System for characterizing transistor circuits

Abstract

To provide a system for characterizing a transistor circuit having the minimum value in transmission characteristics by detecting the minimum value.SOLUTION: A system 100 includes: a bias voltage generator 120 generating a toggling signal; a multiplier 140 configured so as to multiply an electric signal as a function of a source / drain current of a transistor circuit 110 by a waveform alternating between two previously defined values in synchronization with a toggling signal; a first integrator that is a first integrator 130 configured so as to integrate an electric signal from the multiplier while linear combinations of output signals of an integrator are provided to further integrators when more integrators exist; and an adder 150 that is configured so as to add a toggling signal and an integral signal and is configured so as to output the sum to a gate of a transistor circuit.SELECTED DRAWING: Figure 5

Description

[Technical Field]

[0001] The present invention relates to the field of transistor circuits having transfer characteristics with local minima, and more particularly to a system for finding the local minima in the transfer characteristics of such transistor circuits. [Background technology]

[0002] Finding the local minimum of a transistor circuit having a transfer characteristic with a local minimum can be achieved by sweeping the gate-source voltage and measuring the source-drain current through the transistor circuit. This makes it possible to find the specific gate-source voltage at which the current is minimum. It would be advantageous if the time to find this specific voltage could be reduced.

[0003] An example of such a transistor circuit is a graphene FET, which has a local minimum at the Dirac voltage. US8638163B2 discloses a device and method in which a semiconductor device is used to generate a test voltage. The graphene transistor is configured to receive a gate-source voltage based on the test voltage, and a detector is configured to detect whether the gate-source voltage is the Dirac voltage of the graphene transistor. Thus, the detector detects whether the graphene transistor is turned off based on the drain-source voltage and / or drain-source current. It would also be advantageous in this case if the time required to find a particular voltage (in this case, the Dirac voltage) could be reduced.

[0004] Therefore, there is a need for an alternative system for determining the local minimum of a transistor circuit having a transfer characteristic with a local minimum. Summary of the Invention

[0005] It is an object of embodiments of the present invention to provide a system for determining local minima in a transistor circuit having a transfer characteristic with a local minima.

[0006] The above objects are achieved by a method and device according to the present invention.

[0007] SUMMARY OF THE INVENTION Embodiments of the present invention relate to a system for characterizing a transistor circuit.

[0008] The transistor circuit comprises a gate, a source, and a drain, and is configured such that the drain-source current to gate-source voltage transfer function has a local minimum for a particular voltage.

[0009] The system is configured to measure this particular voltage, a transistor circuit; -Generate a toggling signal to achieve a predefined bias voltage v around a given bias point G a bias voltage generator configured to toggle between positive and negative; one or more integrators; a multiplier configured to generate an electrical signal by multiplying an electrical signal that is a function of the drain-source current of a transistor circuit with a waveform that alternates between two predefined values ​​plus and minus A that alternate in synchronization with the toggling signal.

[0010] A first integrator of the one or more integrators is configured to integrate the electrical signal from the multiplier, and if more integrators are present, linear combinations of the integrator output signals are provided to further integrators.

[0011] The system further comprises an adder configured to add the toggling signal and the integrated signal, or a processed version thereof, where the integrated signal is obtained by linearly combining the outputs of one or more integrators, and configured to output the sum to a gate of the transistor circuit.

[0012] In an embodiment of the present invention, the transistor circuit comprises: a first transistor and a second transistor; a first voltage converter configured to convert a voltage at the gate of the transistor circuit or at the source of the transistor circuit into a gate-source voltage between the gate and source of the first transistor according to a transfer function having a first slope; a second voltage converter configured to convert the voltage at the gate of the transistor circuit or at the source of the transistor circuit into a gate-source voltage between the gate and source of a second transistor according to a transfer function having a second slope.

[0013] The first slope and the second slope have opposite signs.

[0014] When the first voltage converter is configured to convert the voltage at the source of the first transistor, the transistor circuit may further comprise a third voltage converter configured to apply a voltage to the drain of the first transistor so as to obtain a stable drain-source voltage for the first transistor.

[0015] When the second voltage converter is configured to convert the voltage at the source of the second transistor, the transistor circuit may further comprise a fourth voltage converter configured to apply a voltage to the drain of the second transistor so as to obtain a stable drain-source voltage for the second transistor.

[0016] In an embodiment of the present invention, the first transistor or the second transistor is exposable to and sensitive to a chemical component.

[0017] In an embodiment of the present invention, the first transistor and the second transistor are metal oxide semiconductor FETs or bipolar transistors.

[0018] In an embodiment of the present invention, the transistor circuit is a graphene FET.

[0019] In an embodiment of the present invention, the system comprises a sample and hold circuit for sampling and holding the integrated signal to obtain a processed version of the integrated signal.

[0020] In an embodiment of the present invention, the system comprises exactly one integrator.

[0021] In an embodiment of the present invention, the system comprises exactly two integrators, and the input signal of the second integrator is the sum of the output signal of the first integrator and the output signal of the second integrator multiplied by a predefined constant a1.

[0022] In an embodiment of the present invention, the predefined bias voltages are such that the sum obtained by the adder is within the quadratic region of the transistor circuit characteristic.

[0023] In an embodiment of the present invention, the predefined bias voltages are such that the sum obtained by the adder is in the linear region of the transistor circuit characteristic.

[0024] In an embodiment of the present invention, in the first stage, the predefined bias voltages may be such that the sum obtained by the adder is within the linear region of the transistor circuit characteristic, and in the second stage, the predefined bias voltages may be such that the sum obtained by the adder is within the quadratic region of the transistor circuit characteristic.

[0025] In an embodiment of the invention, the system comprises a quantizer configured to quantize the integrator signal at a predefined sampling frequency, and a digital-to-analog converter for converting the quantized signal to an analog signal for summing with the toggling signal in an adder.

[0026] In an embodiment of the present invention, the digital-to-analog converter toggles between a first predefined reference voltage for a digital zero input and a second predefined reference voltage for a digital one input, and the first and second reference voltages and the predefined bias voltage are selected such that toggling at the predefined bias voltages results in a voltage in the left-hand linear region and a voltage in the right-hand linear region of the transistor circuit.

[0027] In an embodiment of the present invention, the digital-to-analog converter toggles between a first predefined reference voltage for a digital zero input and a second predefined reference voltage for a digital one input. The first reference voltage and the predefined bias voltage are selected such that toggling at the predefined bias voltage results in a voltage at a left portion of a secondary region and a voltage at the same left portion of the secondary region. The second reference voltage and the predefined bias voltage are selected such that toggling at the predefined bias voltage results in a voltage at a right portion of the secondary region of the transistor circuit and a voltage at the same right portion of the secondary region.

[0028] In an embodiment of the present invention, the quantizer is a predefined number N q a multi-bit quantizer having N bits, and a digital-to-analog converter q It has bits.

[0029] Particular and preferred aspects of the invention are set out in the accompanying independent and dependent claims. Features from the dependent claims may be combined with features of the independent claims and with features of other dependent claims as appropriate and not merely as explicitly set out in the claims.

