1. Field of the Invention
The present invention relates to integrated circuits and more particularly generating a reference signal in integrated circuits.
2. Description of the Related Art
In general, a bandgap reference circuit provides a voltage reference with improved temperature stability and is less dependent on power supply voltage than other known voltage reference circuits. Bandgap reference circuits typically generate a reference voltage approximately equal to the bandgap voltage of silicon extrapolated to zero degrees Kelvin, i.e., VG0=1.205V. Typical voltage reference circuits include a current minor coupled to the power supply and the voltage reference node to provide a current proportional to absolute temperature (i.e., PTAT) to the voltage reference node. These circuits can be made with relatively low cost, but have the disadvantages of being sensitive to mechanical strain and/or aging, which reduces the accuracy of the voltage reference. In addition, typical voltage reference circuits generate PTAT (or equivalent) output currents that vary across temperature, which make those voltage references less useful as standalone current generators. An additional voltage-to-current generator is typically used to stabilize the output current.
Accordingly, improved techniques for generating reference voltages are desired.
Reference signal generators using thermistors are disclosed. In at least one embodiment of the invention, an apparatus includes a first device having a first temperature coefficient and a thermistor having a second temperature coefficient. The second temperature coefficient has a sign opposite to a sign of the first temperature coefficient. The apparatus includes a circuit configured to maintain equivalence of a first signal and a second signal and further configured to offset a first temperature variation of the first device using a second temperature variation of the thermistor to generate the second signal having a low temperature coefficient. The first device may be a bipolar transistor configured to generate a base-emitter voltage. The thermistor may be coupled in series with the bipolar transistor. The first signal may be a first voltage on a first node, and the second signal may be a second voltage on a second node. The circuit may be configured to maintain effective equivalence of the first voltage and the second voltage. The apparatus may include a resistor coupled to the second node and having a third temperature coefficient. The third temperature coefficient may have a magnitude substantially less than a magnitude of the first temperature coefficient and substantially less than a magnitude of the second temperature coefficient. The first signal may be a first current and the second signal may be a second current. The first device may be a metal-oxide-semiconductor field-effect transistor (MOSFET) device coupled to the thermistor and coupled to a second MOSFET device having a different gate-to-source voltage than the first MOSFET device.
In at least one embodiment of the invention, a method includes. maintaining equivalence of a first signal and a second signal. The method includes offsetting a temperature variation of a third signal having a first temperature coefficient using a thermistor having a second temperature coefficient to generate the second signal having a low temperature coefficient. Maintaining equivalence may include generating an indicator of a voltage difference between a first voltage on a first node coupled to a first load including a series combination of the thermistor having a resistivity proportional to temperature and a diode having the first temperature coefficient. The second signal may be a second voltage on a second node coupled to a second load. The method may include adjusting the first and second signals in response to the indicator. The method may include controlling a first current source to generate the first voltage in response to the indicator. The method may include controlling a second current source to generate the second voltage in response to the indicator. The first signal may be a first current and the second signal may be a second current. Offsetting the temperature variation may include using the thermistor to compensate for a difference in gate-to-source voltages of a first metal-oxide-semiconductor field-effect transistor (MOSFET) device and a second MOSFET device.
The present invention may be better understood, and its numerous objects, features, and advantages made apparent to those skilled in the art by referencing the accompanying drawings.
The use of the same reference symbols in different drawings indicates similar or identical items.
A typical bandgap voltage reference utilizes temperature behavior of diodes to generate a voltage having a negative temperature coefficient (i.e., a negative first-order temperature coefficient) and a voltage having a positive temperature coefficient (i.e., a positive first-order temperature coefficient) and combines those voltages to produce an approximately zero temperature coefficient reference voltage. In general, voltage reference circuits take advantage of two electrical characteristics to achieve the desired VREF: the VBE of a bipolar transistor is nearly complementary to absolute temperature, e.g., VBE=(−1.5 mV/°K*T+1.22)V, and VT is proportional to absolute temperature, i.e, VT=kT/q. Although pure diodes are preferable because they generate a higher diode drop for the same current, the typical bandgap voltage reference manufactured in a complementary metal-oxide-semiconductor (CMOS) process uses diode-coupled, bipolar junction transistors (i.e., BJTs or bipolar transistors), which are readily available in a CMOS process (e.g., PNPs for instance are bipolar devices formed from P-diffusion, an N-well, and a P-well in a CMOS process). The voltage across the diodes (or diode-coupled bipolar junction transistors) has a negative temperature coefficient, but the voltage difference between two diode drops in which the current densities differ is proportional to absolute temperature (PTAT). The use of two banks of bipolar junction transistors of different sizes (or two identical banks with different currents) can generate ΔVBE. The typical bandgap forces ΔVBE across a relatively temperature insensitive resistor (e.g., a polysilicon resistor) using negative feedback, which generates a PTAT current through the resistor. Another resistor is placed in series, which amplifies ΔVBE to cancel the negative temperature coefficient of the diode drop.
