Abstract:
A temperature compensated low voltage reference circuit can be realized with a reduced operating voltage overhead and reduced spatial requirements This is accomplished in several ways including integrating one or more bipolar junction transistors into a current differencing amplifier and reducing the number of components required to implement various voltage reference circuits. All of the reference circuits may be constructed with various types of transistors including DTMOS transistors.

Description:
BACKGROUND 
       [0001]    1. Field of Invention 
         [0002]    The present invention relates to semiconductor integrated circuits, and more specifically, to a low voltage reference circuit that is capable of outputting a plurality of voltages with minimal operating voltage overhead. 
         [0003]    2. Description of Related Art 
         [0004]    In many devices that incorporate analog, digital, and/or mixed-signal integrated circuits, voltage reference circuits are of critical importance to the proper functioning of the device. For example, circuits such as oscillators, Phase Locked Loops (PLLs), Digital-to-Analog Converters (DACs), and Analog-to-Digital Converters (ADCs), depend on stable, temperature-independent voltage references. As the critical dimensions of integrated circuits have decreased over time, the operating voltages of these integrated circuits have also decreased. With the decrease in operating voltages of integrated circuits, the need for temperature-independent voltage reference circuits with low operating voltages has increased. Many of these voltage reference circuits provide a stable reference voltage output while operating at voltages at or below 1.3V. 
         [0005]    One of the ways to reduce the costs associated with the manufacture of integrated circuits involves limiting the area used to implement circuits within the integrated circuit. In general, circuits that are less complex and require less area to implement are less expensive to manufacture. Further, by reducing the area required to implement some of the circuits within an integrated circuit, it may be possible to reduce the overall size of the integrated circuit, permitting the integrated circuit to be incorporated into smaller devices. 
       SUMMARY 
       [0006]    Disclosed herein are voltage reference circuits that provide temperature compensated voltage outputs with a reduced operational input voltage overhead and may be implemented over a smaller surface area than conventional voltage reference circuits. 
         [0007]    In example embodiments, a current differencing amplifier is incorporated into a voltage reference circuit, wherein Bipolar Junction Transistors (BJTs) that are traditionally constructed as components outside of the current differencing amplifier are incorporated into the current differencing amplifier. In some example implementations, two current mirrors within the current differencing amplifier are modified to include floating BJTs. In such example implementations, the incorporation of BJTs into the current differencing amplifier reduces the space required to implement the particular voltage reference circuit by eliminating the need to construct two BJTs in another portion of the circuit. 
         [0008]    In example implementations of some of the embodiments disclosed herein, a current differencing amplifier with BJTs is incorporated into a voltage reference circuit that is configured to operate at a supply voltage less than the bandgap voltage of the semiconducting material used to construct the voltage reference circuit. 
         [0009]    These as well as other aspects and advantages of the present invention will become apparent to those of ordinary skill in the art by reading the following detailed description, with appropriate reference to the accompanying drawings. 
     
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         [0010]    Preferred embodiments of the present invention are described with reference to the following drawings, wherein: 
           [0011]      FIG. 1  is a schematic drawing of a prior art voltage reference circuit; 
           [0012]      FIG. 2  is a schematic drawing depicting additional details of the prior art voltage reference circuit shown in  FIG. 1 ; 
           [0013]      FIG. 3  is a schematic drawing of a voltage reference circuit in accordance with an aspect of the invention; 
           [0014]      FIG. 4  is a schematic drawing depicting additional details of the voltage reference circuit shown in  FIG. 3 ; 
           [0015]      FIG. 5  is a schematic drawing of a second prior art voltage reference circuit; 
           [0016]      FIG. 6  is a schematic drawing of a second voltage reference circuit in accordance with an aspect of the invention; 
           [0017]      FIG. 7  is a schematic drawing of a third example voltage reference circuit in accordance with an aspect of the invention; 
           [0018]      FIG. 8  is a schematic drawing of a fourth example voltage reference circuit in accordance with an aspect of the invention; 
           [0019]      FIG. 9  is a schematic drawing of a fifth example voltage reference circuit in accordance with an aspect of the invention. 