[0030] These and other aspects of the invention will be apparent from and elucidated with reference to the embodiments described hereinafter. [Brief explanation of the drawings]

[0031] [Figure 1]1 shows a schematic diagram of a transistor and a graph showing the drain-source current as a function of the gate voltage of the transistor. [Figure 2A] 1 shows a transistor circuit according to an embodiment of the present invention, comprising a voltage converter on the gate of the transistor. [Figure 2B] 1 shows a transistor circuit according to an embodiment of the present invention, comprising a voltage converter at the source of the transistor and optionally at the drain of the transistor. [Figure 3] GFET drain-source current versus gate voltage and its approximation. [Figure 4] 1 shows a schematic diagram of a device for integrating transistor circuit currents in a system according to an embodiment of the present invention; [Figure 5] 1 illustrates a basic primary measurement loop of a system for measuring a specific voltage of a transistor circuit, according to an embodiment of the present invention. [Figure 6] FIG. 1 shows a block diagram of a first-order linear system according to an embodiment of the present invention. [Figure 7] FIG. 1 shows a schematic diagram of a secondary system, according to an embodiment of the present invention. [Figure 8] FIG. 2 shows a block diagram of a secondary system according to an embodiment of the present invention. [Figure 9] 10 illustrates an output voltage of a system with large gain modulation of a second order system with a bandwidth of 70 Hz, in accordance with an embodiment of the present invention. [Figure 10] An enlarged version of Figure 9 is shown. [Figure 11] 9 shows the frequency response of the second-order system that was also used to obtain the simulation results in FIG. [Figure 12] 10 illustrates output voltage as a function of time for a system with small gain modulation for a second-order system with a bandwidth of 70 Hz, in accordance with an embodiment of the present invention. [Figure 13] An enlarged version of Figure 12 is shown. [Figure 14] 10 illustrates the frequency response of a system with large gain modulation of a second-order system with a bandwidth of 7 Hz, in accordance with an embodiment of the present invention. [Figure 15] 15 shows the output voltage of the system of FIG. [Figure 16] An enlarged version of Figure 15 is shown. [Figure 17] 1 shows a schematic diagram of an exemplary system for measuring a particular gate voltage that results in a minimum current in a transistor circuit, the system comprising a 1-bit quantizer and a digital-to-analog converter, in accordance with an embodiment of the present invention. [Figure 18] 1 illustrates a GFET characteristic and its linear approximation used by a system including a quantizer and a digital-to-analog converter, according to an embodiment of the present invention. [Figure 19] 10 illustrates the output of the decimation filter converted to a voltage for a system according to an embodiment of the present invention. [Figure 20] 19 shows a zoomed plot of the settling output of the decimation filter of FIG. [Figure 21] 20 shows a zoomed plot of the settling output of the decimation filter for a reference voltage closer to a particular voltage compared to the reference voltage used to obtain the plot of FIG. [Figure 22] 1 shows a schematic diagram of an exemplary system for measuring a specific voltage of a transistor circuit, the system comprising an Nq-bit quantizer and an Nq-bit digital-to-analog converter, according to an embodiment of the present invention. [Figure 23] 10 shows a plot of decimation filter output in function of sample number for a simulation illustrating the operation of a system with an Nq-bit quantizer and an Nq-bit digital-to-analog converter, in accordance with an embodiment of the present invention. [Figure 24] 23 shows a zoomed plot of the settling output of the decimation filter for the same simulation. [Figure 25] Figure 23 shows the 5-bit quantizer output as a function of the number of samples for the same simulation.

[0032] Any reference signs in the claims shall not be construed as limiting the scope. In different drawings, the same reference signs refer to the same or similar elements. DETAILED DESCRIPTION OF THE INVENTION

[0033] The present invention will be described with respect to particular embodiments and with reference to certain drawings but the invention is not limited thereto but only by the claims. The drawings described are schematic only and are non-limiting. In the drawings, the size of some of the elements may be exaggerated and not drawn to scale for purposes of illustration. The dimensions and relative dimensions do not correspond to actual reductions to practicing the invention.

[0034] Terms such as first, second, and the like in this specification and claims are used to distinguish between similar elements and not necessarily to describe an order, temporally, spatially, sequentially, or in any other manner. Terms so used are interchangeable under appropriate circumstances, and it is understood that embodiments of the invention described herein are capable of operating in orders other than those described or illustrated herein.

[0035] It should be noted that the term "comprising" used in the claims should not be interpreted as being limited to the means listed thereafter, nor does it exclude other elements or steps. Thus, it is interpreted as specifying the presence of stated features, integers, steps or referenced components, but does not exclude the presence or addition of one or more other features, integers, steps or components, or groups thereof. Thus, the scope of the expression "a device comprising means A and B" should not be limited to a device consisting of only components A and B. This means that, in the context of the present invention, the only relevant components of the device are A and B.

[0036] References throughout this specification to "one embodiment" or "an embodiment" mean that a particular feature, structure, or characteristic described in connection with an embodiment is included in at least one embodiment of the present invention. Thus, the appearances of the phrase "in one embodiment" or "in an embodiment" in various places throughout this specification do not necessarily all refer to the same embodiment, although they may. Furthermore, the particular features, structures, or characteristics may be combined in any suitable manner in one or more embodiments, as would be apparent to one of ordinary skill in the art from this disclosure.

[0037] Similarly, in describing exemplary embodiments of the invention, it should be understood that various features of the invention may be grouped together in a single embodiment, figure, or description for the purpose of streamlining the disclosure and aiding in understanding one or more of the various inventive aspects. This method of disclosure, however, is not to be interpreted as reflecting an intention that the claimed invention requires more features than are expressly recited in each claim. Rather, as the following claims reflect, inventive aspects lie in less than all features of a single foregoing disclosed embodiment. Thus, the claims following the detailed description are expressly incorporated into this detailed description, with each claim standing on its own as a separate embodiment of this invention.

[0038] Furthermore, some embodiments described herein may include some features included in other embodiments but may not include other features, and as will be understood by those skilled in the art, combinations of features from different embodiments are meant to be within the scope of the present invention and form different embodiments. For example, in the following claims, any of the claimed embodiments can be used in any combination.

[0039] In the description provided herein, numerous specific details are set forth. However, it will be understood that embodiments of the present invention may be practiced without these specific details. In other instances, well-known methods, structures, and techniques have not been shown in detail in order not to obscure an understanding of this description.

[0040] In embodiments of the present invention, when we refer to the quadratic region of a transistor circuit, we are referring to the region where the current versus gate characteristic can be approximated by a quadratic curve.

[0041] In embodiments of the present invention, when we refer to the linear region of a transistor circuit, we refer to the region where the current versus gate characteristics can be approximated by two linear functions.

[0042] An embodiment of the present invention relates to a system 100 for characterizing a transistor circuit having a gate, a source, and a drain. The transistor circuit is configured such that the drain-source current in function of a gate-source voltage transfer function has a local minimum value for a particular voltage. The system 100 is configured to measure the particular voltage.

