GB2310941A - Bipolar multiplier - Google Patents

Bipolar multiplier Download PDF

Info

Publication number
GB2310941A
GB2310941A GB9704931A GB9704931A GB2310941A GB 2310941 A GB2310941 A GB 2310941A GB 9704931 A GB9704931 A GB 9704931A GB 9704931 A GB9704931 A GB 9704931A GB 2310941 A GB2310941 A GB 2310941A
Authority
GB
United Kingdom
Prior art keywords
transistors
pair
output
multiplier
voltage
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Withdrawn
Application number
GB9704931A
Other versions
GB9704931D0 (en
Inventor
Katsuji Kimura
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
NEC Corp
Original Assignee
NEC Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by NEC Corp filed Critical NEC Corp
Publication of GB9704931D0 publication Critical patent/GB9704931D0/en
Publication of GB2310941A publication Critical patent/GB2310941A/en
Withdrawn legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06GANALOGUE COMPUTERS
    • G06G7/00Devices in which the computing operation is performed by varying electric or magnetic quantities
    • G06G7/12Arrangements for performing computing operations, e.g. operational amplifiers
    • G06G7/16Arrangements for performing computing operations, e.g. operational amplifiers for multiplication or division
    • G06G7/163Arrangements for performing computing operations, e.g. operational amplifiers for multiplication or division using a variable impedance controlled by one of the input signals, variable amplification or transfer function

Description

BIPOLAR MULTIPLIER The present invention relates to a multiplier circuit for multiplying two input signals and more particularly, to a bipolar multiplier having an improved linearity within a wide input voltage range, which is preferably formed on a bipolar semiconductor integrated circuit device (it), and which is operable at a low supply voltage.
A conventional bipolar multiplier is shown in Fig. 1, which was disclosed in the Japanese Examined Patent Publication No. 55-19444 published in 1980.
In rig. 1, two bipolar transistors Q111 and Q112 whose emitters are coupled together constitute a differential amplifier.
The coupled emitters of the transistors Q111 and Q112 are connected through an emitter resistor to a first end of a constant current sink 101 sinking a constant current I. A second end of the current sink 101 is connected to the ground.
Two bipolar transistors Q113 and Q114 whose emitters are coupled together constitute another differential amplifier. The coupled emitters of the transistors Q113 and Q114 are connected through an emitter resistor to the first end of the constant current sink 101.
Collectors of the transistors Qlll and Q114 are coupled together to be connected to a first output terminal 102. Collectors of the transistors Q112 and Q113 are coupled together to be connected to a second output terminal 103.
Four bipolar transistors Ills, Q116, Q117, and Q118 constitute a voltage-current (V-I) converter for converting 2 first input signal voltage V1 into four input signal currents proportional to the voltage V1. These four bipolar transistors Q115, Q116, Q117, and 4118 further supply the input signal currents thus generated to the transistors Qlll, Q112, Q113, and Q114, respectively.
Emitters of the bipolar transistors Q115 and Q116 are coupled together to be connected through an emitter resistor to a first end of a constant current sink 104 sinking a constant current I1. A second end of the current sink 104 is connected to the ground. Emitters of the bipolar transistors Q117 and Q118 are coupled together to be connected through an emitter resistor to the first end of the constant current sink 104.
Bases of the transistors Q115 and Q116 are coupled together. Bases of the transistors Q117 and Q118 are coupled together. The first input signal voltage V1 is applied across the coupled bases of the transistors Q115 and Q116 and those of the transistors Q117 and Q118.
A collector of the transistor Q115 is connected to a base of the transistor Q111. A collector of the transistor Q116 is connected to a base of the transistor Q113. A collector of the transistor Q117 is connected to a base of the transistor Q112.
A collector of the transistor Q118 is connected to a base of the transistor Q114.
Four bipolar transistors Q119, Ql20 Q121, and 4122 serve to apply a second input signal voltage V. to the transistors Qlil, Q112, Q113, and Q114, respectively.
