be mentioned that because the main DAC is
tri-level based, the measurement of capacitive mismatch is
somewhat different from the conventional method. The
measurement of capacitor mismatch error is executed using
a 3-bit example shown in Fig. 8. The calibration cycle
begins by measuring the nonlinearity due to the MSB
capacitor 2C. First, MSB capacitor 2C is switched to the
VREFP and all the other capacitors are connected to VCM,
Vxp and Vxn are shorted to VCM at the same time. Then,
the bottom plate voltages are exchanged between 2C and
all the other capacitors, and the short switches are open. At
this time, the ideal residual voltage Vxp-Vxn is 0; however,
due to the MSB capacitor mismatch eMSB, the actual
residual voltage is [17]:
VresMSB ¼ Vxp� Vxn ¼ eMSBðVREFP� VREFNÞ ð11Þ
If the MSB capacitor is perfect, it will have exactly half of
the total array capacitance, the weight of MSB capacitor is
exactly 12. A ratio error in the MSB will cause a weight error,
the error voltage VeMSB due to MSB capacitor ratio error is
VeMSB ¼1
2eMSBðVREFP� VREFNÞ ð12Þ
It can be easily shown that the general relation between
residual voltage Vres and the error voltage due to MSB
capacitor ratio error is
VresMSB ¼ 2VeMSB ð13Þ
or in digital domain
DVeMSB ¼DVresMSB
2ð14Þ
Where DVeMSB and DVresMSB stand for digitized error
voltages and digitized residual voltages, respectively. Once
the first capacitor is measured, the same procedure can be
repeated to measure other capacitors one by one.
It is worth noting that the capacitor mismatch calibration
and the comparator offset calibration make use of the same
auxiliary calibration capacitive DAC to decrease die area
and complexity of layout, so the digitized offset must be
subtracted from Eq. (14), then, Eq. (14) becomes
DVeMSB ¼ ðDVresMSB � DOFFÞ � 1 ð15Þ
C C
2C CC
VREFPVCM
VCM
VREFN
VCM
Vxp
Vxn
2C
VREFN
VREFP
C C
2C CC
VREFPVCM
VCM
VREFN
VCM
Vxp
Vxn
2C
VREFN
VREFP
Fig. 8 MSB capacitor
mismatch error measurement
Analog Integr Circ Sig Process (2013) 74:239–254 247
123
Here, ‘‘ �’’ 1 represents shift right operation, and DOFF is
the digital representation of the offset voltage.
Similarly, errors due to smaller capacitors are measured
DVeMSB�1 ¼ ðDVresMSB�1 � DOFF � DVeMSBÞ � 1 ð16Þ
DVeMSB�2 ¼ðDVresMSB�2 � DOFF�DVeMSB � DVeMSB�1Þ � 1
ð17Þ
..
.
DVeLSB ¼ ðDVresLSB�DOFF �X
8
i¼2
DVeiÞ � 1ð18Þ
After each residue voltage has been digitally captured
using calibration DAC, all these error terms are stored in
digital memory.
The calculations involved in this measurement consist of
simple addition, subtraction, in combination with shift right
operations, enabling a small and efficient on-chip digital
calibration engine.
It is worth noting that the mismatch calibration logic
based on tri-level DAC is simpler than the conventional
calibration logic which must be in step with ‘‘trial and error’’
search procedure. In conventional SAR ADC, when the nth
bit is being tested, at first, the corresponding capacitor is
switched to VREFP by giving a test bit of 1, and the cor-
rection term DVen is added to the correction terms accumu-
lated from the first bit (MSB) through the (n - 1)th bit. If the
bit decision is 1, the added result is stored in the accumulator.
Otherwise, DVen is dropped, leaving the accumulator with
the previous result [18]. However, in tri-level based charge
redistribution SAR ADC, the straightforward DAC switch-
ing avoids the switch-back operations in the conventional
design, the computation of correction term just needs to be
directly performed. Assuming that the ones equal in average
to the zeros, 6 times of unnecessary subtraction operations
are avoided.
Capacitor mismatch calibration provides the opportunity
to minimize the capacitor sizes, resulting in compact
design, layout, smaller area in turn contributes to smaller
power consumption, because the smaller parasitic capaci-
tance reduces the required drive power.
