# EMI Susceptibility Issue in Analog Front-End for Sensor Applications

Authors: Anna Richelli
Journal: Journal of Sensors
 (2016)

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## Abstract

The susceptibility to electromagnetic interferences of the analog circuits used in the sensor readout front-end is discussed. Analog circuits still play indeed a crucial role in sensor signal acquisition due to the analog nature of sensory signals. The effect of electromagnetic interferences has been simulated and measured in many commercial and integrated analog circuits; the main cause of the electromagnetic susceptibility is investigated and the guidelines to design high EMI immunity circuits are provided.


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## Body

## 1. Introduction

Current trends in consumer electronics highlight an increased interest in ubiquitous electronic devices. This is especially true in the field of sensors which can enable a variety of applications including interactive environments for medicine [1–5], military target tracking, automotive [6, 7], and environmental monitoring networks [8, 9]. Analog circuits still play a crucial role in sensor signal acquisition due to the analog nature of sensory signal: they are indeed widely used in the sensor readout front-end, since it directly interfaces the sensor [10–12]. Analog circuits are indeed employed for signal conditioning and conversion, generation of bias and reference voltages and currents, and systems interfacing.In recent years, integrated sensor systems have become widely commercially available. These systems usually contain microsensor array and sensor electronics [13–15]. When the sensor integration is not feasible due to economical or technical reasons, off-chip sensors may also be used. Nevertheless, the common feature is that the sensor electronics, sensor signal conditioning, processing, and conversion, generation of necessary bias, and reference voltages as well as currents, control, clock signals, and sensor system interface are located on a single chip or a chip set.In the literature, much attention is paid to many aspects, such as the resolution of a sensor system. The final limit of the resolution is represented by the sensor-input referred noise. This noise may contain contributions of the sensor itself and of sensor electronics and therefore a lot of attention has been paid in noise reduction techniques to improve the sensor resolution.Another important issue is that the noise can be generated by neighboring circuits and enter the system due to crosstalk, which can be either capacitive (due to stray capacitances) or conductive and inductive, through the power supply rails.In the literature the effect of the noise and the crosstalk have been widely investigated and many noise reduction techniques and guidelines are depicted and provided [16].However, when several analog and digital subsystems are required to coexist on the same chip, eventually sharing the same power sources, as in the sensor applications, another issue is becoming more and more important: the immunity to electromagnetic interferences (EMIs). As an example of this scenario, in Figure1 a schematic view of a pressure sensor, with highlighted analog and digital blocks, is shown.Figure 1
Example of a sensor circuit, with highlighted analog and digital blocks, eventually sharing the same chip and power supplies.In such a system, EMI may arise from external circuits and from subsystems integrated on the same die, spreading through the supply lines and the I/O interconnections.In the sensor design the influence of EMI is generally not treated explicitly or even neglected.This paper describes the effect of the electromagnetic interferences in analog circuits, widely used in the sensor interface: general-purpose operational amplifiers and voltage references. Measurement results of the EMI susceptibility in commercial devices are provided and the state-of-the-art design of high EMI immunity amplifiers and voltage references is depicted. In particular, in Section2, the problem of electromagnetic interferences will be briefly introduced and the results of measurements performed on several commercial amplifiers victims of EMI will be provided; in Section 3, the design of high-immunity amplifiers will be depicted and in Section 4 the guidelines to design high EMI immunity voltage references will be provided and finally conclusions will be drawn.