       
    
    
     DETAILED DESCRIPTION 
       [0020]    In view of the wide variety of embodiments to which the principles of the present invention can be applied, it should be understood that the illustrated embodiments are examples only, and should not be taken as limiting the scope of the present invention. 
         [0021]    Several embodiments of a temperature compensated voltage reference circuit are presented herein. In the embodiments described herein, a current differencing amplifier is incorporated into the voltage reference circuit. In such embodiments, the current differencing amplifier has been constructed such that one or more Bipolar Junction Transistors (BJTs) are integrated into the current differencing amplifier, eliminating the need to construct the integrated BJTs elsewhere in the voltage reference circuits. In some of these embodiments, the area required to implement one of the disclosed voltage reference circuits is smaller than the area required to implement a comparable prior art voltage reference circuit. 
         [0022]    Turning now to the figures,  FIG. 1  is a schematic drawing of a prior art temperature compensated voltage reference circuit  100  similar to a circuit described in U.S. Pat. No. 7,122,997 which is hereby incorporated by reference. The operating voltage for the circuit  100  is marked as V IN    101  and it is applied at the node of the connected sources of transistors M 1    102 , and M 3    103 . As shown in  FIG. 1 , the circuit  100  employs a feedback network comprised of a current-differencing amplifier AR 1   104 . AR 1   104  translates a difference in currents into an output voltage. Those skilled in the art will appreciate that a current differencing amplifier can be made in various ways and is usually designed such that it does not place constraints on the operating voltage, V IN    101 . In circuit  100 , terminals V C1    105  and V C2    106  are usually operated at close to 0V. In general, V C1  and V C2  are usually kept below approximately 0.3V for proper circuit operation at high temperatures. 
         [0023]    The emitter current of transistors Q 1    107 , which is shown as I 1 , and Q 2    108 , which is shown as I 2 , have a designed ratio of p=I 2 /I 1 . In some implementations, this ratio is 1:1 but the ratio p can vary depending on the design of the circuit  100 . The emitter area of both transistors  107  and  108  is also designed to have a ratio given by r=A 1 /A 2 . As a result, transistors Q 1    107  and Q 2    108  have a fixed current density ratio, J 2 /J 1 , that is equal to the product of p and r. 
         [0024]    This circuit produces a reference voltage V REF    110 , which is referenced to ground, in accordance with the equation: V REF =R 3  [(V E2 /R 2 )+(p+1) (V T /R 1 ) ln (p r)], wherein V E2  is the voltage across the base-to-emitter junction of Q 2 , the ratio p=I 2 /I 1 , the ratio r=A 1 /A 2 , and V T =kT/q. 
         [0025]    In the circuit  100 , the temperature coefficient of the reference voltage V REF    110  is controlled by the ratio of a resistor R 2 , marked in  FIG. 1  as  111 , to another resistor R 1 , marked in  FIG. 1  as  112 . The magnitude of the reference voltage V REF    110  is controlled by the value of a resistor R 3 , marked in  FIG. 1  as  113 . Circuit  100  in  FIG. 1  is capable of operating at a supply voltage, V IN    101  that is less than the bandgap voltage of the semiconducting material used to construct the circuit  101 . For example, if the circuit  100  was constructed out of silicon, the circuit  100  would be capable of operating at a supply voltage of less than 1.25V. 
         [0026]    By way of example,  FIG. 2  shows additional details of the voltage reference circuit  100  by assuming a particular implementation of current differencing amplifier  104 . While there are literally hundreds of ways to implement a current differencing amplifier, the amplifier in  FIG. 2 , consisting of three current mirrors, is one of the simplest. In  FIG. 2 , the current differencing amplifier  104  is shown as consisting of three DTMOS current mirrors  201 ,  202 , and  203 . These current mirrors use Dynamic Threshold MOS (DTMOS) transistors to ensure that the amplifier  104  is operational at a supply voltage that is less than the V BE  voltage of transistors  107  and  108 . As such, the amplifier  104  does not limit the potential for low voltage operation of the circuit  100 . As shown in  FIG. 2 , both of the N-type current mirrors  201  and  202  have an area ratio of sqrt(p):1. When constructed in accordance with this ratio, these current mirrors  201  and  202  ensure that the ratio of I 2 /I 1  is p, wherein sqrt(p) 2 =p, when the ratio of the P-type current mirror  203  is 1:1 as also shown in  FIG. 2 . While not depicted in  FIG. 2 , it is also possible to generate this same ratio of I 2 /I 1  by using N-type current mirrors with an area ratio of 1:1 and a P-type current mirror with a ratio of p:1. However, such a configuration may require more area to implement. 