Referring to
where J1 and J2 are the current densities of corresponding bipolar transistors. Accordingly, voltage reference circuit 100 includes a pair of PNP bipolar transistors (i.e., transistors 106 and 108) that are coupled in a diode configuration (i.e., the collectors and bases of these transistors are coupled together) and coupled to ground. Transistor 108 has an area that is N times larger than the area of transistor 106. Thus, the current densities of transistor 108 and transistor 106 vary by a factor of N. The emitter of transistor 106 is coupled to an inverting input of operational amplifier 116. The emitter of transistor 108 is coupled, via resistor R1, to the non-inverting input of operational amplifier 116. Operational amplifier 116 maintains equivalent voltages at nodes 118 and 120, i.e., V118=V120=VBE106. Hence, the difference between VBE106 and VBE108 (i.e., ΔVBE106,108) forms across resistor R2. Operational amplifier 116 and transistors 102 and 104 convert this voltage difference into a current (i.e., current IPTAT) proportional to the voltage difference:
Since the thermal voltage VT is proportional to absolute temperature via the constant factor k/q, k=1.38*10−23J/K and q=1.6*10−19C, the current proportional to the voltage difference is also proportional to an absolute temperature, i.e., IPTAT is a PTAT current.
Transistor 108 provides a voltage nearly complementary to absolute temperature (i.e., a ‘CTAT’ voltage) because the VBE of a bipolar transistor is nearly complementary to absolute temperature. By compensating the PTAT current with a CTAT voltage, transistors 102, 104, 106, and 108, and resistors R1 and R2, may be appropriately sized to generate a particular reference voltage output having an approximatley zero temperature coefficient:
VREF is approximately equal to, VG0=1.205V, i.e., the bandgap voltage of silicon extrapolated to zero degrees Kelvin.
Adding a PTAT voltage to a diode drop produces an approximately zero temperature coefficient point at approximately 1.2 V, resulting in a circuit that is not substantially sensitive to the effects of process variation on the bipolar junction transistor. The ratiometric manner in which the resistors are used also reduces effects of process variation, aging, and strain sensitivity. However, a noise transfer function of voltage reference circuit 100 is dependent on a ratio of the load resistors. In an exemplary embodiment of the voltage reference, the ratio of R1 to R2 is approximately 5 to 10 (i.e., R1/R2≈5-10), and ΔVBE, which is typically less than 100 mV, is amplified along with its noise by operational transconductance amplifier 116. Operational transconductance amplifier 116 has a feedback factor of R2/(R1+R2), which causes a reduction in loop gain and bandwidth from the open loop gain.
A technique for reducing effects of noise on the reference voltage as compared to noise sensitivity of a reference voltage generated by voltage reference generator 100 includes using a VGS-R topology. For example, the voltage reference generator of
Referring to
Referring to
By making use of thermistors, i.e., resistors that have a resistance that varies substantially with temperature, e.g., PTAT metal resistors and/or PTAT silicided resistors, in the core of the voltage reference generator, only a constant current may be generated and provided to Rthermistor to maintain a zero temperature coefficient on VREF. Accordingly, a voltage-to-current generator that generates a constant current that may be required by other voltage reference generator topologies can be eliminated when there is no need for alterative circuits elsewhere in the system. In addition, since metal and silicide resistors are not piezo-resistive, the associated voltage reference generator response has little or no strain sensitivity. Moreover, aging of these types of metal and silicide resistors is generally superior to alternative integrated circuit resistors, increasing stability of the output voltage as a function of time. Another benefit of embodiments of the VBE-Rthermistor voltage reference generator includes lower noise than conventional voltage reference generator topologies.
Metal resistors are not commonly used in conventional analog circuits and bandgap voltage reference circuits since metal layers in typical CMOS processes are intended to provide low-resistance interconnects and thus have very low sheet resistance. The low sheet resistance (e.g., 60 milli-Ohms per square) requires resistors having large area to implement even small resistances (e.g., 10-20 kilo-Ohms) However, a stack of multiple metal layers coupled by conductive via(s) of a CMOS process may be configured as electrically coupled metal resistors (e.g.,
Referring to
Referring back to
Referring to
Referring to
Circuits 1000 are less sensitive to process variations than the VGS-R topology described above since the threshold voltage does not affect the bias current. In addition, circuit 1000 can operate at a lower supply voltage since 1.2V is not required to produce a bandgap voltage. Circuit 1000 is simpler than other reference generator circuits since the circuit behaves as an amplifier and an operational transconductance amplifier is not required. However the output currents of circuits 1000 may include flicker noise and may be noisier than the output of a VGS-R reference, but not as noisy as a bandgap voltage reference generator. Circuits 1000 are strain insensitive. Note that circuits 1000 do not generate a voltage with a zero temperature coefficient since the constant current that flows through the thermistor results in a temperature dependent voltage. The temperature coefficient of the thermistor should be less than a metal resistors PTAT resistivity. Accordingly, the thermistor may be implemented using a polysilicon resistor in series with a metal resistor to obtain the target temperature coefficient. Note that circuits 1000 and the other self-biased circuits described herein require a startup circuit to prevent the circuit from latching in an off state. Any suitable startup circuit known in the art may be used.
The description of the invention set forth herein is illustrative, and is not intended to limit the scope of the invention as set forth in the following claims. For example, while the invention has been described in an embodiment in which p-type MOSFETs are configured as current sources and a PNP-type bipolar junction transistor is used to generate the VBE, one of skill in the art will appreciate that the teachings herein can be utilized with n-type MOSFETs configured as current sinks and an NPN-type bipolar junction transistor coupled to generate the VBE. In addition, diodes may be stacked to further enhance ΔVBE (e.g., for embodiments including two diodes stacked in series for each bipolar device, ΔVBE becomes VTIn(N2)). Variations and modifications of the embodiments disclosed herein, may be made based on the description set forth herein, without departing from the scope and spirit of the invention as set forth in the following claims.
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