The disclosure relates to a multiplexer, and to a method for operating a multiplexer. More particularly, the disclosure relates to an anolog multi-channel multiplexer with pumped bulk wells, and a method for operating such an analog multi-channel multiplexer.
Conventional microcontroller or microprocessor systems—e.g., systems that are used in the automotive field—frequently have to monitor a lot of analog input channels. Typically, a plurality of analog input channels may be digitized by some analog-to-digital converter (ADC). This may be done by feeding a plurality of input channels into a multi-channel multiplexer, where the output of this multiplexer may serve as an input of an ADC.
Typically, analog multi-channel multiplexers comprise an arrangement of (analog) transmission-gate switches. Such transmission-gate switches are typically controlled by a control voltage. The transmission-gate switch may forward an input signal received at an input-channel to its output if the control voltage assumes a first value, typically denoted by VDD. On the other hand, the transmission-gate switch may block an input signal received at an input-channel if the control voltage assumes a second value, typically given by ground, VGND.
Known transmission-gate switches comprise semiconductor devices, typically metal-oxide-semiconductor field-effect transistors (MOSFETs) with different conductivity types, i.e., with either electron (n) doped source and drain regions and a hole (p) doped bulk region (nMOS), or with p-doped source and drain regions and an n-doped bulk region (pMOS).
Because of this, each MOSFET includes two diode (np) structures, that may either be forward-biased if the n-structure lies on a lower potential than the p-structure, or it may be reverse-biased if the n-structure lies on a higher potential than the p-structure. It is known that for an electric current to flow through a forward-biased diode a so-called built-in voltage or diode drop voltage is necessary to be applied to the terminals of the np-structure. It is only under this condition that a diffusion current appearing in proximity of the np-junction can be counterbalanced.
The diode drop voltage depends on several factors, e.g., the doping of the n- and p-structures, current, the semiconductor material and temperature. Typically, the diode drop voltage ranges from 0.4 V to 1.0 V.
When considering an nMOS transistor first, typically the control voltage is applied to the gate terminal of the nMOS transistor while the input line is connected with the drain region (which is equivalent to the source region in this case). The bulk region of the nMOS transistor is also kept at VGND. It might well be that an input voltage is more than one diode drop voltage smaller than VGND. Because of this, the potential of the n-doped drain region is more than a diode drop voltage lower than the potential of the p-doped bulk region. This may, however, lead to a current flow through the nMOS transistor despite a control voltage VGND, indicating the blocking of the nMOS transistor.
Analogous considerations apply if one considers a pMOS transistor comprising p-doped source and drain regions and an n-doped bulk region. Known transmission-gate switches typically include an inverter that inverts the control voltage at the gate terminal of the pMOS transistor with respect to the control voltage at the gate terminal of the nMOS transistor. This means that in the case of a control voltage set to VGND, the gate terminal of the pMOS transistor is set to VDD, and vice versa. It may well be that an input voltage, applied to the source terminal of the pMOS transistor, is more than one diode drop voltage higher than VDD. The bulk region of the pMOS transistor is also kept at VDD. Because of this, the potential of the p-doped drain region is more than a diode drop voltage higher than the potential of the n-doped bulk region. This may lead to a current flow through the pMOS transistor despite a control voltage VGND, indicating the blocking of the entire transmission-gate switch.
Therefore, transmission-gate switches may go to bipolar conduction due to forward-biased source-bulk or drain-bulk diodes when the input voltages either go more than a diode drop voltage below VGND, or when the input voltages exceed VDD by more than a diode drop voltage.
A second effect might lead to weak conduction of a known transmission-gate switch even at input voltages that are less than a diode drop voltage but more than a MOSFET threshold voltage below VGND, or at input voltages that are less than a diode drop voltage, but more than a MOSFET threshold voltage above VDD. The MOSFET threshold voltages may depend on several physical parameters, e.g., the gate material, the thickness of the oxide layer, the conductivity type, doping concentrations of the bulk region, the distance between the source region and the drain region, the temperature and the voltage between source region and bulk region. Typical MOSFET threshold voltages in the case with source and bulk regions at the same potential are a few 100 mV. Already at the before-mentioned MOSFET threshold voltages an n-type (conductive) inversion channel may develop at the semiconductor-oxide interface of the nMOS transistor (thus, the conductivity type is n), and a p-type (conductive) inversion channel may develop at the semiconductor-oxide interface of the pMOS transistor (thus, the conductivity type is p), respectively. Since the inversion channel is of the same type as the source and drain regions, current may pass through it.
The two previously described phenomena are known as parasitic conduction. Parasitic conduction may lead to distortion of an input signal at a multi-channel multiplexer both already at the input channel and/or at the output of the multi-channel multiplexer.
If transmission-gate switches are used in multi-channel multiplexer designs, the selected input signal might be distorted at the output whenever at least one of the input signals corresponds to a voltage that is only a few 100 mV below VGND or a few 100 mV above VDD. Already at such small voltages weak conduction through the inversion channel of a MOSFET might occur. At input voltages that are at least a diode drop voltage below VGND or above VDD, the situation worsens again because of the additional bipolar conduction, e.g., due to the forward-biased source-bulk diode of the nMOS transistor.
However, today, integrated circuit design typically requires very accurate output signals at the multi-channel multiplexer with an error of less than 5 mV, typically between 0.1 mV and 1 mV. This can, however, not be provided by the known transmission-gate switches comprised by known multi-channel multiplexers.