Emitters of the transistors Q119, Q120, Q121, and Q122 are connected to the bases of the transistors Q111, Q112, Q113, and Q11t, respectively. Bases of the transistors Q119 and Q120 are coupled together. Bases of the transistors Q121 and Q122 are coupled together. The second input signal voltage V is applied across the coupled bases of the transistors Q119 and Q120 and those of the transistors Q121 and Q122. Collectors of the transistors Q119, Q120, Q121, andQ122 areappliedwith apowersupplyvoltage.
In Fig. 1, the character x denotes the rate of the constant current I1 flowing through the emitter resistor for the transistors Q115 and Q116. Similarly, the character y denotes the rate of the constant current 12 flowing through the emitter resistor for the transistors Q111 and Q112. The rates of x and y vary dependent upon the applied first and second input signal voltages V, and Vz, respectively.
In this case, the currents flowing through the transistors Q111, Q112, Q113, Q114, Q115, Q116, Q117, and Qlla are expressed as shown in Fig. 1, respectively, where a and b are positive constants. / Here, the collector current ayI: is defined as I, i.e., ayI2 = I*, and the current yI2 flowing thorough the emitter resistor for the transistors Q111 and Q112 is defined as I, i.e., yIw = I3. Then, Ic = (1 - x)I@ is established.
This means that the output current I@ of the differential amplifier comprised of the transistors Q111 and Q112 is independent of the input current (x/2)I1 and that it varies dependent upon the rate x only. Therefore, the output current Ic has a linear characteristic and no temperature dependence.
The same reason is applicable to the differential amplifier comprised of te transistors Q113 and Q114.
As a result, the conventional bipolar multiplier of Fig.
1 is capable of multiplication of the first and second input signal voltages V and V2.
However, the Japanese Examined Patent Publication No.
55-19444 only disclosed the current distribution in the conventional multiplier of Fig. I as the explanation about the circuit analysis. Therefore, the circuit operation of the conventional multiplier of Fig. 1 is extremely difficult to understand. The reason is that the current distribution is not clear in each of the differential pairs of the transistors Q111 and Q112 and Q113 and Q114; in other words, the circuit analysis in the conventional multiplier of Fig. 1 is not based on the physical principle of the bipolar transistors.
Further, the transistors Q'11, Q112, Q113, and Qllt are driven by the single constant current sink 101 and therefore, the subcircuitcomprisedof the transistors Q111, Q112, Q113, andQ114 may be termed the "quadritail cell" or "multiplier core". The circuit analysis of this "quadritail cell" or "multiplier core" is extremely difficult, because of the existence of the emitter resistors.
With reference to an article written by the inventor, Ximura, IEICE Trans. Fundamentals, Vol. E78-A, No. 5, pp. 560 565, issued in May 1995, entitled "A Bipolar Very Low-Voltage Multiplier Core Using a Quadritail Cell", it is certain that the conventional multiplier of Fig. 1 is capable of the multiplication behavior of the first and second input signal voltages V1 and Vz, as disclosed in the japanese Examined Patent Publication No.
55-19444.
However, the conventional multiplier of Fig. 1 does not have the satisfactory linearity in multiplication behavior.
On the other hand, a multiplier is an essential, basic function block in analog signal applications. Recently, fabrication processes for large-scale integrated circuit devices (LSIs) have been becoming finer and finer pandas a result, the supply voltage for the LSIs has been decreasing from S V to 3 V, or lower. This tendency has been increasing the necessity for the low-voltage circuit technique more and more.
Accordingly, an object of at least the preferred embodiments of the present invention is to provide a multiplier capable of completely linear operation within the entire operable input range with respect to one of two input signals to be multiplied.
Another such object is to provide a multiplier capable of completely linear operation within the entire operable input range with respect to both input signals to be multiplied.
Still another such object is to provide a multiplier capable of operation at a low power supply voltage such as approximately 1.9 V with respect to at least one of two input signals to be multiplied.
The above objects together with others not specifically mentioned will become clear to those skilled in the art from the following description.