         [0027]      FIG. 3  is a schematic drawing of an example voltage reference circuit  300  in accordance with one aspect of the invention. As shown in  FIG. 3 , the circuit  300  is arranged similarly to the circuit  100  depicted in  FIG. 1  in that the circuit  300  comprises a current differencing amplifier  301  and produces a reference voltage  303  in accordance with the same equation presented above in reference to circuit  100 . However, in the circuit  300 , the transistors  107  and  108 , which were constructed externally to the current differencing amplifier  104  in circuit  100  have been omitted. In the configuration shown in  FIG. 3 , one terminal of resistor R 1    305  is electrically connected to input terminal VB 1   307  of current differencing amplifier  301 . A second terminal of resistor R 1    305  is electrically connected a terminal of resistor R 2    309 , the drain of transistor M 1    311 , and input terminal VB 2  of current differencing amplifier  301 . In the configuration shown in  FIG. 3 , the input transistors of the current differencing amplifier  301  are constructed using bipolar junction transistors rather than MOS transistors or some other input architecture. By using bipolar junction transistors as the input transistors of the current differencing amplifier  301 , it is possible to simplify the overall voltage reference circuit. 
         [0028]    By way of example,  FIG. 4  shows additional details of the voltage reference circuit  300  by presenting a particular implementation of the current differencing amplifier  301 , shown in  FIG. 3 . As shown in  FIG. 4 , one of the current mirrors  402  within the current differencing amplifier  301  has been constructed to incorporate a BJT similar to transistor  107  shown in  FIG. 1 . Also shown in  FIG. 4 , a second current mirror  403  within the current differencing amplifier  301  has been constructed to incorporate a BJT similar to BJT  108  shown in  FIG. 1 . Current mirror  402  is constructed to have an area ratio of r sqrt(p):r, and current mirror  403  is constructed to have an area ratio of 1:1. In this example configuration, the critical transistors, Q 1   404  and Q 2   405 , will have an area ratio of r=A 1 /A 2 . Also shown in  FIG. 4  is a DTMOS current mirror  404 , which is constructed to have an area ratio of sqrt(p):1 in the particular example shown in  FIG. 4 . In other example embodiments of current differencing amplifier  301 , a P-Type current mirror may be constructed to have a current ratio of p:1 and the current mirror  402  may be constructed to have a ratio of r:r. In this implementation of the current differencing amplifier, it is not necessary to use DTMOS transistors in the P-type current mirror if PNP transistors with sufficiently high gain are used. In implementations of the circuit shown in  FIG. 4 , the input NPN current mirrors could also be implemented with DTMOS transistors to reduce the required operating voltage. However, those of skill in the art will appreciate that the bandgap voltages of DTMOS transistors are more highly dependent on process variables and the inclusion of DTMOS transistors may impact the accuracy of the circuit. 
         [0029]    In  FIG. 4 , the current I 3   407  is equal to the sum of three other currents: I 1   409 ,  12   407 , and IR 2   413 . 
         [0000]        I 3 =I 1 +I 2 +IR 2 
         [0000]    Since 12=p I 1 , this is equivalent to the following. 