## 2. The Problem of Electromagnetic Interferences in the Analog Circuits

Electromagnetic interference (EMI) effects may arise from a wide class of sources (cellular telephones, CD players, laptop computers, etc.): as an example, aircraft may be susceptible to electronic interferences because of their reliance on radio communication and navigation systems whose electromagnetic spectrum ranges from 10 kHz (navigation systems) to above 9 GHz (weather radar). Furthermore, the massive introduction of electronics in automotive may cause a number of problems: cellular telephone transmitters, for instance, can induce disturbances in braking systems (ABS). EMI may arise from inside the automobile as well: alternators, ignition systems, switching solenoids, and electric starters are potential sources of such disturbances. Furthermore, due to the high density of components packed on printed circuit boards as well as the increasing speed of mixed analog/digital circuits, IC designers have to consider EMI during design phase. Neglecting these aspects may lead to failures on integrated circuits induced by spurious signals, including EMI at frequencies outside the working bandwidth of the circuit. Two different interferences should be considered, depending on the way they reach the circuits: the distributed ones and the conveyed ones. However, considering the chip size and the frequencies, the most important are the conveyed ones.In recent years, the effects of the conveyed EMI were carefully investigated both theoretically and experimentally in order to find possible prevention methodologies [17–25], in particular, in high-performance digital/analog ICs that may include several operational amplifiers. The most sensitive circuits to EMI are, indeed, the analog ones and, among them, the OpAmps.In order to investigate the EMI effects on a generic amplifier, the interfering signals are often represented by a sinusoidal waveform generated with zero DC mean value superimposed on the pins connected to long wires (long wires, indeed, act as antennas for EMI) [18, 20]. The amplifier is in the voltage follower configuration, as reported in the literature [21–23] and shown in Figure 2, since it is the worst case condition, because the input differential pair experience the largest disturbance. One of the most undesirable effects of interferences is the shift of the output DC mean value (offset) that may asymptotically force the amplifier to saturation [23–25]. Furthermore, among all the possible interfering signals the ones superimposed on the input pins of the operational amplifier are the most difficult to prevent [24, 25]. This is due to the fact that the adoption of external filters may modify the original input signals which are often very weak. As far as the power pins are concerned, easy filtering can prevent the dangerous DC offset from being formed.Figure 2
Effect of EMI conveyed into the input pin of an operational amplifier in voltage follower configuration.The maximum measured EMI induced voltage offset of some commonly used commercial amplifiers is listed in Table1: all the amplifiers were connected in a voltage follower configuration and the interfering sinusoidal signal, applied to the noninverting input pin, had an amplitude of 1 V at a frequency ranging from 100 kHz up to 1 GHz. The power supply was set to 12 V. Several samples of the most widely used technologies are listed: bipolar, jfet, and CMOS. The amplifiers were measured on a simple PCB following the schematic illustrated in Figure 3. A 33120A Hewlett-Packard RF function generator has been used with 50 Ω matching load to generate the EMI; the power supply and the biasing voltages were supplied by E3630A Hewlett-Packard power supply. The board interconnections were designed as short as possible along with straight paths and ground shields, in order to minimize all the undesired signals arising from the measurement setup itself. The resistor R1 in Figure 3 is used for the matching load, while C1 and C2 are power supply filters of, respectively, 100 nF and 10 μF; furthermore, the output pin is connected to an RC (R2=1 kΩ, C3=1 nF) filter with cut-off frequency of 160 kHz in order to evaluate the mean voltage that easily and accurately quantifies the DC shift due to EMI effects. Clearly, the measured offset voltage is significant and can cause failures (due to debiasing) in the circuits connected to the OpAmps. Finally, to have an easy view of the EMI effect in some commercial amplifiers, the induced offset in mV is plotted in Figure 4.Table 1
Measured EMI induced offset in commercial amplifiers.
Amplifier
Technology
Voltage offset
Critical frequencies
UA741
BJT
650 mV
0.1 MHz–3 GHz
AD705
BJT
350 mV
0.3 MHz–1 GHz
NE5534
BJT
360 mV
3 MHz–0.6 GHz
OPA177
BJT
360 mV
0.6 MHz–0.1 GHz
OP176
JFET In/BJT Out
200 mV
3 MHz–1 GHz
MC33181
JFET In/BJT Out
210 mV
6 MHz–0.6 GHz
CA3140
CMOS In/BJT Out
350 mV
0.1 MHz–1 GHz
ICL7611
CMOS
380 mV
0.3 MHz–0.3 GHzFigure 3
Schematic of the PCB used to characterize the EMI susceptibility of several commercial amplifiers.Figure 4
Measured EMI induced offset in uA741, CA3140, and ICL7611.