In a first aspect, the present invention provides a bipolar multiplier comprising: a quadritail cell formed by emitter-coupled first, second, third, and fourth bipolar transistors adapted to be driven by a single constant current source/sink; collectors of said first and fourth transistors being coupled together to form a first output terminal; said first and fourth transistors constituting a differential pair; collectors of said second and third transistors being coupled together to form a second output terminal; said second and third transistors constituting another differential pair; a voltage to current convertor for converting an applied first input voltage into a first pair of output currents and a second pair of output currents;; a first transistor pair of fifth and sixth bipolar transistors adapted to be driven respectively by said first pair of output currents to generate a first pair of output voltages; and a second transistor pair of seventh and eighth bipolar transistors adapted to be driven respectively by said second pair of output currents to generate a second pair of output voltages; bases of said fifth and seventh transistors and bases of said sixth and eighth transistors being adapted to receive a second input voltage applied thereacross; bases of said first and fourth transistors of said quadritail cell being adapted to receive said first pair of output voltages differentially applied thereacross; bases of said second and third transistors of said quadritail cell being adapted to receive said second pair of output voltages differentially applied thereacross;; whereby an output of said multiplier comprising the result of multiplying said first and second input voltages is derivable from at least one of said first and second output terminals.
According to a preferred embodiment of this first aspect of the present invention, a bipolar multiplier is provided.
This multiplier includes (a) a quadritail cell formed by emitter-coupled first, second, third, and fourth bipolar transistors driven by a single constant current sourcefsink, (b) a voltage-current (V-I) converter for converting an applied first initial input voltage to a first pair of output currents and 2 second pair of output currents, (c) a first transistor pair of fifth and sixth bipolar transistors driven by the first pair of output currents, and generates a first pair of output voltages, respectively, and (d) a second transistor pair of seventh and eighth bipolar transistors driven by the second pair of output currents, and generates a second pair of output voltages, respectively.
Collectors of the first and fourth transistors of the quadritail cell are coupled together to form a first output terminal. The first and fourth transistors constitute a differential pair.
Collectors ol the second and third transistors of the quadritail cell are coupled together to form a second output terinl. The second and third transistors constitute another differential pair.
A second initial input voltage is applied across bases of the fifth and seventh transistors and across bases of the sixth and eighth transistors, respectively.
The first pair of output voltages from the first transistor pair of fifth and sixth transistors are differentially applied across bases of the first and fourth transistors of the quadritail cell.
The second pair of output voltages from the second transistor pair of seventh and eighth transistors are differentially applied across bases of the second and third transistors of the quadritail cell. An output of the multiplier including the multiplFcation result of the first and second initial input voltages is derived rom at least one of the first and second output terminals.
With the multiplier according to the first aspect of the present invention, a first input voltage is converted to the first pair of differential output currents and the second pair of differential output currents by the voltage-current converter.
The first transistor pair of fifth and sixth transistors are respectively driven by the first pair of differential output currents thus generated. The second transistor pair of seventh and eighth transistors are respectively driven by the second differential output currents thus generated. A second input voltage is applied across bases of the fifth and seventh transistors and across bases of the sixth and eighth transistors, respectively.
Thus, the first pair of output voltages, which are generated by the first transistor pair of fifth and sixth transistors, have a value proportional to an arc hyperbolic tangent (tanh-l) of the first initial input voltage. The second pair of output voltages, which are generated by the second transistor pair of seventh and eighth transistors, have a value proportional to an tanh1 of the first input voltage.
On the other hand, the first and fourth transistors of the quadritail cell, which constitute a differential transistor pair, has a hyperbolic tangent (tanh) transfer characteristic with respect to the differentially-applied first pair of output voltages. Similarly, the second and third transistors of the quadritail cell, which constitute another differential transistor pair, has a tanh transfer characteristic with respect to the differentially-applied second pair of output voltages.
Therefore, the first initial input voltage is tanh1- converted by the voltage-current converter, and then, it is tanh-converted by the differential pair of the first and fourth transistors of the quadritail cell and by the differential pair of the second and third transistors thereof.
Because the output of the multiplier including the multiplication result of the first and second initial input voltages is derived from at least one of the first and second output terminals, the multiplication operation of the multiplier according to the first aspect is completely linear with respect to the first initial input voltage.
This means that this multiplier is capable of completely linear operation within the entire operable input range with respect to one cf two input signals to be multiplied.
Further, the tanh-l conversion of the first input voltage is performed with the use of the V-I converter, the first transistor pair of the fifth and sixth transistors, and the second transistor pair of the seventh -and eighth transistors.