         [0000]        I 3=(1 +p ) I 1 +IR 2 
         [0000]    The first term, (1+p) I 1 , forms a current that is proportional to absolute temperature (PTAT) and the second term, IR 2 , is proportional to V BE  or complementary to absolute temperature (CTAT). When these two currents are summed in the correct proportions, the temperature dependencies cancel and, to a first order, I 3  is constant with respect to temperature. By applying this constant current to resistor R 3   415 , a constant voltage may be developed across R 3   415  of any arbitrary value; including values less than the bandgap voltages of transistors Q 1   404  and Q 2   405 . In  FIG. 4  this temperature independence (or V REF  flatness) may be optimized by adjusting the values of resistors R 1   417  and/or R 2   419 . Due to process variations, it is often necessary to perform this calibration in high precision voltage references after the circuit  300  is fabricated. In some situations, performing a post-fabrication calibration of resistors in the circuit  300  can be difficult to implement in some commercially available semiconductor manufacturing processes. 
         [0030]    The prior art circuit  500  shown in  FIG. 5  presents one means of addressing the difficulties associated with post-fabrication calibration by separating current IR 2   501  from current I 1   503  and current I 2   505 . In this circuit, a CTAT current I 4   507  is generated by a P-type current mirror composed of transistors M 2   509  and M 4   511  and a PTAT current I 3   513  is generated by another P-type current mirror composed of transistors M 1   515  and M 3   517 . The ratio of I 4   507  to IR 2   501  is controlled by the relative sizes of transistors M 2   509  and M 4   511 . Likewise, the ratio of I 3  to (I 1 +I 2 =(1+p) I 1 ) is controlled by the relative sizes of transistors M 1   515  and M 3   517 . If either or both of these current mirrors is constructed from an array of much smaller transistor segments, it is possible to control the current transfer ratio of one or both of these current mirrors by digital means after chip fabrication. 
         [0031]    In  FIG. 6 , the reference circuit  500  has been modified in accordance with one aspect of the invention to achieve a voltage reference circuit  600 . In circuit  500 , the BJTs  519  and  521  were constructed external to a current difference amplifier  523 . In circuit  600 , transistors similar to BJTs  519  and  521  have been integrated into a current differencing amplifier  601 . The current differencing amplifier  601  may be constructed in accordance with any of a number designs. For example, the design shown in  FIG. 4  may be used as the current differencing amplifier  601 . As shown in  FIG. 6 , a first terminal of resistor R 1   603  is electrically connected to a first input terminal of the current differencing amplifier  601 , and a second terminal of resistor R 1   603  is electrically connected to a second input terminal of the current differencing amplifier  603 . The second terminal of the resistor R 1   603  is also electrically connected to the drain of transistor M 1   605 . 
         [0032]    Similar to  FIG. 5 ,  FIG. 6  depicts two current mirrors, one formed by transistors M 1   605  and M 3   607  and the other formed by transistors M 2   609  and M 4   611 , which can be used to control the ratios of currents within circuit  600  in the same manner transistors  509 ,  511 ,  515 , and  517  control currents within circuit  500 . As shown in  FIG. 6 , currents I 3  and I 4  flow through a resistor R 3   613 , wherein one terminal of resistor R 3   613  is electrically connected to ground. The output voltage Vref  615  can be measured at the node comprising the drain connections of transistors  607  and  611  and the ungrounded terminal of resistor  613 . 
         [0033]    Those of skill in the art will appreciate that the example circuits presented thus far require a start-up circuit. For clarity, such start-up circuits are not shown. 
         [0034]      FIG. 7  depicts an example of a shunt type voltage reference circuit  700  in accordance with another aspect of the invention. The circuit  700  may be used to provide a reference voltage in a wide variety of circuits where a sub-bandgap output voltage is not required. In  FIG. 7 , a PMOS transistor  701  is used as a shunt element, and a resistor  702  is placed in series with the VB 2  input  703  of the current differencing amplifier  704 . 
         [0035]    Those skilled in the art will appreciate that the PMOS transistor  701  could be replaced with a NMOS transistor, a PNP bipolar transistor, a P-type DTMOS (Dynamic Threshold Metal Oxide Semiconductor) or LDMOS (Laterally Diffused Metal Oxide Semiconductor) transistor, or another circuit element. In the configuration shown in  FIG. 7 , a PTAT current flows through the resistor  702 , allowing the circuit to achieve a constant reference voltage rather than a constant current that is translated to a voltage. While  FIG. 7  shows the current differencing amplifier  704  as an inverting amplifier, those skilled in the art will appreciate that the circuit  700  could be configured such that a non-inverting current differencing amplifier could also be used. The source resistance, RS  706 , is required in any practical application but is not a part of the shunt regulator circuit  700 . Unlike other examples described above where additional circuitry, such as start-up circuitry, was omitted for clarity, the shunt regulator of  FIG. 7  is complete. Circuit  700  does not require the start-up circuits that the other circuits require because it is automatically self-starting when power for the current differencing amplifier is derived from either VIN  708  or VREF  710 . 