## 3. The Design of High EMI Immunity OpAmps

As stated above, among all the possible interfering signals the ones superimposed on the input pins are the most difficult to prevent.When electromagnetic interference is injected in the input pins of an operational amplifier, the latter generates an EMI induced offset voltage because of the nonlinear distortion taking place in the input differential pair [20].This behavior is correlated to the slew rate asymmetry and to the unequal parasitic capacitances which play a significant role, respectively, at low-medium frequencies and at high frequencies, outside the working bandwidth [20, 24, 25].Recently, some solutions have been proposed to intrinsically improve the immunity of the amplifiers to EMI signals arising from the input pins. For example, in [26] the design of an input stage is reported, based on a double cross-connected differential pair along with a simple high-pass filter, as shown in Figure 5. The cross-connected differential pair becomes active only in the passband of the RC high-pass filter. More recently, in [27], a comparison between the architecture proposed in [26] and a simple differential pair with an RC low-pass filter, as the one in Figure 6, has been illustrated.Figure 5
The high EMI immunity cross-coupled differential pair with high-pass filter proposed in [26].Figure 6
A simple RC filter on the input differential pair, as the one discussed in [27].However, as stated above, a filter may modify the response of the amplifier and, thus, it can just operate at out-of-band frequencies, while the EMI effects are relevant also at low-medium frequencies.Another solution has been proposed in [28], based on a double differential pair: in this architecture the nominal differential pair is bootstrapped using bulk biasing: the use of a bootstrapped differential pair results in an advantageous effect of the parasitic capacitances presented at the common source of the differential pair. In the design example shown in [28], the bootstrapped differential pair exhibits an EMI immunity two orders of magnitude larger than the classic differential pair. Nevertheless, following this approach, only a P-type differential input stage can be fabricated in a standard CMOS technology: the N-type stage requires, indeed, a triple-well technology due to the bulk biasing.EMI resistant differential pairs are proposed in other recent works as well [29, 30]; among them a simple and interesting approach to enhance the EMI immunity is based on an RC filter connected to an auxiliary differential pair, as proposed in [31–33]. The RC filter on the auxiliary differential pair introduces indeed a pole-zero doublet and allows for a larger GBW product and a better phase margin, compared to the RC filter connected to the main differential pair, still showing an improved EMI immunity.Another successful approach to intrinsically reduce the EMI effects, without adding any kind of filter, is presented in [34] and is based on the design of strongly symmetrical topologies. The symmetrical topology proposed in [34] is based on two identical fully differential source cross-coupled amplifiers, combined in cascade connection in order to achieve a large gain. The circuital scheme is shown in Figure 7. This topology is very useful when the output slew rate of the OpAmp is an important task; moreover, such a scheme leads to a strong symmetry of the output voltage thanks to the mirrored path of the signals. Indeed, as shown in Figure 7, the input voltages are applied to the gates of both M2a and M2b, in order to bias the NMOS differential pair, and to the gates of M1a and M1b to bias the PMOS differential pair.Figure 7
Highly symmetrical fully differential source cross-coupled amplifier proposed in [34].NMOS and PMOS differential pairs are connected with cross-coupled sources. Hence, the input voltages are symmetrically applied to the gates of the 2nd differential pairs M3 and M4.Thus, any voltage mismatch, due to stray elements and nonidealities, is removed by this cross-connection. This leads to a very symmetrical path for both signals across the amplifier and to an EMI immunity more than 2 orders of magnitude increased, as clearly demonstrated by the plot in Figure8 where the EMI induced offset is compared to that of the uA741.Figure 8
Measured EMI induced offset: a comparison between the uA741 and the amplifier proposed in [34], in the case of 1Vp EMI signal.The architecture proposed in [34] is unfortunately not suited for the ultralow voltage supply of current integrated circuits. This is mainly due to the complex cascode connections.Therefore, an alternative solution is proposed derived from the Miller amplifier [35]. The overall schematic is shown in Figure 9.Figure 9
Highly symmetrical fully differential amplifier for low voltage supply proposed in [35].Finally, a circuit that enhances the EMI immunity of amplifiers by deleting the common mode signals has been recently proposed. The EMI induced voltage generated at the output of the input stageVos is indeed due to the differential and the common mode signals Vdm and Vcm, as calculated in the following mathematical expression:(1)Vos=∫-∞∞Hcmjω·Vcmjω·Vdmjω·cos⁡ϕ·dωVGS1,2-Vt.In a differential amplifier, the differential signals cannot of course be removed, but the common mode components can be deleted. The schematic of the common mode cancellation circuit proposed in [36] is shown in Figure 10. If the circuit is properly sized (by choosing the right value of the resistors) the common mode signals are cancelled while the differential signals are doubled.Figure 10
The common mode cancellation circuit proposed in [36]: it is used as input stage, to increase the EMI immunity in a Miller differential amplifier.Consequently, the resulting EMI susceptibility is reduced, as plotted in Figure11, where the offset is compared between the original amplifier and the one modified by including the common mode cancellation stage.Figure 11
Simulated EMI induced offset: comparison between the original Miller differential amplifier and the one modified by adding the common mode cancellation stage depicted in [36].