Each channel of a multi-channel multiplexer may comprise a combination of two transmission-gate switches, forming a so-called double-transmission gate, hence comprising two nMOS transistors and two pMOS transistors. In the fabrication process of such double transmission-gate switches each of the two nMOS transistors is implanted on a single p-doped bulk layer, a so-called p-well. Analogously, each of the pMOS transistors is implanted on a single n-doped bulk layer, a so-called n-well.
However, this spatial separation of the single transistors leads to a drastic increase of the area occupied by the multi-channel multiplexer within, e.g., a microcontroller or microprocessor system.
For these or other reasons there is a need for an improved multi-channel multiplexer, and an improved method for operating a multi-channel multiplexer.
The accompanying drawings are included to provide a further understanding of the present disclosure and are incorporated in and constitute a part of this specification. The drawings illustrate embodiments of the present disclosure and together with the description serve to explain the principles of the disclosure. Other embodiments of the present disclosure and many of the intended advantages of the present disclosure will be readily appreciated, as they become better understood by reference to the following detailed description.
a schematically depicts an analog multi-channel multiplexer feeding one of a selected analog input channels into an analog-to-digital converter (ADC);
b schematically depicts one possible arrangement of transmission gates comprised by an analog multi-channel multiplexer according to an embodiment of the disclosure;
a schematically depicts exemplarily two nMOS transistors fabricated on a single p-well as comprised by embodiments of the disclosure;
b schematically depicts exemplarily two pMOS transistors fabricated on a single n-well as comprised by embodiments of the disclosure;
In the following detailed description, reference is made to the accompanying drawings, which form a part hereof, and in which is shown by way of illustration specific embodiments in which the disclosure may be practiced. It is to be understood that other embodiments may be utilized and structural or other changes may be made without departing from the scope of the present disclosure. The following detailed description, therefore, is not to be taken in a limiting sense, and the scope of the present disclosure is defined by the appended claims.
a shows a schematic view of a multi-channel multiplexer (MUX) 101 that is connected to an analog-to-digital converter (ADC) 102. The multiplexer 101 may select one of several signals. In general, the signals might be either analog or digital signals. In the following, analog signals will be considered. In this case, the multiplexer may be a special type of an analog switch comprising so-called transmission gates, described in more detail below in relation to
b shows schematically an arrangement of transmission gates 110.1, 110.2, 110.3, . . . , 110.n. In complementary metal-oxide-semiconductor (CMOS) technology multi-channel multiplexers comprising transmission gates are called analog multi-channel multiplexers (analog multiplexers). In the case of analog multiplexers, the entire input signal, e.g., input voltage, may be forwarded to an output of the analog multiplexer. This is accomplished by creating a conductive channel between the input and output of the analog multiplexer. Since the conductive channel is not sensitive to the direction of current flow through it, the analog multiplexers might be used at the same time as analog demultiplexers. This means, a signal entering the multiplexer at, e.g., its output 103, that is the demultiplexer's input, might be forwarded to one of the multiplexer's input lines 101.1, 101.2, 101.3, . . . , 101.n, that is, the demultiplexer's output lines.
Each of the transmission gates may be controlled, that is, either blocked or set in conduction state, by applying control voltages Vg1, Vg2, Vg3, Vgn, 111.1, 111.2, 111.3, . . . , 111.n, respectively, at the transmission gates 110.1, 110.2, 110.3, . . . , 110.n, respectively. Typically, the control voltages Vg1, Vg2, Vg3, Vgn, 111.1, 111.2, 111.3, . . . , 111.n, respectively, are chosen such that only one of the transmission gates 110.1, 110.2, 110.3, . . . , 110.n is conducting while the others are blocked (so-called n-to-1 multiplexers). In such a configuration, only the one selected of the input signals, e.g., of the input voltages Vin1, Vin2, Vin3, . . . , Vinn, 112.1, 112.2, 112.3, . . . , 112.n, respectively, is forwarded to the output 103 of the analog multiplexer. Typically, each of the control voltages Vg1, Vg2, Vg3, Vgn, 111.1, 111.2, 111.3, . . . , 111.n, respectively, may assume two values, e.g., the negative supply voltage, VSS, and the positive supply voltage, VDD, introduced further below, e.g., VSS=−3 V to 0 V, for instance, VSS=VGND=0 V and VDD=2 V to 6 V or VDD=6 V to 20 V, e.g., VDD=5 V, VDD=15 V, characterizing the blocking and the conducting, respectively, of each corresponding transmission gate 110.1, 110.2, 110.3, . . . , 110.n.