[0043] Exemplary embodiments of such a system 100 are shown in FIGS.

[0044] A system according to an embodiment of the present invention comprises: a transistor circuit 110; -Generate a toggling signal to achieve a predefined bias voltage v around a given bias point G a bias voltage generator 120 configured to toggle between positive and negative; one or more integrators 130; a multiplier 140 configured to generate an electrical signal by multiplying an electrical signal that is a function of the drain-source current of the transistor circuit 110 with a waveform that alternates between two predefined values ​​plus and minus A that alternates in synchronization with the toggling signal, wherein a first integrator 130 of the one or more integrators 130 is configured to integrate the electrical signal from the multiplier 140, or if there are more integrators 130, a linear combination of the integrator output signals is provided to a further integrator 130; an adder 150 configured to add the toggling signal and the integrated signal, or a processed version thereof, where the integrated signal is obtained by linearly combining the outputs of one or more integrators 130 and is configured to output the sum as the gate-source voltage of a transistor circuit.

[0045] In embodiments of the present invention, the gate voltage or source voltage can be toggled to obtain a toggling of the gate-source voltage corresponding to the toggling signal. When toggling the source voltage, the drain voltage can be toggled simultaneously so that the drain-source voltage remains stable. Toggling the source voltage can be advantageous for common-gate operation. In such a configuration, the common gate of one or more transistor circuits can be maintained at a fixed potential, and a feedback voltage (i.e., the sum of the toggling signal and the integrated signal, or a processed version thereof) can be applied to the source. A version of the feedback voltage should then also be applied to the drain simultaneously so that a stable drain-source voltage is obtained. This is also advantageous for common-gate operation. When toggling the source voltage without toggling the drain voltage, instability in the drain-source voltage can be compensated for by post-processing to remove errors due to instability in the drain-source voltage.

[0046] It is an advantage of embodiments of the present invention that it is possible to derive from the integrated signal, or from a processed version of the integrated signal, specific voltages associated with local minima in the transfer function of the transistor circuit.

[0047] System 100 according to embodiments of the present invention may include different types of transistor systems. The inventors have discovered specific transistor circuits that can be used to detect and / or quantify chemical components, such as biomolecules or ions, according to embodiments of the present invention. The transistor circuits may be sensitive to different kinds of chemical components (e.g., different types of biomolecules or different types of ions).

[0048] In the field of sensing, field effect transistors (FETs) can be used with gate electrodes that are sensitive to one or more chemical components. When the gate electrode is exposed to a liquid or gas containing one or more chemical components, these one or more chemical components interact with the gate electrode in a specific way, so that the FET can detect, for example, a gate-source voltage V GS and drain-source voltage V DS Its electrical characteristics vary as a function of the drain-source current Ids, f. DS =f(V DS ,V GS ).

[0049] The usual approach is DS =f1(V DS ,V GS ) is either known or is measured before the transistor is exposed to the medium.

[0050] After exposure to the medium and interaction of the molecule to be detected with the gate, V DS , V GS and I DS The relationship between DS =f2(V DS ,V GS ) In most cases, the inventors have observed that f2 is shifted compared to f1.

[0051] In the classical approach, the shift between f2 compared to f1 is measured and analyzed. This is time consuming and requires some complex hardware / software work. The left diagram in Figure 1 shows a classical n-channel field effect transistor with gate G, source S, and drain D terminals. The right graph shows the gate-source voltage V GS Drain-source current Ids(I DS =f(V GS )) characteristics. At a given bias point V b In this case, the drain-source current as a function of bias voltage is I DS =f(V b ) can be derived.

[0052] The inventors have found that by combining transistors in a transistor circuit, the drain-source current of this transistor circuit as a function of gate-source voltage has a local minimum.

[0053] An example is illustrated in Figure 2A. Transistor circuit 110 comprises a first transistor 111 and a second transistor 112 with a shared source forming the source of transistor circuit 110 and a shared drain forming the drain of transistor circuit 110. A first voltage converter 113 converts the voltage at the gate of transistor circuit 110 to a voltage at the gate of first transistor 111 according to a transfer function having a first slope, and a second voltage converter 114 converts the voltage at the gate of transistor circuit 110 to a voltage at the gate of second transistor 112 according to a transfer function having a second slope. The first slope and the second slope have opposite signs.

[0054] Alternatively, first and second voltage converters 113 and 114 may be connected to the source of first transistor 111 and the source of second transistor 112, respectively, to generate gate-source voltages. An example of this is illustrated in FIG. 2B . In this case, the transistor circuit may additionally include third and fourth voltage converters 113′ and 114′ connected to the drains of first and second transistors 111 and 112, respectively, to drive the drains with versions of the signals on the sources of the first and second transistors, respectively, to achieve a constant drain-source voltage of the first transistor and a constant drain-source voltage of the second transistor, thereby achieving a stable drain-source current. This also favors constant gate operation given the two-transistor circuit.

[0055] It is not strictly necessary to keep the drain-source voltage constant. Systems according to embodiments of the present invention can also operate with some modulation of the drain-source voltage. This will cause a shift in the detected conduction minimum, but in different applications this is acceptable. A user may be interested in drift before and after exposure to a chemical of interest, for example, and the drift measured with a drain-source voltage modulation may be the same as the actual voltage drift for a particular voltage (e.g., Dirac voltage). In embodiments of the present invention, the system may be configured for post-processing of the found minimum to compensate for changes in the drain-source voltage.

[0056] The transistor circuit 110 of Figure 2 can be susceptible to any type of exposure. The two transistors can be the same type of transistor. They can be, for example, two n-channel transistors (as shown in the schematic), or they can also be, for example, two p-channel transistors, two depletion transistors, or two zero threshold voltage transistors.

[0057] A transistor has a threshold voltage V, which can be positive, negative, or zero, for example. th It can be characterized by:

[0058] In an embodiment of the present invention, the transistor has a non-linear current versus control voltage characteristic having a quadratic term in the polynomial expansion of their I=f(V) characteristics in the vicinity of the operating point V b . Any transistor can be used. They can also be bipolar transistors or MOSFET transistors, and they can also be used in the range below their threshold (<Vth).

[0059] The first voltage converter 113 uses the following equation to convert the voltage V GS at the gate of the transistor circuit to the voltage at the gate of the first transistor 111. V GS1 =V b +G(V GS -V d )

[0060] This function defines the operating point of the first transistor at the minimum conduction point (gate voltage V GS =V d ) that occurs at the control voltage V b . The voltage V GS1 applied between the gate and source of the first transistor increases with the control voltage V GS according to a given slope (G).

[0061] The second voltage converter 114 uses the following equation to convert the voltage V GS at the gate of the transistor circuit to the voltage at the gate of the second transistor 112. V GS2 =V b +G(V GS -V d )

[0062] The voltage V GS2 applied between the gate and source of the second transistor 、 decreases with the control voltage V GS according to the opposite slope or gain factor (-G).

