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1101700_V1_DS22_Functional_Description


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22bit Sigma-Delta ADC Theory and Circuit Operation

                               J. G. Pett

Introduction

A basic Sigma-Delta ADC is shown in Fig.1 and has an action essentially the same as a
Charge-Balance type. This is termed a 1st order modulator. Additional integrators can be
added between the first integrator and the comparator, where Fig.2 shows a 3rd order
modulator. The following sections explain firstly the basic theory of operation of a SD type
of ADC and then give a detailed description of the modulator circuit. The digital filter is
described in the final section.

Theoretical Concepts

Oversampling

Any ADC can be described as an electronic circuit that quantises a given input signal. This
means that the digital output has a number of output codes, each of which describes a
particular interval of the input signal. For a perfect ADC of n bits, each interval will be equal
to Vfsr/ 2n [Vfsr = the full-scale range of the input signal]. If a perfect transition from one
output code to the next occurs as the input signal increases, then it becomes possible to
interpolate between each interval using averaging techniques and hence improve the
resolution beyond that of the n bit ADC. Such methods are termed oversampling. [In
practise, the input signal must frequently traverse at least two adjacent intervals to ensure
correct averaging. This is assured for most cases by the signal noise, the ADC internal noise
or an externally applied "dither" signal, which sweeps the input over a narrow range of bit
intervals, or transitions.]

Normal averaging of 10 output values allows each interval to be divided by 10, effectively
increasing the resolution by more than 3bits, but this requires sampling the signal 10 times
faster to retain the same signal bandwidth. Alternatively, we can express this as reducing the
quantising "noise", or uncertainty. Averaging 100 values will improve the noise by 40dB and
so on. Oversampling by 500 will reduce the quantisation noise by 54dB, however this also
means that ADC bandwidth is traded against improved resolution.

Consider an example from the 22bit ADC. For a 1kHz bandwidth signal to digitise, we must
sample at 2kHz [Nyquist criteria]. If we now oversample at 1MHz to improve the resolution,
we will obtain approx. 9 extra bits of resolution and improve the signal to noise ratio by
54dB. [Note : the definition of oversampling ratio is fs/fNyquist.]

Noise Shaping

Provided that the input signal is not a stationary [DC] value, the above quantisation noise can
be described as 'white noise' with a bandwidth of fs/2.

The basic Sigma-Delta modulator is a form of charge-balance ADC having a 1bit quantiser
[the comparator] and a 1bit very-high-precision DAC. The quantisation noise is that coming
from the 1bit DAC and is large [N/S is approximately 0dB]. This noise is integrated by the
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first integrator and hence modifies the theoretical white noise spectrum, reducing it where the
integrator has internal gain i.e. below the gain = 1 point. This process is termed noise
shaping. In the 22bit case, if the integrator gain = 1 point is set at 25kHz then the noise
reduction is about 20dB/decade and at 1kHz is approx. = 28dB. Adding this to the above
54dB gives an overall N/S ratio of about -82dB. Therefore, with a single integrator filtering
the quantisation noise of a very simple 500x oversampling, 1bit ADC we can obtain a
resolution at 1kHz of about 1part in 12,000 or nearly 14bits. Extra stages filtering the
quantisation noise are possible and can improve the resolution by about 28dB for each
additional integrator. Again using the 22bit case we obtain 54 + (3x28) = 138dB or >22bits.

Noise shaping using filters in the forward path of the charge-balance circuit, along with a high
oversampling ratio, constitute the basic theoretical concepts on which Sigma-Delta ADCs
work.

Filtering

It remains to filter the wanted output data from the 1bit stream of data at 1MHz. This is done
using a low-pass digital filter, which essentially removes the quantisation noise above the
wanted band [DC to 1kHZ] while increasing the output word length. In order to suppress
noise above the signal pass-band, a low pass filter having approximately the same attenuation
rate as the noise shaping filter is required, to match the rising noise-shaped spectrum. This
ensures that all signals above the filter cut-off frequency are kept below the base-band noise
floor.

If the input signal spectrum contains components above fs /2, aliasing will occur. Therefore
an analog input filter must lower any such signals to below the ADC noise threshold. For
traditional sample rates just above the Nyquist rate such a filter becomes a major design
limitation. However, the SD ADC actually samples at say 500x Nyquist, which means that
adequate attenuation can be achieved with simple passive single or two pole filters. This is
particularly important for very high performance ADCs since input signal quality can be
maintained.

Functional Description of 22bit SD Circuit Diagram

Isolation and EMC

The whole of the modulator circuit is floating with respect to ground and is contained within a
guard box. This method assures a common-mode rejection ratio of greater than 150dB at
50Hz. To provide adequate EMI suppression, a capacitive coupling network is placed
between the input cable screen and ground, followed by two isolating hf chokes at the single-
ended buffer input. This protection has been shown to provide >2.5KV burst test immunity.

Input Buffer and Anti-Alias Filter

The high input impedance buffer amplifier IC16 is preceeded by a two-pole anti-alias filter
[break freq. = 5kHz] giving > 94dB attenuation at the sampling frequency of 1MHz. Any
input signals at 1MHz +/-1kHz should therefore be < 100mV [-40dB of 10V] to avoid
aliasing, and this will normally be easy to ensure.