The nMOS transistor 201 comprises a drain terminal 201.1 connected to a first n-doped region that may be fabricated within a p-doped well (p-well), a source terminal 201.3 connected to a second n-doped region that may be fabricated within the p-well, and a gate terminal 201.2. The gate terminal 201.2 might be formed by a metal, e.g., aluminium, but it is not restricted to; nowadays, the gate terminal is often formed by, e.g., a layer of polycrystalline silicon or transition metals. The gate terminal 201.2 may be separated by an oxide, but is not restricted to, since also different dielectric materials may be used, e.g., in particular high-k dielectrics, from a p-doped bulk 210 which may correspond to the p-well. In the example transmission gate 200 the drain terminal 201.1 is connected to an input line 206, e.g., the input voltage Vin, the source terminal 201.3 is connected to the output channel 207. The gate terminal 201.2 is connected to the control voltage Vg 204. The p-doped bulk 210 which may, for way of example, correspond to or be part of the p-well, is connected to the voltage VBn 208. The p-doped bulk 210 may be connected with a, e.g., negative supply voltage VSS; in this case VBn=VSS. It should be noticed, that in this case, source and drain terminals are completely equivalent, that is, current may flow in either direction through the nMOS transistor 201. The pMOS transistor 202 comprises a drain terminal 202.1 connected to a first p-doped region that may be fabricated within an n-doped well (n-well), a source terminal 202.3 connected to a second p-doped region that may be fabricated within the n-doped well, and a gate terminal 202.2. The gate terminal 202.2 might be formed by a metal, e.g., aluminium, but it is not restricted to, or by, e.g., a layer of polycrystalline silicon or transition metals. The gate terminal 202.2 may be separated by an oxide, but is not restricted to, since also different dielectric materials may be used, e.g., in particular high-k dielectrics, from an n-doped bulk 211 which may correspond to the n-well. In the example transmission gate 200 the drain terminal 202.1 is connected to the output channel 207, and to the source terminal 201.3 of the nMOS transistor 201. The source terminal 202.3 is connected to the input line 206, e.g., the input voltage Vin, and to the drain terminal 201.1 of the nMOS transistor 201. The gate terminal 202.2 is connected to the control voltage
The functionality of the transmission gate 200 is, thus, amongst others, governed by the functionality of the nMOS transistor 201 and the pMOS transistor 202. The nMOS transistor 201 may become conducting if the voltage Vg,n at the gate terminal 201.2 is a typical threshold voltage, Uth,n, higher than the voltage VS,n at the source terminal 201.3. Once the gate voltage, Vg,n, is a typical threshold voltage, Uth,n, higher than the source voltage, VS,n, a so-called (n-conducting) inversion channel may be formed through the p-doped bulk. The threshold voltage may depend on many factors, e.g., the gate material, the thickness of the oxide layer, the conductivity type, the doping concentration of the bulk, the temperature, and the channel length, that is the distance between the two n-doped regions of the source terminal 201.3 and of the drain terminal 201.1. In the case that the bulk voltage, VBn, is equal to source voltage, VS,n, typical threshold voltages, Uth,n, may be a few hundred milli-volts. The bulk voltage, VBn, does not need to equal the source voltage, VS,n. In the case that VBn<VS,n the threshold voltage depends on, amongst others, the difference VS,n−VBn. The effect of such a voltage difference may be explained by considering a backward-biased diode formed by the n-doped source region and the p-doped bulk region. Since the voltage VS,n on the source terminal is higher than the voltage VBn on the bulk, this diode is backward biased. Because of this, a higher threshold voltage may need to be applied to the gate terminal in order to create an inversion channel. Analogous considerations apply for the pMOS transistor 202. The pMOS transistor 202 may become conducting if the voltage Vg,p at the gate terminal 202.2 is a typical threshold voltage, Uth,p, lower than the voltage VS,p at the source terminal 202.3. Once the gate voltage, Vg,p, is a typical threshold voltage, Uth,p, lower than the source voltage, VS,p, a so-called (p-conducting) inversion channel may be formed through the n-doped bulk and current may flow from the source region to the drain region. The threshold voltage may depend on, e.g., the same factors as discussed above in relation to the nMOS transistor 201. In the case that the bulk voltage, VBp, is equal to source voltage VS,p, typical threshold voltages may be a few hundred milli-volts. For analogous reasons as discussed above with respect to the nMOS transistor 201, in the case of VS,p<VBp, a higher threshold voltage, may need to be applied to the gate terminal in order to create an inversion channel, that is, the difference VS,p−Vg,p may need to be larger in the case VS,p<VBp as compared to the case VS,p=VBp.
Finally, it should be noted that it may also be possible to apply a control voltage at the gate terminal 202.2 of the pMOS transistor 202. In this case the inverted voltage is applied at the nMOS transistor 201.
First, the behavior of an ideal transmission gate 200 is described: assume that the control voltage, Vg, 204 may assume the two values VSS and VDD of the negative and positive supply voltages that may be connected with the p-bulk 208 and n-bulk 209, respectively. For the mere purpose of example, assume that the control voltage, Vg, 204 has a value VSS which might indicate the blocking of the transmission gate 200. In this case, the gate terminal 201.2 and the bulk 210 of the nMOS transistor 201 are at the same potential and no or only a weak inversion channel may develop between the drain region 201.1 and the source region 201.3 of the nMOS transistor 201, regardless of the input voltage, Vin, 206. At the same time, the inverter 203 may generate a voltage
The behavior described previously corresponds to the functioning of an ideal transmission gate 200. The situation might, however, be more involved because of the semiconducting devices comprised in the fabrication of a transmission gate 200. For way of example, an nMOS transistor 201 comprises an np-junction between the source region and the bulk, and it comprises a pn-junction between the bulk and the drain region. Because of this, the nMOS transistor 201 may be thought of an arrangement of two diodes, the one of which is forward-biased, the other is backward-biased. An np-junction may begin conducting when the voltage at the n-region is a typical diode threshold (diode drop) voltage smaller than the voltage at the p-region. In this case, the diode is said to be forward biased. This diode drop voltage may depend on several factors, e.g., the semiconductor material, the conductivity type, the doping concentration of the n- and p-regions, and the temperature. Typical values of the diode drop voltage range from 0.5 V to 1.0 V or from 0.6 V to 0.8 V, and is typically in the ballpark of 0.7 V. An analogous effect may arise within the nMOS transistor 201. It may happen, that the input voltage, Vin, 206 falls a typical diode drop voltage below the negative supply voltage, VSS, applied to the bulk 210 of the nMOS transistor 201. As described previously, the nMOS transistor 201 comprises an immanent structure of a bipolar npn-transistor. Therefore, the nMOS transistor 201 not only might become conducting when an n-conducting inversion channel develops, but also when the input voltage, Vin, 206 is a diode drop lower than the voltage at the bulk 210. This may imply that the nMOS transistor 201 might become conducting also in cases that exclude such a conduction e.g., when Vg=VSS. The bipolar conduction through the immanent npn-transistor comprised by the nMOS transistor 201 is one source of so-called parasitic conduction. Analogous considerations apply to the pMOS transistor 202 that comprises an immanent pnp-transistor. This pnp-transistor might begin conduction when the input voltage, Vin, 206 is a diode drop voltage larger than VDD.