Accordingly, the necessary power supply voltage can be decreased, resulting in that the multiplier according to the first aspect is operable at 2 low supply voltage such as approximately 1.9 V.
In a preferred embodiment of the multiplier according to the first aspect, the V-I converter includes a differential pair of ninth and tenth bipolar transistors and an emitter resistor connected to emitters of the ninth and tenth transistors.
In this case, it is preferred that the V-I converter further includes first and second current mirror circuits. The first pair of output currents and the second pair of output currents are derived through the first and second current mirror circuits, respectively.
It is preferred that each of the first and second current mirror circuits has an emitter-folloer bipolar transistor.
In another preferred embodiment of the multiplier according to the first aspect, the V-I converter includes a differential pair of ninth and tenth bipolar transistors and serially-connected first and second emitter resistors. The first and second emitter resistors are connected to emitters of the ninth and tenth transistors, respectively.
In still another preferred embodiment of the multiplier according to the first aspect, the V-I converter includes a differential pair of ninth and tenth bipolar transistors and a differential pair of eleventh and twelfth bipolar transistors connected in parallel, and serially-connected first and second emitter resistors. The first and second emitter resistors are connected to emitters of the ninth and tenth transistors and emitters of the eleventh and twelfth transistors, respectively.
In a second aspect, the present invention provides a bipolar multiplier comprising: a quadritail cell formed by emitter-coupled first, second, third and fourth bipolar transistors adapted to be driven by a single constant current source/sink; collectors of said first and fourth transistors being coupled together to form a first output terminal; said first and fourth transistors constituting a differential pair; collectors of said second and third transistors being coupled together to form a second output terminal; said second and third transistors constituting another differential pair; a first voltage to current converter for converting an applied first input voltage into a first pair of output currents and a second pair of output currents;; a first transistor pair of fifth and sixth bipolar transistors adapted to be driven by said first pair of output currents respectively to generate a first pair of output voltages; and a second transistor pair of seventh and eighth bipolar transistors adapted to be driven by said second pair of output currents respectively to generate a second pair of output voltages; a second voltage to current converter for converting an applied second input voltage to a third pair of output currents; a third transistor pair of ninth and tenth bipolar transistors adapted to be driven by said third pair of differential output currents respectively to generate a third pair of output voltages; bases of said first and fourth transistors of said quadritail cell being adapted to receive said first pair of output voltages differentially applied thereacross;; bases of said second and third transistors of said quadritail cell being adapted to receive said second pair of output voltages differentially applied thereacross; bases of said fifth and sixth transistors and bases of said seventh and eighth transistors being adapted to receive said third pair of output voltages differentially applied thereacross; an output of said multiplier comprising the multiplication result of said first and second initial input voltages being derivable from at least one of said first and second output terminals.
According to a preferred embodiment of this second aspect of the present invention, another bipolar multiplier is provided, which is equivalent to one obtained by adding (e) another V-I converter for converting the applied second initial input voltage to a third pair of output currents, and (f) a third transistor pair of ninth and tenth bipolar transistors driven by the third pair of output currents, and generate a third pair of output voltages, respectively.
The third pair of output voltages from the third transistor pair are differentially applied across bases of the fifth and sixth transistors and across bases of seventh and eighth transistors.
With the multiplier according to the second aspect of the present invention, the second initial input voltage is converted to the third pair of differential output currents by the corresponding V-I converter. The third transistor pair of ninth and tenth transistors are respectively driven by the third pair cf differential output currents thus generated.
Thus, the third pair of output voltages, which are generated by the third transistor pair of ninth and tenth transistors, have a value proportional to an tanh of the second initial input voltage.
Therefore, because of the same reason as that of the first initial input voltage, the multiplication operation of the multiplier according to the second aspect is completely linear with respect to the second initial input voltage also.
This means that this multiplier is capable of completely linear operation within the entire operable input ranges with respect to both of two input signals to be multiplied.
Further, since the tanh1 conversion of the second initial input voltage is performed with the use of the corresponding V-I converter and the third transistor pair of ninth and tenth transistors, the necessary power supply voltage can be decreased.
As a result, the multiplier according to the second aspect is operable at a low supply voltage such as approximately 1.9 V with respect to the first and second initial input voltages.