[0063] The drain-source current of the first transistor is shown in Figure 2 as a function of gate-source voltage, I ds = f(T1). Because of the first voltage converter, it has a positive slope. The drain-source current of the second transistor is shown in Figure 2 as a function of the gate-source voltage, I ds = f(T2). Because of the second voltage converter, it has a negative slope. The trace is mirrored vertically in the unexposed transistor, as this is the initial state.

[0064] The drain-source current of both transistors together is the sum of the drain-source current of each transistor, I ds = f(T1, T2). This last trace of the transistor circuit is characterized by a local minimum in the current, and a quadratic behavior of the current around that minimum.

[0065] This minimum occurs when the voltage-current characteristic of one of the transistors is shifted, V d , the voltage of the first transistor is shifted to a position other than the minimum. This can occur, for example, when the first transistor or the second transistor is exposed to a chemical component and is sensitive to the chemical component. When the sensitive transistor is exposed to a chemical component (e.g., a biomolecule or an ion), this causes a shift in the transfer function and therefore a shift in the minimum. Advantageously, the specific voltage of this minimum can be measured using a system according to an embodiment of the present invention.

[0066] 2 may be exposed to and sensitive to a chemical component while the other transistor is not exposed to the chemical component, which may be present in a given medium such as a liquid, gel, or gas.

[0067] In the transistor circuit illustrated in FIG. 2, the transistors may be, for example, graphene transistors in which both transistors are exposed to a medium, but only one transistor is functionalized, for example, to be more sensitive to a given type of chemical moiety (e.g., a biomolecule), and the other is not.

[0068] In embodiments of the present invention, a single graphene field effect transistor (GFET) can also be used as the transistor circuit 110 (see inset in FIG. 3 ). This is because a single GFET has a local minimum in its current-voltage characteristic. In this case, the particular gate-source voltage at which the drain-source current reaches a local minimum is the Dirac voltage of the GFET. Using a system according to embodiments of the present invention, the GFET is integrated into a closed-loop system that functions as a low-pass filter delivering an output voltage equal to the Dirac voltage of the GFET. The loop can be a sigma-delta modulator that delivers a digital value of the Dirac voltage. In embodiments of the present invention, the Dirac voltage is shifted during exposure of the GFET to a chemical component to which the GFET is sensitive.

[0069] In the transistor circuit illustrated in FIG. 2, when two graphene transistors are used, one exposed and the other unexposed, or one functionalized and the other unfunctionalized, this results in the overlay of two nonlinear functions, both of which have Dirac points, and the combination of these functions has a common Dirac point. This common Dirac point shifts during exposure, as the exposure changes the electrical properties of the exposed graphene transistor. This is not illustrated in the graph on the right side of FIG. 2, which instead shows the current-voltage characteristics of a regular MOS transistor. In an embodiment of the present invention having a transistor circuit as illustrated in FIG. 2, both transistors may produce a transfer function that, for MOS transistors, can be approximated, for example, by a quadratic function near the point of minimum conduction. I DS =I1+a1(V GS -V d)+b1(V GS -V d ) 2 +I2-a2(V GS -V d )+b2(V GS -V d ) 2 I DS =I1+I2+(a1-a2)(V GS -V d )+(b1+b2)(V GS -V d ) 2

[0070] If the electrical characteristics of one of the transistors are changed, the minimum conduction point will shift. If transistor T2 is exposed, this could be I2, a2, and / or b2.

[0071] These equations and the following ones are valid when the transistor is a MOS transistor. Similar equations can be derived when two GFETs are used.

[0072] In the particular case of a MOS transistor biased in strong inversion, where Vth1 and Vth2 are the threshold voltages of the transistor, ds =f(V GS ) properties can be derived. I ds =a1(V GS1 -V th1 ) 2 +a2(V GS2 -V th2 ) 2 I ds =a1(V b +G(V GS -V d )-V th1 ) 2 +a2(V b +G(V GS -V d )-V th2 ) 2

[0073] In an embodiment of the present invention, the transistor circuit is such that the minimum conduction point of the system before exposure with identical matched transistors is at a gate voltage V GS =V d = 0. The following equation can then be derived: I ds =a1(V b +GV GS -V th1 ) 2 +a2(V b +GV GS -V th2 ) 2

[0074] The point of minimum conduction is when the transistor T2 is exposed to, for example, a chemical component, and the gain a2 or threshold V th2 is modified, it is shifted.

[0075] Minimum conduction point V GSmc The specific voltage at ds can be obtained by calculating the first derivative of and setting this derivative equal to zero, resulting in

number

[0076] A transistor circuit, such as that shown in Figure 2, has a local minimum (point of minimum conduction) at a specific voltage. If one of the transistors is sensitive and exposed to a chemical component, the specific voltage changes.

[0077] Advantageously, this particular voltage can be obtained using a system 100 according to an embodiment of the present invention that includes this transistor circuit.

[0078] In embodiments of the present invention, the transistors of the transistor circuit can be chemically sensitive transistors (CHEMFETs), or ion-sensitive transistors (ISFETs), but in a differential approach can be graphene transistors (GFETs). New application areas can also be supported, for example for measurements at very high temperatures or in harsh media, where graphene transistors are not sufficiently sensitive.

[0079] In embodiments of the present invention, the first transistor or the second transistor is exposed to and sensitive to the chemical component, in embodiments of the present invention, only one of the transistors is exposed to and sensitive to the chemical component.

[0080] In an embodiment of the present invention, a first transistor and a second transistor can be exposed to a chemical component, and only one is sensitive to the chemical component. For example, in the case of two (graphene) transistors, only one can be functionalized while both are exposed, and the other is not.

[0081] In embodiments of the present invention, only one of the first transistor or the second transistor can be exposed to a chemical moiety, and the first transistor and the second transistor are sensitive to the chemical moiety. For example, both transistors can be identical (e.g., two identical chemFETs), and only one is exposed to the chemical moiety.

[0082] Figure 3 shows the MIT model of the GFET. This model is presented in "Mackin, C. (2018) Graphene chemical and biological sensors: Modeling, systems, and applications. PhD thesis at the Massachusetts Institute of Technology." Figure 3 shows fitting using simple linear and quadratic approximations.

[0083] Dirac point (V d ), the current versus gate voltage characteristic can be approximated by a quadratic curve. I DS (V G )=I DS0 +α(V G -V d ) 2

[0084] Away from the Dirac point, the characteristics become more linear and can be approximated by two lines. I DS (V G )=I DS1 -2αV1(V G -(V d -V1))V G ≦V d -V1 I DS (V G )=I DS1 +2αV1(V G -(V d +V1))V G ≧V d +V1

[0085] The junctions between the three parts are connected by the gate voltage V d -V1 and V d +V1. At these points, I DS =I DS1 =I DS0 +α(V1) 2 and the slope (transconductance) is 2αV1. I DS (V G )={I DS1 -2αV1(V G -(V d -V1))if V G ≦V d -V1;I DS0 +α(V G -V d ) 2 if V d -V1 <V G <V d +V1;IDS1 +2αV1(V G -(V d +V1))if V G ≧V d +V1}

[0086] In systems according to embodiments of the present invention, where the transistor circuit 110 is a GFET, an analog low-pass filter loop automatically adjusts the gate voltage to the Dirac point. The advantage of this approach is that it allows for low-noise, high-resolution measurements of the Dirac point to be obtained in approximately the same time that the cited prior art systems take for each single step in their gate voltage ramp. Embodiments of the present invention allow for the use of simple analog / digital circuits that result in low energy consumption.

