The present invention relates to circuits, and more particularly, to analog circuits to provide a transistor body bias voltage.
Circuits on a die may experience a wide temperature range, where changes in temperature may be both spatial and temporal in nature. This may be of concern in a computer system such as that illustrated in
As operating frequency and transistor integration increase, one or more die used in the computer system of
A temperature change in a transistor, unless compensated for, will change the threshold voltage as well as carrier mobility of the transistor. As temperature decreases, the magnitude of the threshold voltage and carrier mobility increase. This will affect both the OFF (or leakage) current IOFF of the transistor as well as the ON current ION of the transistor. The effect of temperature change on IOFF is more severe than that of ION. But the ratio of ION/IOFF affects performance robustness. Consequently, circuit designers usually try to keep this ratio greater than some minimum value, e.g., on the order of 100 to 1000, by designing a circuit to operate at its worst-case ION/IOFF ratio, corresponding to its expected maximum temperature. But when the temperature is lower than its expected maximum, a circuit designed for its worst-case ION/IOFF ratio will not operate optimally, unless other changes are made to the circuit parameters.
Because carrier mobility increases with decreasing temperature, a circuit designed for its worst-case ION/IOFF ratio may be made to operate faster by increasing its clock frequency to take advantage of the increased carrier mobility. However, even greater gains in circuit operation frequency than this may be realized by modulating the threshold voltage as a function of temperature. This can be accomplished by changing the body biasing of transistors as temperature changes. For example, if no changes in body biasing is made, then as temperature decreases, IOFF decreases significantly due to an increase in the magnitude of the threshold voltage. As a result, unless otherwise compensated for, a circuit will operate at a larger ION/IOFF ratio than necessary. Embodiments of the present invention change the body biasing so as to reduce the magnitude of the threshold voltage when temperature decreases, so that the ION/IOFF ratio may be brought back (or closer) to the design point (worst-case ION/IOFF ratio). The frequency of operation of the circuit may then be increased because of the reduction in the magnitude of the threshold voltage. Therefore, by modulating threshold voltage to maintain a fixed ION/IOFF ratio as temperature changes, the frequency may be maximized for a given temperature.
Embodiments of the present invention generate a body bias voltage to decrease the magnitude of the threshold voltage when temperature decreases, and to increase the magnitude of the threshold voltage when temperature increases. The body bias may be applied to pFETs, nFETs, or both types of transistors. For example, shown in
Preferably, Vbp should be chosen so as to prevent turning ON the parasitic junction diode formed by the source/drain terminals and the n-well. Typically, the body bias voltage is in the range (Vcc−500 mV) to (Vcc+500 mV), where Vcc is the supply voltage. The lower end of the range represents forward body biasing so as to decrease the magnitude of the threshold voltage, whereas the upper end of the range represents reverse body biasing so as to increase the magnitude of the threshold voltage.
In the case of body biasing a nFET, a p+ region is formed in the channel of a nFET to serve as a body terminal. Again, the body bias voltage should be chosen so as to prevent turning ON the parasitic junction diode formed by the source/drain terminals and the p-substrate. Typically, the body bias voltage is in the range (Vss−500 mV) to (Vss+500 mV), where Vss is the ground of the circuit. The lower end of the range represents reverse body biasing so as to increase the magnitude of the threshold voltage, whereas the upper end of the range represents forward body biasing so as to decrease the magnitude of the threshold voltage.
An embodiment circuit for body biasing nFETs is shown in
In general, transistors 312 and 314 need not have the same width or length. However, it is preferable that they have the same length as each other, and the same length as the transistors to be biased, so that ION and IOFF track temperature in the same way. If transistors 312 and 314 do not have the same width, then this should be taken into account when setting the current mirror gains so as to realize the desired ION/IOFF ratio. This will be discussed in more detail later. For the present discussion, assume that transistors 312 and 314 have the same width and length.
The combination of OPAMP 318 and resistors 320 and 322 provide the input-output functional relationship Vbn=(1+R2/R1)V1−(R2/R1)V0, where R2 and R1 are the resistances of resistors 322 and 320, respectively, V1 is the voltage at node 316 (which is the input port of OPAMP 318), and V0 is an offset voltage provided at input port 324. The circuit design parameters R1, R2, and V0, as well as A and B, among others, are chosen so that Vbn is in the range (Vss−500 mV) to (Vss+500 mV).