4 Experimental results
4.1 ADC test setup
The prototype was fabricated in a 0.18-lm six-metal one-
polysilicon (6M1P) CMOS process with MIM capacitors.
A micrograph of the entire ADC is shown in Fig. 9. The
active area of the ADC is 1,565 9 1,772 lm with digital
circuits implemented on-chip. All measurement results
described in this section were obtained at room tempera-
ture. The testing was carried out using Printed-Circuit-
Boards (PCBs). Major testing equipments include signal
generators, power supplies and logic analyzer. Agilent
33120A was used to generate high performance system
clock signal. Firstly, when the start signal is active, the
digital circuits will start to generate control signals and
DATAREADY signal. Thus, by observing the DATA-
READY signal, it can be initially checked if digital circuits
are operated as expected. Secondly, the sine wave is gen-
erated by an ultra-low distortion function generator DS360,
which can provide better than -100 dB distortion over the
audio frequency range, and no filter was used. The sine
input voltage is sampled and converted into 12-bit digital
codes by the proposed data converter. The output codes of
D0 to D11 were captured by Logic Analyzer, and then
transferred to a PC to obtain the ENOB, SNDR and SFDR
using matlab. Table 1 lists all the details of all the equip-
ments used during the SAR ADC testing.
4.2 Dynamic performance
The dynamic performance test of the prototype SAR ADC
was conducted using a full-swing, differential sinusoidal
input with amplitude of 1.2 V. To test the 10-bit mode
Cal
ibra
tion
DA
C
MA
IN-D
AC
Com
para
tor
Con
trol
ler
Sub
-DA
C
1772 m1565
m
Fig. 9 Micrograph of entire ADC prototype
Table 1 List of test equipments
Function Equipment name
CLK generator Agilent 33120A
Vin generator Standford Research Systems DS360
Power supplies Agilent E3631A
Logic analyzer Agilent 16823A
Evaluation software Matlab
PCB board Custom design
248 Analog Integr Circ Sig Process (2013) 74:239–254
123
linearity, no calibration is performed. In 10-bit mode, Fig. 10
shows the SNDR and SFDR variations of this ADC with
respect to the input frequency. With the input frequencies
increased to the Nyquist frequency, the SNDR and SFDR
maintain over 60.92 and 76.36 dB at 100 kS/s; the SNDR
and SFDR maintain over 60.97 and 76.18 dB at 200 kS/s. A
fast Fourier transform (FFT) of the ADC at Nyquist opera-
tion in 10-bit mode is shown in Fig. 11(a) (fs = 100 kS/s)
and Fig. 11(b) (fs = 200 kS/s). The ADC achieves a
Nyquist SNDR of 61.11dB (9.86 ENOB) and an SFDR
of 77.8 dB when it samples at 100 kS/s, and achieves a
Nyquist SNDR of 60.99 dB (9.84 ENOB) and an SFDR
of 76.18 dB when it samples at 200 kS/s.
In 12-bit mode, Fig. 12 presents the dynamic perfor-
mance versus the input frequency measured with a 2.4-Vpp
input. Solid and dashed curves represent the measured
SNDR and SFDR before and after calibration respectively.
In the left figure, the SAR ADC was measured at 100 kS/s,
with a 39.83-kHz input, the peak SNDR and SFDR are
68.92 dB (11.16 ENOB) and 90.64 dB, respectively. In the
right figure, the SAR ADC was measured at 200 kS/s, with
a 18.78-kHz input, the peak SNDR and SFDR are 68.96 dB
(11.16 ENOB) and 89.05 dB, respectively, the SFDR drops
by 4.93 dB with an ENOB loss of 0.1-bit at the Nyquist
frequency (99.78 kHz) with respect to its low frequency
value, this distortion is due to the nonlinearity of the input
switch resistance, the loss of SNDR is likely due to noise
from the substrate and references.