[0087] A system 100 for measuring a specific voltage (e.g., a Dirac voltage) of a transistor circuit 110 (e.g., a graphene field effect transistor or a transistor circuit such as that of FIG. 2 ) according to an embodiment of the present invention includes a transistor circuit 110 and a predefined bias voltage v , which is positive and negative around a given bias point. G and a bias voltage generator 120 configured to generate a toggling signal that toggles between . Thus, the bias point is the average level of the toggling signal generated by the bias voltage generator. The given bias point may be, for example, zero volts. However, the present invention is not limited thereto. The given bias point may also be different from zero.

[0088] Furthermore, the system 100 can measure the drain-source current of a transistor circuit (e.g., the channel current I of the graphene field effect transistor 110). DS , or the current I through transistors T1 and T2 in the circuit of FIG. DSThe present invention further includes a multiplier 140 configured to generate an electrical signal by multiplying an electrical signal, which is a function of the gate voltage (sum of A and B), by a waveform that alternates between two predefined values ​​+A and −A, alternating in synchronization with the toggling signal. Depending on the frequency of the toggling gate voltage and the characteristics (frequency response) of the transistor circuit, the alternating waveform applied to the multiplier can thereby be delayed (phase-shifted) relative to the gate voltage toggling signal. The predefined value A can be, for example, equal to 1. However, the present invention is not limited thereto. Other values ​​of A are also possible. The coefficient A is a multiplication coefficient of the signal to be integrated. This signal can be the drain current of the transistor circuit (e.g., a GFET drain current), a multiplication of the drain current, or the output of a transimpedance amplifier, and is referred to as the transistor circuit signal. This signal is integrated by an integrator that also has a gain coefficient. In an embodiment of the present invention, A is selected so that the product of all multiplication coefficients applied to the transistor circuit signal does not result in saturation of the first integrator at any time. This total gain coefficient affects the loop bandwidth and stability. The feedback or feedforward coefficients are preferably selected to achieve the desired bandwidth and stability, taking into account the transistor circuit characteristics and all multiplication coefficients involved in the integration of the transistor circuit signal. In an exemplary embodiment of the invention, A may be in the range of, for example, 0.001 to 1000.

[0089] The system 100 further comprises one or more integrators 130, a first integrator 130 of which is configured to integrate the electrical signal from the multiplier 140, and if more integrators 130 are present, a linear combination of the integrator output signals is provided to further integrators 130.

[0090] Furthermore, the system 100 includes an adder 150 configured to add the toggling signal of the bias voltage generator 120 and the integrated signal, or a processed version thereof, where the integrated signal is obtained by linearly combining the outputs of one or more integrators 130.

[0091] In an embodiment of the present invention, the system comprises a sample and hold circuit for sampling and holding the integrated signal to obtain a processed version of the integrated signal.

[0092] In an embodiment of the present invention, the integrated signal may be sampled before the toggling signal applied to the multiplier toggles from -A to +A (or +A to -A) and held for one full period of the toggling signal applied to the multiplier (which may have the same frequency as the toggling voltage applied to the gate, but with a possible delay), and thus until the next toggling from -A to +A (or +A to -A). However, the present invention is not so limited. A sample-and-hold circuit is not strictly required, and if a sample-and-hold circuit is present, the sample moment may be selected differently as specified above.

[0093] In an embodiment of the present invention, the last integrator in the loop may be implemented using a switched capacitor circuit to provide a sample and hold function.

[0094] In such a system, according to an embodiment of the present invention, a loop is formed. For the loop to converge to a stable gate voltage at a specific voltage minimum, the low-pass filter loop must integrate a quantity that is zero when the gate voltage is at the specific voltage and linearly dependent on the gate voltage near the specific voltage.

[0095] Near a certain voltage, the current versus gate voltage characteristic is quadratic, so that its derivative is a linear function of gate voltage that is null at the local minimum of the current.

[0096] Therefore, the loop calculates the quantity ΔI DS (V G )=I DS (V G +v G )-I DS (V G -v G ), where v Gis the predefined bias voltage, so the current difference is V G can be expressed using the derivative of the current at ΔI DS (V G )=2α(V G -V d )(2v G )

[0097] Therefore, the system must handle the difference between two current measurements performed at slightly different gate voltages. These current measurements must be performed sequentially. The gate voltage (V GS , V ゲート (also called V) G +v G and V G -v G and V G -v G The difference can be calculated in the integrator by reversing the integrating current when is applied to the gate.

number

number

number

[0098] This integration of the drain-source current of a transistor circuit is illustrated in Figure 4. A basic first-order measurement loop of a system for measuring a specific voltage at a local minimum (e.g., the Dirac voltage if the transistor circuit is a GFET) according to an embodiment of the present invention is illustrated in Figure 5. This shows a transistor circuit 110 (represented by its characteristic graph having a local minimum in its current-voltage characteristic), a bias voltage generator 120, a first integrator 130, a multiplier 140, and an adder 150. In this example, the bias point of the bias voltage generator is zero, so that the integrated signal is a specific voltage that corresponds to the local minimum in this example. If the bias point is different from zero, the integrated signal is the specific voltage minus the bias point.

[0099] The integrator integrates the difference between the two transistor circuit currents corresponding to two different gate voltages in order to integrate the slope of the current versus gate voltage characteristic rather than the current itself.

[0100] The basic loop illustrated in FIG. 5 forms a first-order linear system whose block diagram is shown in FIG.

[0101] The loop can be extended to any order. In an embodiment of the present invention, the system comprises exactly two integrators, and the input signal of the second integrator is the sum of the output signal of the first integrator and the output signal of the second integrator multiplied by a predefined constant a1. An example is illustrated in Figure 7, which shows a transistor circuit 110 (which can be, for example, a GFET or a transistor circuit as illustrated in Figure 2), a bias voltage generator 120, a first integrator 130a, a second integrator 130b, a multiplier 140, an adder 150, a multiplier 191 for multiplying the output signal of the second integrator 130b by a predefined constant a1, and an adder 192 for adding the output signal of the first integrator 130a and the output signal of the second integrator 130b.

[0102] The corresponding block diagram of a second-order system is illustrated in Figure 8. In this block diagram, K1 holds the product multiplication coefficients, such as the possible transimpedance coefficient, the amplitude of the multiplication waveform (A), and the capacitor used to implement the continuous-time integrator. K2 holds the time constant of the second continuous-time integrator.

[0103] In an embodiment of the present invention, the system has a predefined bias voltage modulation that is small enough so that the modulation is within the quadratic region of the transistor circuit characteristic (e.g., GFET characteristic).