In a first embodiment of the present disclosure which is described in the following with regard to
In the following the blocking of the transmission gates that are comprised by the analog multiplexer according to the first embodiment of the disclosure will be described. Typically, in an n-to-1 analog multiplexer, n-1 transmission gates might be blocked, while only one, say the m-th, transmission gate is conducting. This may, e.g., imply, that n-1 control voltages Vg,j=VSS,j, while one, e.g., Vg,m=VDD,m. It may well be that VSS,j=VSS, VDD,j=VDD for all j. It is understood that the aforementioned example is not restrictive. An anlog multiplexer according to the first embodiment of the disclosure might also comprise k outputs, where k is, in general, an integer number between 1 and n, with n being the number of input lines of the analog multiplexer. In this general case, n-k transmission gates may be blocked, while k transmission gates are conducting.
As described above, parasitic conduction may arise if the input voltages Vin,j, 112.1, 112.2, 112.3, . . . , 112.n lie outside the operation ranges VSS,j to VDD,j, independent of the corresponding control voltages Vg,j, 111.1, 111.2, 111.3, . . . , 111.n. Because of this, the voltages VBn,j and VBp,j at the bulks of, respectively, the nMOS transistors and pMOS transistors of each of the transmission gates 110.1, 110.2, 110.3, . . . , 110.n may be set, respectively, to a voltage that is at least a diode drop voltage lower or higher than VSS,j or VDD,j. Typically, VBn,j and VBp,j may be chosen to be VSS,j−aj·Udiode, and VDD,j+aj·Udiode, respectively, wherein Udiode denotes the diode drop voltage and each of the aj may be any real number typically larger than 1, typically ranging between 0.8 and 2. The values chosen for the aj may depend on several factors, e.g., typical input voltage values Vin,j 112.1, 112.2, 112.3, . . . , 112.n, the claimed accuracy of the output signal 103 with respect to an input signal 112.1, 112.2, 112.3, . . . , 112.n. Typically, the aj may, however, be restrained by minimal input voltages, Vin,j,low*, or maximal input voltages, Vin,j,high*, that are let through the source terminals 202.3 or drain terminals 201.1 by so-called electrostatic discharge (ESD) preventing structures. Such ESD preventing structures prevent voltages that might cause damage or destruction of electronic components or assemblies, e.g., a transmission gate or a multiplexer, from being applied to said components or assemblies. For many purposes it may be the case that there is no distortion of the output signal 103 with respect to an input signal at all; in practice, this might imply that the difference between the voltage at the output 103 with respect to the voltage at a selected input ranges from 10−9 V to 10−3 V, wherein typical input voltages might be of the order of a few volts. It might be, hence, of uttermost importance that no signal, that is, e.g., current or voltage, may pass through each of the blocked transmission gates. If a signal passed through one of the blocked transmission gates, the signal, e.g., current or voltage, of the one selected channel (transmission gate) would be distorted.
The aforementioned voltages typically, VBn,j and VBp,j may be properly adjusted with the aid of, e.g., one or more charge pumps 501 as schematically depicted in
So far, only the elimination of the parasitic bipolar conduction has been described. As pointed out before an nMOS transistor 201 may start conducting when the gate terminal 201.2 is at a higher voltage, Vg,n, than the source terminal 201.3 (source voltage VS,n). If the voltage difference Vg,n−VS,n is larger than a typical threshold voltage, Uth,n, the nMOS transistor 201 develops an n-conducting inversion channel, and the input signal may pass through the nMOS transistor 201. It should be noticed, that it is known that the threshold voltage, Uth,n, may depend on the difference VS,n−VBn. Because of this, the necessary threshold voltage may increase with an increasing difference VSS−VBn. Nevertheless, even at very high differences VSS−VBn, which might imply large values of the aj, e.g., aj ranging between 1.5 and 2, an input signal 206 may pass through the nMOS transistor 201. This is because the threshold voltages in the case VS,n−VBn>0 may still be in the ballpark of a few 100 mV. Analogous considerations apply to the pMOS transistor 202 which may start conducting when the gate terminal 202.2 is at a lower voltage, Vg,p, than the source terminal 202.3 (source voltage VS,p). If the voltage difference VS,p−Vg,p is larger than a typical threshold voltage, the pMOS transistor 202 develops a p-conducting inversion channel, and the input signal may pass through the pMOS transistor 202. It should be noticed, that it is known that the value of the threshold voltage of a pMOS transistor 202 may depend on the difference VBp−VS,p. Because of this, the necessary threshold voltage may increase with an increasing difference VB,p−VDD. For the same reasons as discussed above in relation to the nMOS transistor 201, even at very high differences VBp−VDD, which might imply large values of the aj, e.g., aj ranging between 1.5 and 2, an input signal 206 may pass through the pMOS transistor 202.