The significance of the current mirror gains is that the path from node 316 through the amplifier comprising OPAMP 318 and resistors 320 and 322, to the body terminals 308 and 310 of nFETs 312 and 314, respectively, and to node 316 via the current mirrors, comprises a negative feedback loop such that under steady state AION=BIOFF. When steady state is reached, it is also assumed that there is thermal equilibrium, or near thermal equilibrium, locally so that nFETs 312 and 314 are at a well-defined temperature. Thus, A and B are chosen to set the ION/IOFF ratio, that is, under steady state ION/IOFF=B/A. (This assumes that the various current mirrors are operating in their saturation regions so that current mirrors 304 and 306 are providing constant gains A and B, respectively, and that the other circuit parameters, such as R2, R2, V0, etc., are properly chosen.)
To describe the negative feedback, suppose the circuit has stabilized at a constant temperature so that AION=BIOFF. Now suppose there is a sudden decrease in the temperature at nFETs 312 and, 314. This will tend to cause a decrease in ION and a much more significant decrease in IOFF, so that now AION>BIOFF and the ratio ION/IOFF has increased relative to its steady state value. But with current mirror 304 trying to source AION into node 316, and with the current mirror comprising nFEFs 326 and 328 trying to sink BIOFF from node 316, where AION>BIOFF, the voltage at node 316 will rise. But a rise in this voltage at node 316 will cause a rise in Vbn at output port 302, which is fed back to body terminals 308 and 310. This will increase the forward body bias of nFETs 312 and 314. This increase in forward body bias will decrease the effective threshold voltage of nFETs 312 and 314, which will cause an increase in ION and a much more significant increase in IOFF so as to decrease the ratio ION/IOFF.
Thus, with a sudden temperature decrease that causes an increase in ION/IOFF, negative feedback will decrease ION/IOFF. Similar reasoning will show that with a sudden temperature increase that causes a decrease in ION/IOFF, negative feedback will increase in ION/IOFF. Consequently, there is negative feedback such that a change in ION/IOFF is countered by an opposite change in ION/IOFF, and the steady state is AION=BIOFF.
Current mirrors 304 and 306 may be single-stage current mirrors, but they may also each comprise more than one stage in order to achieve ION/IOFF ratios of 100 to 1000. An embodiment of these current mirrors is provided in FIG. 4. Here, the combination of transistors 402, 404, 406, 408, 410, and 412 realize current mirror 304; and the combination of transistors 414 and 416 realize current mirror 306. Note that transistors 418 and 420 could be lumped together with transistors 414 and 416 so that the combination of transistors 414, 416, 418, and 420 realize a current mirror. That is, referring to
An embodiment providing a bias voltage Vbp to bias pFETs is shown in FIG. 5. Current mirror 502 is biased by pFET 504, which has its gate connected to its source to provide a source-drain current IOFF. Current mirror 506 is biased by pFET 508, which has its gate connected to its drain to provide a source-drain current ION. Note that the current mirrors in
Similar reasoning as considered with respect to
Various modifications may be made to the disclosed embodiments without departing from the scope of the invention as claimed below. For example,
As another example of a modification to the disclosed embodiments, programmability may be built into the disclosed circuits to allow tuning under various process conditions. For example, current mirrors 304 and 306 in
As discussed previously, transistors 312 and 314 need not have the same width. For example, we could let ION and IOFF represent the ON-current and leakage current per unit transistor width, respectively. Consider
It is to be understood in these letters patent that the meaning of “A is connected to B” (A and B as used here are phrases, not the current mirror gains) is that A and B are connected by a passive structure for making a direct electrical connection so that the voltage potentials of A and B are substantially equal to each other. For example, A and B may be connected by way of an interconnect, transmission line, etc. In integrated circuit technology, the “interconnect” may be exceedingly short, comparable to the device dimension itself. For example, the gates of two transistors may be connected to each other by polysilicon or copper interconnect that is comparable to the gate length of the transistors.
It is also to be understood that the meaning of “A is coupled to B” is that either and B are connected to each other as described above, or that, although A and B may not be connected to each other as described above, there is nevertheless a device or circuit that is connected to both A and B. This device or circuit may include active or passive circuit elements. For example, A may be connected to a circuit element which in turn is connected to B.
It is also to be understood that the term “current mirror” may include a single stage current mirror, or a multiple stage current mirror.
It is also to be understood that various circuit blocks, such as current mirrors, amplifiers, etc., may include switches so as to be switched in or out of a larger circuit, and yet such circuit blocks may still be considered connected to the larger circuit because the various switches may be considered as included in the circuit block.
Number | Name | Date | Kind |
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6087892 | Burr | Jul 2000 | A |