[0104] The linear system description is based on a predefined bias voltage v G >2V1 and difference I DS (V G +v G )-I DS (V G -v G ) is valid when the gate voltage involved is in both linear regions of the transistor circuit characteristics. V G -v G ≦V d -V1 and V G +v G ≧V d +V1.

[0105] In that case, I DS (V G +v G )-I DS (V G -v G ) =I DS1 +2αV1(V G -(V d +V1))-[I DS1 -2αV1(V G -(V d -V1))] =4αV1(V G -V d )

[0106] The difference from the previous case is that the gain is 4αv G The problem is that it is 4αV1 rather than 4αV1.

[0107] Using large gate voltage modulation allows searching for a particular voltage over a large gate voltage range.

[0108] In embodiments of the present invention, the loop may be implemented with a continuous-time integrator or a discrete-time integrator.

[0109] The Matlab simulation results below show the behavior of the described second-order system, where the transistor circuit is a GFET. The MIT model used for the GFET is V d = 0.61 V. The approximation described in the document has the following parameters: α = 0.0016 A / V 2 , V1=0.0457V, I DS0 = 23 μA. These parameters are those of the model in Figure 3.

[0110] The first loop was constructed with a bandwidth of approximately 70 Hz. The predefined bias voltage was + / - 0.2 V at 1 kHz (i.e., large gate voltage modulation). The loop parameters were calculated considering a gain value of 4αV1. The simulation results in Figures 9 and 10 show that the filter output reaches the Dirac voltage in less than 50 ms (see Figure 7). There is a residual oscillation of + / - 1 mV at 1 kHz (see Figure 10, an enlarged version of Figure 9, from 0.607 to 0.612 V). Figure 11 shows the frequency response of the second-order system.

[0111] The simulation results below show a gate voltage modulation with the same bandwidth of 70 Hz, but with a predefined bias voltage v of 0.01 V (i.e., a smaller gate voltage modulation) instead of 0.2 V. G The second loop design uses the loop parameters, 4αv G The integrator time constant was calculated taking into account the current difference ΔI. Therefore, the integrator time constant is different from that used with larger bias voltages. The plot in Figure 12 shows the settling at the output of a second-order system with a small gate voltage modulation. Starting with the integrator drained, the correct value is reached within 100 ms. The loop isDS (V G )=-2αV1 is V G The loop first operates outside the quadratic GFET current region where V is constant instead of proportional to V. The loop only begins to operate when V enters the quadratic region, which is explained further in the following paragraph.

[0112] The residual oscillations of a second-order system with a bandwidth of 70 Hz and a small gate voltage modulation at 1 kHz have an amplitude of 2 mV. This is illustrated in Figure 13, which shows an expanded version of Figure 12 from 0.598 to 0.618 V.

[0113] The oscillation can be reduced with a smaller filter bandwidth. Figures 14, 15, and 16 show the results for a loop with a bandwidth less than 7 Hz and a large gate signal modulation. The filter settles within 500 ms with a residual oscillation of 15 μV. Figure 14 shows the frequency response of a second-order system with a 7 Hz bandwidth and a large gate voltage modulation. Figure 15 shows Matlab simulation results illustrating the settling of a second-order system with a 7 Hz bandwidth and a large gate voltage modulation. Figure 16 shows Matlab simulation results illustrating the residual oscillation at the output of a second-order system with a 7 Hz bandwidth and a large gate voltage modulation. The residual oscillation can be reduced by introducing a sample-and-hold circuit; however, this is not strictly required.

[0114] In an embodiment of the present invention, system 100 comprises a quantizer 160 configured to quantize the integrator signal at a predefined sampling frequency. Additionally, system 100 comprises a digital-to-analog converter 170 for converting the quantized signal to an analog signal for summation with the toggling signal at summer 150.

[0115] In this way, the low-pass filter loop is transformed into a sigma-delta modulator, which converts the current difference, ΔI DS This is possible due to the linear relationship between , and the gate voltage.

[0116] FIG. 17 shows a schematic diagram of an exemplary system for measuring a specific voltage corresponding to a local minimum value of current in a transistor circuit (which may be, for example, a GFET) with a second-order sigma-delta ADC, in accordance with an embodiment of the present invention.

[0117] 17 includes a transistor circuit 110, a bias voltage generator 120, a digital-to-analog converter 170, and an adder 150 for adding a signal from the bias voltage generator 120 and a signal from the digital-to-analog converter 170. The output of the adder 150 is connected to the gate of the transistor circuit 110. The system 100 further includes a waveform generator 142 configured to generate a waveform alternating between +A and −A, and a multiplier 140 configured to multiply the waveform generator waveform by an electrical signal that is a function of, for example, the channel current of a GFET or the sum of two resulting channel currents of both transistors in the transistor circuit 110. The system further includes a first integrator 130a for integrating the signal from the multiplier 140, and a second integrator 130b for integrating the sum of the signal from the first integrator 130a and the quantized output of the second integrator multiplied by a predefined coefficient a1 using a multiplier 191, obtained using an adder 192. The system further comprises a 1-bit quantizer for quantizing the output signal of the second integrator 130b, and a decimation filter 180 at the output of the quantizer.

[0118] In the exemplary embodiment illustrated in FIG. 17, instead of smoothly regulating the gate voltage to a particular voltage (e.g., the Dirac point in the case of a GFET), the sigma-delta loop regulates the gate voltage between two fixed voltages, V, within the region of validity of the linear relationship between the current difference and the gate voltage. ref1 and V ref2 , between the gate voltage V G Therefore, the output of the 1-bit quantizer is V ref1 and V ref2 and connects them to the adder 150.

[0119] The transistor circuit 110 then outputs only four different possible voltages: V ref1 ±v G and V ref2 ±v G , where v G are predefined voltages of the bias voltage generator 120. These generate only two different values ​​for the current difference. ΔI DS1 =ΔI DS (V ref1 )=I DS (V ref1 +v G )-I DS (V ref1 -v G ) ΔI DS2 =ΔI DS (V ref2 )=I DS (V ref2 +v G )-I DS (V ref2 -v G )

[0120] For the linear relationship to be valid, the gate voltage must be chosen such that: small gate voltage modulation (i.e., within the quadratic region of the transistor circuit), v G , all four gate voltages must be in the central quadratic portion of the transistor circuit characteristic. G Signal modulation is used in the quadratic region, whereby at a first predefined voltage, the gate voltage toggles between two levels on both sides of the specific voltage (the gate voltage is at a specific voltage V d ), and at a second predefined voltage, both levels are to the right of a certain voltage (the gate voltage is at a certain voltage V d greater than).