In each of the transmission gates 110.1, 110.2, 110.3, . . . , 110.n comprised by the analog multiplexer 101 according to the first embodiment of the disclosure each of the gate terminals 201.2 and 202.2 of each of, respectively, the nMOS transistor 201 and pMOS transistor 202 may be connected to one or more charge pumps 501. These charge pumps may be different from the charge pumps connected to the bulk 210 and 211. This allows to set the gate terminals of each of the nMOS transistors 201 and pMOS transistors 202 comprised by the multiplexer 101 to voltages that may be, respectively, lower or higher than extreme input voltages Vin,j,low*, Vin,j,high*. That is, the extreme input voltages Vin,j,low* correspond to the lowest voltages that might arise at the corresponding inputs 101.1, 101.2, 101.3, . . . , 101.n, while the extreme input voltages Vin,j,high* correspond to the highest voltages that might arise at the corresponding inputs 101.1, 101.2, 101.3, . . . , 101.n. For way of example, each gate terminal 201.2 of the nMOS transistors 201 or each of the gate terminal 202.2 of the pMOS transistors 202 might be set to a different value. Alternatively, all gates 201.2 of all nMOS transistors 201 may be pumped to the same voltage, e.g., to the lowest of the voltages Vin,j,low*, and/or all gates 202.2 of all pMOS transistors 202 may be pumped to the same voltage, e.g., to the highest of the voltages Vin,j,high*. In yet another alternative of the first embodiment of the disclosure, the gate terminals of the nMOS transistors 201 and pMOS transistors 202 might be pumped to voltages, e.g., that equal, respectively, VBn,j, and VBp,j with the values given above, that is VBn,j=VSS,j=VSS,j−aj·Udiode, VBn,j=VDD,j+aj·Udiode.
To summarize the blocking of the transmission gates 110.1, 110,2, 110.3, . . . , 110.n comprised by the analog multiplexer according to the first embodiment of the disclosure, it should be noticed that adjustment of the voltages at the gate terminals 201.2 of the nMOS transistors 201 and of the voltages at the gate terminals 202.2 of the pMOS transistors 202, e.g, with the use of at least one charge pump, guarantees, amongst others, that no signal passes from the input line through the transmission gate to the corresponding output. The use of a single charge pump may suffice in order to bring the gate and bulk terminals of all blocking transmission gates to a sufficiently low voltage. The value of this voltage may depend on several factors, e.g., the voltages applied at the input lines 112.1, 112.2, 112.3, . . . , 112.n, accuracy of the output signal with respect to the input signal of the selected, i.e., conducting, transmission gate. The transmission gates 110.1, 110,2, 110.3, . . . , 110.n described in relation with the first embodiment of the disclosure may eliminate two sources of parasitic conduction within a transmission gate: the first is, as detailed out above, the bipolar conduction between the source region and drain region through the bulk region, which occurs significantly whenever the voltage at the source is a diode drop voltage lower than the voltage applied at the p-doped bulk of an nMOS transistor, or if the voltage at the source is a diode drop voltage higher than the voltage applied at the n-doped bulk of a pMOS transistor. The second source of parasitic conduction eliminated by the first embodiment of the disclosure is the conduction that may arise if the voltage at the source or drain terminals differs from the voltage at the gate terminal by more than a threshold voltage Uth which may lead to the creation of a conducting inversion channel through the MOS transistors at the oxide-semiconductor interface.
After the description of the blocking of the transmission gates comprised by the analog multiplexer according to the first embodiment of the disclosure, it is now considered how one or more selected transmission gates can be brought into a conducting state. As describe above a transmission gate begins conduction if the control voltage, Vg, 204 is set to a value higher than the control-voltage value indicating the blocking of a transmission gate. For example, Vg=VDD, might be chosen. Assume that the gate terminals 201.2 of the nMOS transistors 201 of the conducting transmission gates 110.1, 110.2, 110.3, . . . , 110.n are connected with the control voltages Vg1, Vg2, Vg3, Vgn, 111.1, 111.2, 111.3, . . . , 111.n, respectively, then the corresponding gate terminals 201.2 are at the same voltage. Analogously, the gate terminals 202.2 of the pMOS transistors 202 of the conducting transmission gates 110.1, 110.2, 110.3, . . . , 110.n are connected with the control voltages
The analog multiplexer according to the first embodiment of the disclosure leads, thus, to a highly accurate forwarding of the input signal of the selected input line to the output of the analog multiplexer. The distortion of the output signal with respect to the input signal may be reduced to a negligible percentage, i.e., typical relative distortions are smaller than 10−2%.