FFT of the ADC at Nyquist operation in 12-bit 100 kS/s
mode is shown in Fig. 13. Before calibration, odd-order
0 10 20 4030 5060
65
70
75
80
Input Frequency(kHz)
(a)
dB
SNDR
SFDR
0 20 10040 60 8060
65
70
75
80
Input Frequency(kHz)
(b)
dB
SNDR
SFDR
Fig. 10 Measured SNDR and
SFDR versus the input
frequency in 10 bit mode
a at fs = 100 kS/s
b at fs = 200 kS/s
0 20 4010 30 50−120
−100
−80
−60
−40
−20
0
Input Frequency(kHz)
(a)
dB
0 20 10040 60 80−120
−100
−80
−60
−40
−20
0
Input Frequency(kHz)
(b)
dB
Fin=99.78kHz@200kS/sSNDR=60.99dBSFDR=76.18dBENOB=9.84
Fin=49.83kHz@100kS/sSNDR=61.11dBSFDR=77.8dBENOB=9.86
Fig. 11 FFT of ADC in 10 bit
mode with Nyquist input tone
a at fs = 100 kS/s
b at fs = 200 kS/s
0 10 20 30 40 5060
65
70
75
80
85
90
Input Frequency(kHz)
(a)
dB
0 20 10040 60 8065
70
75
80
85
90
Input Frequency(kHz)
(b)dB
SNDR(CAL OFF)SFDR(CAL OFF)SNDR(CAL ON)SFDR(CAL ON)
SNDR(CAL OFF)SFDR(CAL OFF)SNDR(CAL ON)SFDR(CAL ON)
Fig. 12 Measured SNDR and
SFDR versus the input
frequency in 12 bit mode before
and after calibration
a at fs = 100 kS/s
b at fs = 200 kS/s
Analog Integr Circ Sig Process (2013) 74:239–254 249
123
0 10 4020 30 50−120
−100
−80
−60
−40
−20
0Before Calibration
Input Frequency(kHz)dB
0 20 4010 30 50−120
−100
−80
−60
−40
−20
0After Calibration
Input Frequency(kHz)
dB
Fin=49.83kHz@100kS/sSNDR=68.74dBSFDR=90.36dBENOB=11.13
Fin=49.83kHz@100kS/sSNDR=67.2dBSFDR=77.83dBENOB=10.87
Fig. 13 FFT of ADC in 12 bit
mode with 49.83 kHz input tone
before (left) and after (right)calibration
0 200 1000400 600 800−0.2
−0.1
0
0.1
0.2
CODE
LSB
DNL
0 200 1000400 600 800−0.2
0
0.2
0.4
0.6
CODELS
B
INLFig. 14 Measured DNL and
INL in 10 bit mode at 100 kS/s
0 1000 2000 3000 4000−1
−0.5
0
0.5
CODE
LSB
DNL
0 1000 2000 3000 4000−1
−0.5
0
0.5
1
1.5
CODE
LSB
INLFig. 15 Measured DNL and
INL in 12 bit mode before
calibration at 100 kS/s
0 1000 2000 3000 4000−0.4
−0.2
0
0.2
0.4
CODE
LSB
DNL
0 1000 2000 3000 4000−0.5
0
0.5
CODE
LSB
INLFig. 16 Measured DNL and
INL in 12 bit mode after
calibration at 100 kS/s
250 Analog Integr Circ Sig Process (2013) 74:239–254
123
harmonics are clearly visible, the distortion is due to the
capacitor mismatch. The calibration provides around 2-dB
SNDR improvement and almost 13-dB SFDR improvement.
The ADC achieves a Nyquist SNDR of 68.74 dB (11.13
ENOB) and an SFDR of 90.36 dB when it samples at 100 kS/s.
4.3 Static linearity
To test the static linearity, code density test was conducted
using a full-swing, differential sinusoidal input with input
frequency of 288.78 Hz. Figure 14 shows the differential
nonlinearity (DNL) and integral nonlinearity (INL) with
respect to the output code in 10-bit mode. The maximum
DNL is ?0.054 LSB/-0.19 LSB, maximum INL is ? 0.33
LSB/-0.18 LSB at 100 kS/s, while the maximum DNL is
?0.066 LSB/-0.21 LSB, maximum INL is ? 0.32 LSB/
-0.15 LSB at 200 kS/s. In 12-bit mode, without calibra-
tion, the INL plot shows that the INL has a jump at the
middle of output codes, the MSB capacitance might be
responsible for this inference due to technology limitations.
As shown in Fig. 15 and Fig. 16, the calibration improves
the DNL from ?0.2/-0.74 LSB to ?0.23/-0.25 LSB and
INL from ?1.27/-0.97 LSB to ?0.41/-0.4 LSB at
100 kS/s. At 200 kS/s, the calibration improves the DNL
from ?0.25/-0.72 LSB to ?0.23/-0.25 LSB and INL
from ?1.31/-0.81 LSB to ?0.36/-0.43 LSB.