[0121] For the linear relationship to be valid, large gate voltage modulation (i.e., within the linear region of the transistor circuit), v G, all four gate voltages must be outside the central quadratic part of the transistor circuit characteristic. V ref1 +v G >V d (right linear region) V ref1 -v G <V d (left linear region) V ref2 +v G >V d (right linear region) V ref2 -v G <V d (left linear region)

[0122] In an embodiment of the present invention, the sigma-delta loop is

number

[0123] The sigma-delta loop is DS D is adjusted so that the average of ΔI DS is a transistor circuit I DS Against V Gs It is proportional to the slope of the characteristic and goes to zero at a particular voltage. The sigma-delta modulator generates its feedback signal such that the quantity integrated by the integrator is zero on average. I DS =DΔI DS2 +(1-D)ΔI DS1

[0124] Assuming a large gate voltage modulation: I DS =D4αV1(V ref2 -V d )+(1-D)4αV1(V ref1 -Vd ) I DS =0, therefore: D(V ref2 -V d )+(1-D)(V ref1 -V d )=0 D(V ref2 -V ref1 )+V ref1 -V d =0 V d =D(V ref2 -V ref1 )+V ref1

[0125] The present invention is not limited to second-order sigma-delta modulators, and sigma-delta modulators of different orders may be used.

[0126] In embodiments of the present invention, the integrator may be a continuous-time integrator or a discrete-time integrator.

[0127] Matlab simulations were performed of an exemplary system applied to a GFET described by the MIT model according to an embodiment of the present invention and illustrated in Figure 17. The Dirac point is at 0.61 V and the limit of the quadratic region is V = 0.045 V.

[0128] The converter is V ref1 From V ref2 If accurate conversion can be performed over the entire reference voltage range up to the minimum I of both Ts of the transistor circuit 110, the system can DS (i.e., the specific voltage of the transistor circuit) is V ref1 From V ref2 It can be measured in the range of

[0129] If the system is to operate with large gate modulation, the following conditions must be met: V ref1 +v G should be in the linear domain on the right, such that Vref1 +v G ≧V ref2 +V1⇒v G ≧V ref2 -V ref1 +V1 V ref1 -v G should be in the linear domain on the left, such that: V ref1 -v G ≦V ref1 -V1⇒v G ≧V1 V ref2 +v G should be in the linear domain on the right, such that V ref2 +v G ≧V ref2 +V1⇒v G ≧V1 V ref2 -v G should be in the linear domain on the left, such that: V ref2 -v G ≦V ref1 -V1⇒v G ≧V ref2 -V ref1 +V1

[0130] Therefore, in this exemplary embodiment of the present invention, a predefined bias voltage v, also referred to as a modulation voltage, is G must satisfy the following conditions: v G ≧V ref2 -V ref1 +V1

[0131] For the simulations, the following values ​​were used: V ref1 =0.55V, V ref2 = 0.65V, and v G =0.145V. Sample frequency F S = 1 kHz. In an embodiment of the present invention, the system comprises a decimation filter, which may be, for example, a sinc3 filter with an oversampling rate of 256.

[0132] Considering the above values, the GFET operates at the following gate voltages: V ref1 +v G =0.695V V ref1 -v G =0.405V V ref2 +v G =0.795V V ref2 -v G =0.505V

[0133] The plot in Figure 18 shows that these values ​​are at the limit of the linear approximation. In the plot, the drain current is shown as a function of the drain current for the exact model 10 and the approximation 11. The output of the decimation filter gives the Dirac point measurement at 0.6099V.

[0134] The output of the decimation filter converted to a voltage is shown in Figure 19. The output of the filter settles within 3*256 samples, corresponding to a settling time of 768ms.

[0135] FIG. 20 shows a zoomed plot of the settling output of the decimation filter.

[0136] In alternative embodiments of the present invention, the reference voltage may be chosen to be closer to the actual Dirac voltage. The following value may be chosen, for example: V ref1 =0.58V, V ref2 =0.63V, and v G = 0.095 V. In this example, the GFET is operated at four gate voltages where the linear approximation holds better, resulting in a better estimate of the Dirac point. This is illustrated in Figure 21, which shows a zoomed plot of the settling output of the decimation filter for the values ​​quoted above.

[0137] In an embodiment of the present invention, the quantizer 160 is configured to quantize a predefined number N q The digital-to-analog converter 170 is a multi-bit quantizer having Nq An exemplary embodiment of such a system is shown in Figure 22. This schematic shows a quantizer with N q The digital-to-analog converter 170 is an N-bit quantizer. q 17 except for the fact that it has bits.

[0138] The multi-bit approach allows for a wide range of search for a particular voltage. In embodiments of the present invention, the initial settling of the loop handles an initial guess at the particular voltage, and ultimately the DAC toggles between only two or three levels.

[0139] In an embodiment of the present invention, the multi-bit quantizer in the sigma-delta loop is a low-resolution ADC. In this embodiment, instead of converting the output of the current integrator, it converts a linear combination of the outputs of several integrators. In this example, the output voltage of the second integrator is converted.

[0140] In an embodiment of the present invention, the output of the low-resolution multi-bit quantizer is connected directly to the low-resolution DAC without any processing by the control circuit configured to determine the voltage value applied to the control electrode of the control circuit.

[0141] As explained earlier, the current difference ΔI DS and two reference voltages V ref1 , V ref2 A linear relationship between must be valid for the single-bit sigma-delta to deliver the correct value of the Dirac voltage.

[0142] When a multi-bit quantizer is used in a sigma-delta loop, the reference voltage can be extended beyond the region of validity of the linear relationship.

[0143] [V ref1 ;V ref2 Instead of feeding back only two different gate voltages at the extremes of the range [V ref1 ;V ref2 ] spread evenly across 2Nq The different possible DAC voltages are fed back and q is the number of quantizer bits used in the loop. After some settling time, the loop automatically converges to a situation where the feedback gate voltage toggles between only some of its possible feedback voltages, all located near a particular voltage. In an embodiment of the present invention, the number of quantizer bits is selected so that several consecutive DAC voltages are within the region of validity of the linear relationship between the current difference and the gate voltage.

[0144] In the following simulations, the transistor circuit is a GFET. The following simulations demonstrate the small gate voltage modulation (v) that can provide a digital code for the Dirac voltage in the range 0V to 1V using a 5-bit quantizer and a 32-level DAC. G = 5mV). The GFET model is the same as before. For small gate modulations, the current difference varies over the gate voltage range [V d -0.045;V d +0.045]. The DAC step is 1V / 32 = 30mV so that 2 or 3 DAC levels are within that gate voltage range.

[0145] Figure 23 shows a plot of the decimation filter output as a function of the number of samples, Figure 24 shows a zoom of the decimation filter output, and Figure 25 shows the 5-bit quantizer output as a function of the number of samples.

[0146] For small v modulation signals, the IDS vs. V of the GFET is such that the slope (integrated quantity) is proportional to the applied gate voltage. G It is preferable to have several consecutive DAC voltages within the quadratic region of the characteristic. This is a condition for forming a linear feedback system and having an accurate measurement of the Dirac voltage as consecutive DAC voltages. In fact, several DAC voltage outputs Vdac+ / -vG are preferably within the quadratic region.

[0147] Note that the system will likely start in the linear region, where the slope is constant. At that point, there is no actual feedback, but the integrator moves the DAC voltage toward the Dirac voltage. It is only when the DAC voltage enters the curved portion of the characteristic that there is an actual feedback signal and the loop settles. The closer to a quadratic characteristic you are, the more accurate your measurement of the Dirac point will be.