A second embodiment of the disclosure is now described with respect to
The physical layout of the nMOS structure 410 comprising the nMOS transistors M2301.2, M4303.2 comprised by the double transmission gate 300 is shown in
Analogous considerations apply to the case where a p-doped substrate is used: one or more n-wells are diffused into the p-doped substrate for forming the bulks of the pMOS transistors M1301.1, M3303.1 of each of the double transmission gates comprised by the analog multiplexer 101. It is then desirable, but not limiting, to implant, e.g., all p-doped source regions 421.1, 423.1, and drain regions 421.2, 423.2 that correspond to one double transmission gate in one single n-well. As described above, the p-doped source regions and drain regions of all double transmission gates comprised by the analog multiplexer 101 might be implanted in a single or limited number of n-wells. In this second example, the n-doped drain regions 412.1, 414.1, and source regions 412.2, 414.2, of the nMOS transistors M2301.2, M4303.2 of the double transmission gates comprised by the analog multiplexer 101 of the second embodiment of the disclosure, may be implanted in the p-doped substrate. In a further alternative of the second embodiment of the disclosure, the source region 421.2 and the drain region 423.1 might be comprised by a single p-doped region. This reduces the area of the pMOS structure 420 further.
In a further alternative of the second embodiment of the disclosure a so-called triple-well structure may be used: in this case, one or more n-wells 421 may be first diffused into a p-substrate. The n-well(s) 421 form the bulk(s) of pMOS transistors. Next, one or more p-wells 411 may be diffused into (each of) the n-well(s). The p-well(s) 411 form the bulk(s) of nMOS transistors. The pMOS transistors M1301.1 and M3303.1 are formed by diffusing the p-doped source regions 421.1, 423.1 and drain regions 421.2, 423.2 into the n-well(s) 421. The corresponding nMOS transistors M2301.2 and M4303.2 are comprised by the p-well(s) 411 diffused into the n-well(s). As shown in
A triple-well structure might analogously be formed by using an n-doped substrate comprising one or more p-wells each of which comprises one ore more n-wells. The p-well(s) form the bulk of one or more nMOS structures. The n-wells form the bulk of one or more pMOS structures.
In the following, the nMOS structure 410 of the analog multiplexer 101 of the second embodiment of the disclosure is first described. The one or more p-wells comprise at least two nMOS structures M2301.2, M3303.2. As pointed out before, in one alternative it may be desirable to implant more than two or all nMOS structures comprised by the analog multiplexer 101 in a single p-well. Each of the gate terminals, that is the metal-oxide structure, 415, 416 may be fabricated as described above in relation with the first embodiment of the disclosure.
Now, the blocking of one example double transmission gate 300 according to the second embodiment of the disclosure is described. In this case the gate terminals 415, 416, of each double transmission gate 300 that needs to be blocked may be set to the corresponding control voltage Vg,j, e.g., Vg,j=VSS,j, or Vg,j=VSS if all negative supply voltages are the same. The p-well or the p-wells 411 are set to a voltage VBn,j 413 that is at least a diode drop voltage Udiode lower than VSS,j, typically VBn,j=VSS,j−aj ·Udiode, wherein Udiode denotes the diode drop voltage and each of the aj may be any real number typically ranging between 0.8 and 2. The values chosen for the aj may depend on several factors, e.g., typical minimal input voltages, Vin,j,low*, or maximal input voltages, Vin,j,high*, determined by the ESD preventing structures, the claimed accuracy of the output signal 103 with respect to an input signal 112.1, 112.2, 112.3, . . . , 112.n. For many purposes the case may be that there is no distortion of the output signal 103 with respect to an input signal at all; in practice, this might imply that the relative error between the voltage at the output 103 and the voltage at a selected input is smaller than 10−2%. It might, hence, be of uttermost importance that no signal, that is, e.g., current or voltage, may pass through each of the blocked double transmission gates. If a signal passed through one of the blocked double transmission gates, the signal, e.g., current or voltage, of the one selected channel (double transmission gate) would be distorted. Therefore, by setting the voltages VBn,j 413 of the p-well or p-wells properly, the parasitic bipolar conduction can be eliminated. It should be noticed that, since the nMOS structure 410 comprises more than one npn transistor structures, e.g., the npn transistor 417.1 comprising the n-doped drain region 412.1, the n-doped source region 412.2 and the p-well itself, or the npn transistor 417.2 comprising the n-doped drain region 412.1, the n-doped source region 414.2 and the p-well itself. Thus, by applying a properly chosen bulk voltage VBn,j 413, all possible sources for parasitic bipolar conduction are eliminated or highly suppressed. One possibility of how to properly choose the bulk voltages VBn,j 413 will be presented in the following paragraph.
The p-doped substrate or the p-well(s) 411 of the nMOS structure 410 may be connected to one or more charge pumps 501, whereby a typical charge pump has already been described above in relation to the first embodiment of the disclosure, and will, thus, be referred to without being repeated here again. This allows to set the p-doped substrate or the p-well(s) 411 of the nMOS structures 410 comprised by the multiplexer 101 to voltages that may be lower than extreme input voltages Vin,j,low*. That is, the extreme input voltages Vin,j,low* correspond to the lowest voltages that might arise at the corresponding inputs 101.1, 101.2, 101.3, . . . , 101.n, e.g., voltages allowed for by the ESD preventing structures. For way of example, if present, each p-well of the nMOS structures 411 might be set to a different value. Alternatively, all p-wells (if more than one is present) 411 of all nMOS structures 410 may be pumped to the same voltage, e.g., to the lowest of the voltages Vin,j,low*. It should be noted that the values aj given above, might be related to the corresponding Vin,j,low*, that is, e.g., through VBn,j==VSS,j−aj·Udiode.