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Integrators

The 1st summing integrator is IC10, which combines the input signal via a 70K and the 20K
resistors switched by IC8, which together constitute the 1bit precision DAC. Note that all
these resistors are Vishay precision types. In order to circumvent the recently discovered
offset instability of IC10 [Ti/BB 627], an additional chopper-stabilised amplifier ICXX [LTC
1250] has been applied, such that the combined amplifier pair now has both excellent DC
offset stability [<0.05ppm/degC] and high frequency performance. An additional and
important bonus is that the 1/f noise of the 627 has been suppressed, leading to improved
long-term stability.

The 2nd and 3rd integrator stages are constituted by IC15 A+B which are both configured as
non-inverting integrators. This design has two advantages. The first is that each circuit acts
as a unity-gain stopped-integrator above the gain 1 break frequency and the second is that if
saturation occurs due to excessive input signal, clamping can be achieved, [using analog
switches IC14], to give unity gain from input to output of the pair. Under such clamped
conditions the 3rd order configuration [basically unstable] reverts to the 'always stable' 1st
order form and hence continues to function "normally" until the overload is removed. Note
that the overload detection and clamp drive is described later.

Comparator and Dither Generator

The output of the 3rd integrator drives the comparator IC12, the output of which is clocked at
1MHz into IC7. [Note that IC7 decides the polarity of the 1bit DAC, thus closing the self-
oscillating loop.]

A triangular 960kHz "dither" signal is injected into the + ve input terminal of the comparator
for "idle-tone" suppression. The frequency generator is IC11 and P2 adjusts the output to 960
+/- 5 kHz. IC13A buffers this signal. P3 is set such that the pk-pk amplitude of the signal at
TP10 is approx. doubled. This effectively randomises the idle-tone spectrum.

Note - An 'idle-tone' is a part of the modulator output noise occurring at a particular
frequency, which falls within the required pass-band. Often a number of such tones can occur
together. They are particularly noticeable with DC inputs. They can exceed the pass-band
noise floor by up to 20dB and hence become problematic. Idle-tones decrease with increasing
order of the modulator. The above method of suppression has never been reported in earlier
literature.

Precision References

The basic precision-voltage-reference design is a modified "Spreadbury" circuit, using IC5
and IC6. IC6C provides internal temperature stabilisation of the LTZ1000A buried zener,
where R32 sets this temperature to approx. 35degC. Note that R33 is an initial set-up
component = 3.3K which allows the LTZ 1000A to 'burn in' for 15days at 105degC. After this
period R33 should be removed for normal operation. This 'burn-in' removes zener drift, which
would otherwise occur during the first year of operation. IC6D provides the feedback to T2,
which sources the zener. Note that the basic "Spreadbury" circuit is very sensitive to EMI and
that extra ceramic decoupling capacitors have been added to suppress these effects. The 7.1V
output at TP4 connects to an attenuator R70+R75 [2x20K] where the centre point of the 20K
pair is held at zero volts by IC6B. IC6A buffers approx. +5V to power IC8, thus providing
the precision positive voltage for the 1bit DAC. IC6B provides a permanent -5V to the
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combination R73, R74B. Note again the use of L3-5 and extra EMI suppression capacitors.
The output impedance at high frequency of the basic +5V reference is far too high and heavy
decoupling is necessary to prevent signal droop occurring during "shoot-through" operation of
the CMOS output pairs of IC8. Fortunately, the multi-layer ceramic capacitor C20, 2.2uF
solves this limitation. P4 provides the only fine adjustment of DAC output symmetry but as
such it is designed to incorporate all other circuit asymmetries and is not intended to balance
the actual +/-5V reference outputs.

Clock Source, Logic and 1bit DAC Switching

The basic clock source is derived from a 16MHz Xtal controlled oscillator Q1, which has
heavy supply-line decoupling to minimise clock "pulling" and phase jitter. This Xtal type
must not be replaced, as it is critical to obtaining the overall performance. The output of the
oscillator is buffered by IC2B and inverted by IC2A, thus allowing both edges of the signal to
be used. The 16MHz clock feeds an FPGA, IC3, which is programmed to divide this input to
provide the 1MHz clock for IC7 [pin 28]. At the same time a 62.5nsec 'guard pulse' is
generated [pin 9 of IC7B], overlapping the 1MHz edge, which serves to clamp the 1bit DAC
output to zero during basic clock transitions, and also ensuring precisely equal switching
surfaces in the 1bit DAC output irrespective of pulse sequencing.

IC7A latches the comparator value with the 1MHz clock and returns this value to the FPGA
[pin 31]. If the value is a +1 then a 250nsec pulse is output [pin 22] to the fibre Tx. A -1
outputs a 750nsec pulse. This allows the leading edge of these pulses to be use remotely for
re-generation of the 1MHz clock and a sampling of the state of the pulse at 500nsec allows
either a +1 or a -1 to be detected.

The FPGA detects if the modulator is in saturation by detecting more than 15 continuous
output pulses of the same sign. Should this occur, the FPGA outputs a 1



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