[0148] The system 100 may include a higher-level system (e.g., a controller) for selecting a reference voltage for the system 100 such that the loop always starts at the first stage, where a predefined bias voltage v G is selected so that the sum obtained by the adder settles to a first Dirac voltage that is within the linear region, preferably the quadratic region, of the graphene field-effect transistor characteristics. In a second stage, the host system is configured to select a predefined bias voltage so that the sum obtained by the adder is within the quadratic region of the graphene field-effect transistor characteristics. The system then settles to a second Dirac voltage that may be greater than, or at least as accurate as, the first obtained Dirac voltage. This results in a system that performs Dirac point measurements in a two-stage approach.

Claims

1. 1. A system (100) for characterizing a transistor circuit (110) having a gate, a source, and a drain, the transistor circuit being configured such that a drain-source current to gate-source voltage transfer function has a local minimum for a particular voltage, the system being configured to measure the particular voltage, the system comprising: said transistor circuit (110); - Generate a toggling signal to control a predefined bias voltage v around a given bias point. Ｇ a bias voltage generator (120) configured to toggle between positive and negative; one or more integrators (130); a multiplier (140) configured to generate an electrical signal by multiplying an electrical signal that is a function of the drain-source current of the transistor circuit (110) with a waveform that alternates between two predefined values ​​plus and minus A, alternating in synchronization with the toggling signal; a multiplier (140), in which a first integrator (130) of the one or more integrators (130) is configured to integrate the electrical signal from the multiplier (140), and if there are more integrators (130), a linear combination of the integrator output signals is provided to the integrator (130) after the first integrator; an adder (150) configured to add the toggling signal and an integrated signal, or a processed version of the integrated signal, wherein the integrated signal is obtained by linearly combining the outputs of the one or more integrators (130), and the adder (150) is configured to output the sum as the gate-source voltage of the transistor circuit.

2. The transistor circuit (110) a first transistor (111) and a second transistor (112), a first voltage converter (113) configured to convert a voltage at the gate of the transistor circuit (110) or at the source of the transistor circuit (110) into a gate-source voltage between the gate and the source of the first transistor (111) according to a transfer function having a first slope; a second voltage converter (114) configured to convert the voltage at the gate of the transistor circuit (110) or at the source of the transistor circuit (110) into a gate-source voltage between the gate and the source of the second transistor (112) according to a transfer function having a second slope, The system (100) of claim 1, wherein the first slope and the second slope have opposite signs.

3. 3. The system of claim 2, wherein the first transistor (111) or the second transistor (112) is exposed to a chemical component and is sensitive to the chemical component, or the first transistor (111) and the second transistor (112) are exposed to a chemical component and only one is sensitive to the chemical component, or either the first transistor (111) or the second transistor (112) is exposed to a chemical component and the first transistor (111) and the second transistor (112) are sensitive to the chemical component.

4. The system (100) of claim 2, wherein the first transistor (111) and the second transistor (112) are metal oxide semiconductor FETs or bipolar transistors.

5. The system (100) of claim 1, wherein the transistor circuit (110) is a graphene FET.

6. 2. The system (100) of claim 1, wherein the system comprises a sample and hold circuit for sampling and holding the integrated signal to obtain the processed version of the integrated signal.

7. the system comprises exactly two integrators (130a, 130b), The integrator (130) is a first integrator (130a) and a second integrator (130b) corresponding to the integrator subsequent to the first integrator (130a); The input signal of the second integrator (130b) is the output signal of the first integrator (130a) and a predefined constant a １ 2. The system (100) of claim 1, wherein the output signal of the second integrator is a sum of the output signal of the second integrator multiplied by a factor of 1.

8. the predefined bias voltages are such that the sum obtained by the adder is within a quadratic region of transistor circuit characteristics; The system (100) of claim 1, wherein within the quadratic domain of the transistor circuit, the current versus gate characteristic of the transistor circuit can be approximated by a quadratic curve.

9. the predefined bias voltage is such that the sum obtained by the adder is within a linear region of transistor circuit characteristics; The system (100) of claim 1, wherein within a linear region of the transistor circuit, the current versus gate characteristics of the transistor circuit can be approximated by two linear functions.

10. In a first stage, the predefined bias voltage is set so that the sum obtained by the adder is within a linear region of a transistor circuit characteristic, and in a second stage, the predefined bias voltage is set so that the sum obtained by the adder is within a quadratic region of the transistor circuit characteristic; 2. The system (100) of claim 1, wherein within a linear region of the transistor circuit, the current vs. gate characteristics of the transistor circuit can be approximated by two linear functions, and within a quadratic region of the transistor circuit, the current vs. gate characteristics of the transistor circuit can be approximated by a quadratic curve.

11. 2. The system (100) of claim 1, comprising: a quantizer (160) configured to quantize the integrated signal at a predefined sampling frequency; and a digital-to-analog converter (170) for converting the quantized signal to an analog signal for summation with the toggling signal at the summer (150).

12. 12. The system of claim 11, wherein the digital-to-analog converter toggles between a first predefined reference voltage for a digital zero input and a second predefined reference voltage for a digital one input, and the first and second predefined reference voltages and the predefined bias voltage are selected such that toggling at the predefined bias voltages corresponds to voltages in a left linear region of the transistor circuit, where the first predefined reference voltage minus the predefined bias voltage is less than a predetermined voltage and the second predefined reference voltage minus the predefined bias voltage is less than a predetermined voltage, and voltages in a right linear region of the transistor circuit, where the first predefined reference voltage plus the predefined bias voltage is greater than a particular voltage and the second predefined reference voltage plus the predefined bias voltage is greater than a particular voltage, and wherein current versus gate characteristics of the transistor circuit can be approximated by two linear functions in the left linear region and the right linear region of the transistor circuit.

13. the digital-to-analog converter (170) toggles between a first predefined reference voltage for a digital zero input and a second predefined reference voltage for a digital one input, the first predefined reference voltage and the predefined bias voltage being selected such that toggling at the predefined bias voltage results in a voltage at a left portion of a secondary region and a voltage at the same left portion of the secondary region where the first predefined reference voltage minus the predefined bias voltage is less than a predetermined voltage and the second predefined reference voltage minus the predefined bias voltage is less than a predetermined voltage; 12. The system (100) of claim 11, wherein the second predefined reference voltage and the predefined bias voltage are selected such that toggling at the predefined bias voltage results in a voltage at a right portion of the quadratic region of the transistor circuit and a voltage at the same right portion of the quadratic region where the first predefined reference voltage plus the predefined bias voltage is greater than a predetermined voltage and the second predefined reference voltage plus the predefined bias voltage is greater than a predetermined voltage, and where in the quadratic region of the transistor circuit a current vs. gate characteristic of the transistor circuit can be approximated by a quadratic curve.

14. The quantizer (160) selects a predefined number N ｑ a multi-bit quantizer having N bits, and the digital-to-analog converter (170) ｑ The system (100) of claim 11, comprising a bit.

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