As explained already above in relation to the first embodiment of the disclosure, there may exist a second source of parasitic conduction. Once the p-doped substrate or the p-well(s) 411 lies at a lower potential than the gate terminal 415, depending on the voltage Vin,j at the input line 301.3 an n-conducting inversion channel might develop. Such an inversion channel may develop when the input voltage, Vin,j, applied at the drain terminal 412.1 of the nMOS structure 410 is a threshold voltage, Uth,n,j, lower than the voltage at the gate, Vg,j, 310. As pointed out above in relation with the first embodiment of the disclosure, the threshold voltage may depend on many factors, e.g., the gate material, the thickness of the oxide layer, the conductivity type, the doping concentration of the p-well or the bulk, the temperature, and the channel length, that is the distance between the two n-doped regions of the source terminal 412.2 and of the drain terminal 412.1; further, it is known that the threshold voltage may scale as a function of the difference Vin,j−VBn,j. Because of this, the necessary threshold voltage may increase with an increasing difference VSS,j−VBn,j. Nevertheless, even at very high differences VSS,j−VBn,j, which might imply large values of the aj, e.g., aj ranging between 1.5 and 2, an input signal may pass through the nMOS transistor M2301.2. This is because the threshold voltages in the case Vin,j−VBn,j>0 may still be in the ballpark of a few 100 mV. The signal 301.4 at the output of the nMOS transistor M2301.2 may be, e.g., an attenuated or distorted input signal Vin,j. According to the second embodiment of the disclosure, the output signal 301.4 of the nMOS transistor M2301.2 might be brought to a voltage VT,j 308 that makes sure that the nMOS transistor M4303.2 blocks. For this, VT,j 308 may be equal to or higher than the control voltage, Vg,j, indicating the blocking of the double transmission gate, e.g., VT,j=VSS,j or VT,j>VSS,j. In one example of the present embodiment, it may be sufficient to choose one single VT,j 308 for all double transmission gates, e.g., VT=VT,j=VSS,j+ε=VSS+ε, wherein ε may be a small positive real number, typically, e.g., ε equals a few 100 mV. In another alternative, εj=(VDD,j−VSS,j)/2, which sets VT to the middle between VDD,j and VSS;j. The values chosen for the VT,j 308 may depend on several factors, e.g., the control voltages Vg,j indicating the blocking of the nMOS transistors, the claimed accuracy of the output signal 103 with respect to an input signal 112.1, 112.2, 112.3, . . . , 112.n. For the purpose of adjusting the voltage at the input 303.3 of the nMOS transistor M4303.2 a transistor 419 might be used. It may be activated, that is, be set into the conduction direction, when the control voltage, Vg,j, indicates a blocking of the double transmission gate. The transistor 419 serves as a variable resistor: in the case that Vg,j indicates the blocking of the double transmission gate 300, a corresponding base voltage is applied to the transistor which implies that the transistor acts as a low-ohmic resistor (with a resistance that may typically be a few Ohms to kilo-Ohms). Therefore, the input 303.3 to the second transmission gate 303 substantially lies at the potential VT,j 308 which is applied to one terminal of the transistor 419. The voltage difference that drops off at the transistor 419 may be corrected for by choosing the e introduced above accordingly. In this case, the current that is passed through the nMOS transistor M2301.2 may flow off the transistor 419. By the use of, e.g., a transistor M5309, to set the voltage at the input 303.3 of the nMOS M4303.2 to a predetermined value, the nMOS transistor M4303.2 is blocking. The transistor M5309 may be used as a controllable switch; when this switch is closed, the connection line between the output 301.4 of the first transmission gate and the input 303.3 of the second transmission gate is at the potential VT,j 308, when the switch is open, the output signal 301.4 is unalteredly passed to the input 303.3. Because of VT,j=Vg,j or VT,j>Vg,j, wherein Vg,j indicates the blocking control voltage, the drain region 414.1 is at an equal potential as or at a higher potential than the gate voltage Vg,j, and therefore no inversion channel might be created, and, hence, no signal, e.g., voltage or current, is forwarded to the source 414.2 of the nMOS transistor M4303.2.
Turning now to the pMOS structures 420, analogous considerations apply as for the nMOS structure 410. The pMOS structures 420 may be implanted into the n-doped substrate that may comprise the n-well(s) and corresponding nMOS structures 410 as described above, or the pMOS structures 420 may comprise one or more n-wells 421 that are diffused into a substrate. The source regions 421.1, 423.1 and drain regions 421.2 and 423.2 of the pMOS transistors M1301.1 and M3303.1 may, thus, be implanted in the n-doped substrate or in the one or more n-wells.