Table 2 ADC performance
summary
[22] FOMa ¼ Power2ENOB�fs
[3] FOMb ¼ Power10SNDR=20�fs
[3] FOMc ¼ Power10SFDR=20�fs
Process 0.18 lm
Area 1565 9 1772 lm
Voltage supply (V) 1.8
Input range (V) 2.4-Vpp
10 Bit mode 12 Bit mode
Sampling Rate 100 kS/s 200 kS/s 100 kS/s 200 kS/s
SNDR (dB) (at Nyquist) 61.11 60.99 68.74 68.4
ENOB (at Nyquist) 9.86 9.84 11.13 11.07
SFDR (dB) (at Nyquist) 77.8 76.18 90.36 84.11
DNL (LSB) ?0.054/-0.19 ?0.066/-0.21 ?0.23/-0.25 ?0.23/-0.25
INL (LSB) ?0.33/-0.18 ?0.32/-0.15 ?0.41/-0.4 ?0.36/-0.43
Power (lW) 498.6 826.2 579.6 946.8
FOMa (pJ/step) 5.3 4.5 2.59 2.2
FOMb (pJ/step) 4.39 3.69 2.12 1.8
FOMc (pJ/step) 0.64 0.64 0.176 0.295
Table 3 Comparison of performance on several ADCs
This work JSSC [22] IJCTA [6] ISSCC [30] ISSCC [2] JSSC [2] ADI [1]
datasheet
ZMDI [33]
datasheet
Bits 12 12 12 12 12 12 12 12
Process (nm) 180 130 250 45 180 180 – –
MS/s 0.1 22.5 0.05 0.5 0.1 0.1 0.1 0.2
DNL/INL 0.25/0.41 – 1/1.945 1.5/1.4 0.5/0.7 0.66/0.68 0.95/1 1/1
SFDR 90.36 90.3 – 82 71.8 71 83 80
ENOB 11.13 11.35 11.01 11 9.4 10.55 11.5 11
FOMa(pJ/step) 2.59 0.051 14.69 0.78 0.056 0.165 10.36 8.79
FOMb(pJ/step) 2.12 0.0417 11.99 0.64 0.046 0.136 8.46 7.17
FOMc(pJ/step) 0.176 0.004 – 0.13 0.01 0.07 2.12 1.8
[22] FOMa ¼ Power2ENOB�fs
[3] FOMb ¼ Power10SNDR=20�fs
[3] FOMc ¼ Power10SFDR=20�fs
Analog Integr Circ Sig Process (2013) 74:239–254 251
123
Table 2 summarizes the experimental results of the pro-
totype chip. Recently published and commercialized CMOS
ADCs with 12 bit resolution are compared with the proposed
ADC in Table 3. The presented ADC achieves the best
SFDR among all the works in Table 3. With on-chip cali-
bration, it achieves a Nyquist 90.36-dB SFDR when it
samples at 100 kS/s. The ADC presented in [22] also
achieves an SFDR of 90.3-dB, however, all calibration cir-
cuits in [22] are realized by using off-chip software rather
than on-chip implementation. The commercialized CMOS
ADCs dissipate more power consumption than other works is
mainly due to the fact that the power supply for commer-
cialized CMOS ADCs is always larger than 2.5 V. The
presented ADC shows smaller power consumption but
higher performance than the work in [6]. Also, the proposed
ADC shows comparable FOM3 to that of ADC presented in
[30]. Wang et al. [30] adopts the most advanced technology
among all the works in Table 3, and it shows better FOM1
and FOM2 than our work. The works such as [2] and [28] are
more efficient. This is mainly due to the fact that no cali-
bration is applied to the ADCs in [2] and [28], so the SFDR in
both works is non-ideal, about 71-dB. Also, ENOB in [2] or
[28] is smaller than all the other works presented in Table 3.
5 Conclusions
This work proposes a 10 or 12 bit programmable SAR ADC
for sensor interface applications such as bridge stress mon-
itoring systems. Tri-level based switching approach used in
the improved capacitor–resistor network saves capacitor
area by half and simplifies the control logic circuits. The
proposed novel digital time-domain comparator with no
static power consumption can be applied to both single-
ended and differential SAR ADC. The digital time-domain
comparator has obviated the only analog part of SAR ADC.