## 4. Design of High EMI Immunity Voltage Reference

It is well established that analog CMOS circuit design relies on close geometry matching of components which yields precise ratios of component values. As this applies only to a lateral geometry defined within the same mask, only related components (i.e., components of the same nature, so to speak) can be well matched. On the contrary, the definition of absolute values and tolerances is rather poor, as it depends on various material properties and technology processing steps. Nevertheless, absolute reference values are often needed. The on-chip reference generation is usually confined to voltage reference generation using the bandgap principle, which utilizes parasitic pnp-bipolar transistors of a CMOS process for this purpose.It is worth adding that, in the literature, much attention is paid to many quality aspects, such as the mean relative temperature dependency and the accuracy, but the influence of electromagnetic interferences is only recently treated explicitly.In order to reach a clear comprehension of the EMI on a bandgap reference circuit, it should be pointed out that in many applications analog and digital subsystems are required to coexist on the same chip, sharing the same power sources. In such a system, electromagnetic interferences may arise from external circuits and from subsystems integrated on the same die, spreading through the supply lines leading to large unexpected fluctuations of the power supply, as illustrated in Figure12.Figure 12
Scenario of EMI pollution in electronic circuits.In order to investigate the EMI effects on bandgap references, the interferences are modelled by means of spurious signals applied to the power pins. As already stated, EMIs are represented by means of undamped sinusoidal waveforms that allow for an easy measurement in laboratory.Among the various voltage reference architectures, the most popular circuit is the bandgap reference based on pn junctions, OpAmp, and ratioed resistors [37]. On the other hand, in order to meet the important constraints of low power supply voltage and low power dissipation, it is desirable to use simple architectures, avoiding operational amplifiers and additional circuits. Therefore, many different bandgap architectures were also designed [38].The first considered reference is the “Brokaw” circuit, shown in Figure13 [37]: an improved version, widely used in recent ICs, is often called “Kuijk bandgap” [39] and it is based on ratioed resistors and OpAmp, along with the parasitic bipolar pnp transistors provided by the CMOS technology.Figure 13
The “Brokaw” voltage reference circuit.For Brokaw and Kuijk bandgap circuits, a few topologies can be found in the literature [40–44], showing a low EMI susceptibility. Here, the basic topology is often improved by enhancing the EMI immunity of the operational amplifier, following the approaches depicted in Section 3, by changing the bandgap bias current and by introducing filter capacitors. Layout and technological techniques to reduce the coupling between the power supply net and the poly resistors are also useful to increase the immunity to electromagnetic interferences [40].In Figure14 an example of a high EMI immunity bandgap voltage reference is shown, based on the solution proposed in [44].Figure 14
Schematic of the EMI-improved “Kuijk” bandgap proposed in [44].As investigated in [44], the original CMOS voltage reference, designed in AMS CXQ 0.8 μm process, was very susceptible to the 1Vp interferences arising from the power supply rails, showing a large offset as plotted in Figure 15. To reduce its susceptibility a fully differential folded cascode amplifier with high EMI immunity has been used instead of the single ended Miller amplifier and two capacitors were added on the most critical nodes. The simulated offset of the modified “Kuijk” bandgap is shown in Figure 16. The CMOS voltage reference has been fabricated in the AMS CXQ 0.8 μm process and the test chip was measured, exhibiting a high level of EMI immunity as demonstrated by the measurement results plotted in Figure 17: the offset is indeed several orders of magnitude reduced.Figure 15
Offset of the bandgap voltage references caused by1Vp EMI signal superimposed to the power supply rails.Figure 16
Offset of the bandgap circuit modified by using a fully differential amplifier and two capacitors, as shown in the schematic of Figure14.Figure 17
Measured EMI induced offset of the high-immunity bandgap proposed in [44].The second considered bandgap topology uses ratioed transistors biased in strong inversion along with the inverse-function technique to produce temperature-insensitive voltage references [45]. With regard to this bandgap topology, analysis and simulations emphasized that the differential pairs (M1-M2 and M3-M4) play a significant role in EMI susceptibility. Hence, in order to improve the immunity to interferences, M1-M2 and M3-M4 are created in insulated wells and a small capacitor (1 pF) is connected between Vs and ground. In Figure 18 the schematic of the bandgap circuit modified following this approach is shown. The simulations demonstrated the validity of this approach: considering 1Vp EMI signal superimposed to the supply rails, the maximum induced offset of the original circuit was more than 300 mV while the offset of the modified bandgap is less than 20 mV in the whole frequency range.Figure 18
OpAmp-less and resistorless bandgap circuit with enhanced EMI immunity, presented in [45].


## 5. Conclusions

In the frame of a higher attention towards the problem of electromagnetic susceptibility, the design of analog circuits widely used in the sensor systems is discussed. In particular, the effect of the electromagnetic interferences is briefly introduced in the most common analog amplifiers and voltage references. Several and recent solutions to increase the EMI immunity are presented: the resulting amplifiers and voltage references exhibit an EMI susceptibility reduced by 2 orders (or even more) of magnitude compared to the classical ones.



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