         [0036]    Circuit  800  shown in  FIG. 8  depicts another aspect of the invention in which a series regulator rather than a shunt regulator is formed. In  FIG. 8 , a PMOS transistor  801  is used as a pass element. While  FIG. 8  depicts a PMOS transistor as the pass element, those skilled in the art will appreciate that many different transistor types may be used as a pass element in circuit  800 , including, for example, PNP bipolar transistors, P-type DTMOS transistors, or P-type LDMOS transistors. Further, circuit  800  could be configured to use N-type or NPN-type transistors as pass elements. As with circuit  700 , a resistor  802  is placed in series with the VB 2  input  803  of the current differencing amplifier  804 . When in use, a PTAT current flows through another resistor  805 , allowing the circuit  800  to achieve a constant reference voltage measured at VREF  806 . As shown in  FIG. 8 , one terminal of the resistor  805  is electrically connected to the VB 1  input  807  of the current differencing amplifier  804 . For simplicity, the start-up circuit for this voltage regulator is not shown in  FIG. 8 . 
         [0037]      FIG. 9  depicts another aspect of the invention in which circuit  900  may be used to perform a shunt regulation function similar to that shown in  FIG. 7 . In this circuit, the value of R 2   902  is doubled compared to the value of resistor  702  in  FIG. 7 , and an NPN transistor  904  between one terminal of the resistor R 2   902  and the Vout connection  906 . In the configuration shown in  FIG. 9 , the NPN transistor  904  acts to double the voltage at which the circuit regulates to two bandgap voltages (2 Vbg=Vbe+2 R 2 +Vbe), or about 2.5 volts for silicon. Those skilled in the art will appreciate that the first Vbe in this equation is the base-emitter voltage of the transistor  904  and the second Vbe is the base-emitter voltage of the transistor inside AR 1  connected to the positive input terminal. In  FIG. 9 , if the VREF input  908  of the circuit  900  is shorted to the VOUT output  906 , then this shunt regulator may be used with an external power supply, VIN, and a series resistor RS, as shown in  FIG. 7 , to form a 2.5 V voltage reference. The circuit of  FIG. 9  may also be used with a two-resistor voltage divider network to provide other values of reference voltage when the midpoint of the two resistors in the voltage divider network are connected to the VREF input  908  and the two ends of the voltage divider are connected to VOUT  906  and ground. The regulated output voltage of this circuit may be calculated from the formula below where a resistor R 1  is the value of the resistor in a voltage divider network that is connected to ground, R 2  is the value of the resistor in a voltage divider network connected to VOUT, and VREF=2 Vbg. 
         [0000]        V OUT= V REF*(1 +R 2 /R 1) 
         [0000]    This can also be done with the shunt regulator of  FIG. 7  but it is more practical to do this with the circuit of  FIG. 9  because the VREF  908  input current required by this circuit  900  (at the base of transistor  908 ) is much less than the input current, (1+p) I 1  required by the circuit of  FIG. 7 . As before with circuit  700 , this circuit does not require a start-up circuit because it is automatically self-starting when power for the current differencing amplifier is derived from either VIN or VOUT. 
         [0038]    All of the transistors in the above embodiments may be fabricated in a variety of ways. Different types of FETs (such as NMOS or PMOS), DTMOS transistors (such as NDTMOS or PDTMOS) or BJTs (such as NPN or PNP) may be implemented to construct alternative embodiments. Those skilled in the art will understand, however, that additional changes and modifications may be made to these embodiments without departing from the true scope and spirit of the present invention, which is defined by the claims.