Since scaling of CMOS device dimensions offers clear
advantages for digital circuitry in terms of density, speed,
and integration, it is advantageous to move the whole SAR
operation into digital domain. The Digital calibration cancels
the offset of time-domain comparator and improves ADC
linearity, which is affected by different parasitic capaci-
tances between capacitors and neighboring signal lines. The
calibration scheme is implemented on-chip without com-
plicated post-processing, which is important for SOC
applications. In 12-bit mode, the SAR ADC achieves a
remarkable Nyquist SFDR of 90.36 dB and 11.13 ENOB at
100 kS/s after calibration. Using a 1.8-V supply voltage, the
achieved power consumption is 579.6 lW.
As a continuation of the work presented in this paper,
the priority of the future improvement is to design a more
efficient SAR ADC with a lower supply voltage. Since
lowering the supply voltage is the most effective way to
reduce power consumption assuming that the signal power
is proportional to VDD2. Then the low voltage time-domain
comparator needs to be further developed to achieve higher
accuracy and lower complexity. We have already done
some research and made some progress on low voltage
time-mode SAR ADC. For example, a 0.8 V ultra low
power SAR ADC has been proposed [14]. In addition,
discharge currents of C1 and C2 can be terminated as soon
as the comparison result is available [13] to obtain further
energy reductions. On the other hand, the simple back-
to-back NAND SR-latch in Fig. 5(b) suffers from asym-
metrical delays between rising and falling edges, this latch
can be further replaced by a more symmetrical and faster
one presented in [26]. Therefore, the plan for the next step
is to introduce these verified low power technique into our
design. Finally, considering longer term plan for higher
speed and resolution, the SAR ADC with multistage
pipelined architecture is attractive because of the area and
power efficiency [16, 10]. To the best of our knowledge,
pipelined SAR ADC previously published are all based on
voltage mode. If possible, we hope that we can introduce
low power time-mode technique to the pipelined SAR
ADC to obtain further energy reductions.
Acknowledgements This work was supported by the Ph.D. pro-
grams foundation of ministry of education of China (No.
20111011315), and the National Science and Technology Important
Project of China (No. 2010ZX03006-003-01)
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Fan Hua was born in Ziyang,
Sichuan Province, P.R. China,
on December 31, 1981. She
received the B.S. degree in
communications engineering
and the M.S. degree in Com-
puter science and technology,
both from Southwest Jiaotong
University, Chengdu, China, in
2003 and 2006, respectively.
Now she is a Ph.D. student of
Huazhong Yang in NICS labo-
ratory at department of Elec-
tronic Engineering of Tsinghua
University, Beijing, China. Her
research interests include low-power, high-resolution A/D converter
designs.
Han Xue was born in Baicheng,
Jilin Province, P.R. China, on
April 19, 1988. She received
B.S. degree at Beijing Jiaotong
University in 2010. Now she is a
Ph.D. student of Huazhong
Yang and Hui Wang in NICS
laboratory at Department of
Electronic Engineering of
Tsinghua University, Beijing,
China. Her current research is
the realization and application
of high-speed SAR ADC,
focusing on asynchronous cir-
cuit and time interleaving
technique.
Analog Integr Circ Sig Process (2013) 74:239–254 253
123
Wei Qi was born in Ningxia
province, in 1983. He received
the B.S. degree in electrical
engineering, from Northwestern
Polytechnical University, XiAn,
in 2005. He received the Ph.D.
degree from Tsinghua Univer-
sity, Beijing, in 2010. He is
currently a postdoctor in
Department of Electronic Engi-
neering of Tsinghua University.
His research interests focus on
analog IC design and high
performance data convert,
including high performance
operational amplifier, Pipeline ADC, SAR ADC, and current steer
DAC.
Yang Huazhong was born in
Ziyang, Sichuan Province,
P. R. China, on August 18, 1967.
He received B.S. degree in
micro-electronics in 1989, M.S.
and Ph.D. degree in electronic
engineering in 1993 and 1998,
respectively, all from Tsinghua
University, Beijing. In 1993, he
joined the Department of Elec-
tronic Engineering, Tsinghua
University, Beijing, where he has
been a Full Professor since 1998.
Dr. Yang was recognized as 2000
National Palmary Young
Researcher by NSFC. His research interests include chip.
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