In the case that the control voltage, Vg,j, is chosen such as to indicate the blocking of the double transmission gate 300, e.g., Vg,j=VSS,j, the gate terminals 425, 426, of the pMOS transistors M1301.1 and M3303.1 are set, by means of an inverter comprised by the double transmission gate, to corresponding voltages
The n-doped substrate or the n-well(s) 421 of the pMOS structure 420 may be connected to one or more charge pumps 501, whereby a typical charge pump has already been described above in relation to the first embodiment of the disclosure, and will, thus, be referred to without being repeated here again. This allows to set the n-well(s) 421 of the pMOS structures 420 comprised by the multiplexer 101 to voltages that may be higher than extreme input voltages Vin,j,high*. For way of example, if present, each n-well of the pMOS structures 421 might be set to a different value. Alternatively, all n-wells (if more than one is present) 421 of all pMOS structures 420 may be pumped to the same voltage, e.g., to the highest of the voltages Vin,j,high*. It should be noted that the values aj given above, might be related to the corresponding Vin,j,high*, that is, e.g., through VBp,j==VDD,j+aj·Udiode.
As explained above in relation to the nMOS structure 410, there may exist a second source of parasitic conduction. Once the n-doped substrate or the n-well(s) 421 lie at a higher potential than the gate terminal 425, depending on the voltage at the input line 301.3 a p-conducting inversion channel might develop through the pMOS transistor M1301.1. Such an inversion channel may develop when the input voltage Vin,j applied at the source terminal 421.1 of the pMOS transistor M1301.1 is a threshold voltage, Uth,p,j, higher than the voltage at the gate, Vg,j, 425. The threshold voltage, Uth,p,j, may depend on the factors given above in relation to the nMOS structure 410; further, it is known that the threshold voltage may scale as a function of the difference VBp,j−Vin,j. Because of this, the necessary threshold voltage, Uth,p,j, may increase with an increasing difference VBp,j−DD,j. Nevertheless, even at very high differences VBp,j−VDD,j, which might imply large values of the aj, e.g., aj ranging between 1.5 and 2, an input signal may pass through the pMOS transistor M1301.1. This is because the threshold voltages in the case VBp,j−Vin,j>0 may still be in the ballpark of a few 100 mV. The signal 301.4 at the output of the pMOS transistor M1301.1 may be, e.g., an attenuated or distorted input signal Vin,j.
According to the second embodiment of the disclosure, a transistor M5309 may be connected to the connection between the first transmission gate 301 and second transmission gate 303. As detailed out above in relation to the nMOS structure 410, a transistor M5″ 429 may serve as a switch or variable resistance. It should be noticed, that one transistor might be sufficient, that is, M5′ 419 is the same as M5″ 429. In the case that the control voltage, Vg,j, indicates a blocking of the double transmission gate 300, e.g., Vg,j=VSS,j, than the transistor becomes very low-ohmic (resistance of typically a few Ohms to kilo-Ohms) and brings the connection between the output 301.4 of the first transmission gate and the input 303.3 of the second transmission gate to the voltage VT,j 308 described above with respect to the nMOS structure 410. As long as VT,j is 308 chosen in the range from VSS+ε to VDD−ε (ε as indicated above), the pMOS structure 420 may not develop a p-conducting inversion channel, because the gate terminal 426 is, in the case of the blocking, at a voltage
To summarize the blocking of the double transmission gate 300 according to the second embodiment of the disclosure, the use of, e.g., at least one charge pump to bring the p-well(s) 411 of an nMOS structure 410 to a potential that is at least a diode drop voltage lower than the negative supply voltages, VSS,j, and to bring the n-doped substrate or the n-well(s) 421 of the pMOS structure 420 to a potential that is at least a diode drop voltage higher than the positive supply voltage, VDD,j, in addition to transistors 309 that may adjust the potential at the input line 303.3 of the second transmission gate 303, may eliminate both unwanted bipolar conduction due to the immanent bipolar transistor structures 417.1, 417.2, 427.1 and 427.2, and the weak conduction due to the creation of conducting inversion channels through the MOS structures.
Now, the conduction of the double transmission gate 300 is described. In this case, the transistor M5309 or the transistors M5′ 419 and M5″ 429 are switched off, that is, the transistors M5309, M5′ 419 and M5″ 429 are extremely high-ohmic (resistances of typically, e.g., a several giga-Ohms) such that the output signal 301.4 of the first transmission gate 301 is unalteredly passed to the input 303.3 of the second transmission gate 303. The conduction of the double transmission gate is indicated by a corresponding control voltage, Vg,j, e.g., Vg,j=VDD,j; in some alternatives of the second embodiment of the disclosure it may be desirable to choose all Vg,j equal, e.g., Vg=Vg,j=VDD,j=VDD. Consequently, the gate terminals 415 and 416 of the nMOS transistors M2301.2 and M4303.2 may then also be at the potential Vg,j, and the gate terminals 425 and 426 of the pMOS transistors M1301.1 and M3303.1 may be at the potential
The analog multiplexer according to the second embodiment of the disclosure may, in one embodiment, comprise a plurality of n of the above-described double transmission gates 300, e.g., implanted on a single substrate, as outlined above, one or more charge pumps 501, and at least n transistors that might be laid out on the same or a different substrate. According to the second embodiment of the disclosure it is possible to implant the transmission gates comprised by the double transmission gates of the analog multiplexer on a single p- or n-doped well. Because of this, the multiplexer extends over a significantly smaller area as it would, if each MOS structure were implanted in an individual well. Therefore, it is possible to achieve smaller structures, e.g., in microcontroller and/or microchip design. This is accomplished by bringing the well(s) to a lower or higher potential with respect to minimal or maximal input voltages. This may, in one embodiment, be accomplished by the use of a single charge pump.