In the multiplier according to the second aspect, the first V-I converter may be configured in the same way as that of the first aspect. I In a preferred embodiment of the multiplier according to the second aspect, the second V-I converter includes a differential pair of eleventh and twelfth bipolar transistors and an emitter resistor connected to emitters of the . The first and second emitter resistors are connected to emitters of the eleventh and twelfth bipolar transistors, respectively.
In another preferred embodiment of the multiplier according to the second aspect, the second V-I converter includes a differential pair of eleventh and twelfth bipolar transistors and a differential pair of thirteenth and fourteenth bipolar transistors connected in parallel, and serially-connected first and second emitter resistors. The first and second emitter resistors are connected to emitters of the eleventh and twelfth transistors and emitters of the thirteenth and fourteenth transistors, respectively.
Preferred features of the present invention will now be described, purely by way of example only, with reference to the accompanying drawings, in which: Fig. 1 is a circuit diagram of a conventional bipolar multiplier.
Fig. 2 is a circuit diagram of a bipolar multiplier according to a first embodiment of the present invention.
Fig. 3 is a circuit diagram of a bipolar multiplier according to a second embodiment of the present invention.
Fig. 4 is a circuit diagram of a voltage-current converter used in the multiplier according to the first and second embodiments.
Fig. 5 is a graph showing the measured dc transfer characteristics of the voltage-current converter shown in Fig.
4.
Fig. 6 is a graph showing the measured dc transfer characteristics of the bipolar multiDlier according to the second embodiment of Fig. 4.
Fig. 7 is a circuit diagram of a bipolar multiplier according to a third embodiment of the present invention.
Fig. 8 is a circuit diagram of a bipolar multiplier according to a fourth embodiment of the present invention.
Fig. 9 is a circuit diagram of a bipolar multiplier according to a fifth embodiment of the present invention Fig. 10 is a circuit diagram of a bipolar multiplier according to a sixth embodiment of the present invention.
A bipolar multiplier according to a first embodiment is shown in Fig. 2.
As shown in Fig. 2, this multiplier includes a quadritail cell 10, a voltage-current (V-I) converter circuit 11, a balanced transistor pair 13 comprised of npn bipolar transistors Q5 and Q5', and a balanced transistor pair 14 comprised of npn bipolar transistors Q6 and Q6'.
The quadritail cell 10 is formed by four npn bipolar transistors Q1, Q2, Q3, and Q4 whose emitters are coupled together to be connected to one end of a constant current sink 1 sinking a constant current Io. The other end of the current sink 1 is connected to the ground. The emitter areas of the transistors Q1, Q2, Q3, and Q4 are equal to each other.
The transistors Q1 and Qo constitute a differential transistor pair, and the transistors Q2 and Q3 constitute another differential transistor pair. Therefore, it can be said that the quadritail cell 10 is a combination of these two differential transistor pairs connected in parallel.
Bases of the transistors Q1 and Q4 are connected to emitters of the transistors Q5 and Q6 of the first transistor pair 13, respectively. Bases of the transistors Q2 and Q3 are connected to emitters of the transistors Q6' andQ5' of the second transistor pair 14, respectively.
Collectors of the transistors Ql and Q4 are coupled together to be connected to a load resistor 3 with a resistance R. The other end of the resistor 3 is applied with a power supply voltage Vcc. In other words, the collectors of the transistors Q1 and Q4 are coupled together to be applied with the power supply voltage Vcc through the load resistor 3, respectively.
Collectors of the transistors Q2 and Q3 are coupled together to be connected to a load resistor 4 with the same resistance RL as that of the resistor 3. The other end of the resistor 4 is applied with the power supply voltage Vc. In other words, the collectors of the transistors Q2 and Q3 are coupled together to be applied with the power supply voltage Vcc through the load resistor 4, respectively.
A first output terminal S is connected to the connection point of the resistor 3 and the coupled collectors of the transistors Qi and Q4. A second output terminal T6 is connected to the connection point of the resistor 4 and the coupled collectors of the transistors Q2 and Q3.
The V-I converter circuit 11 has first and second input terminals T1 and T2 and first, second, third, and fourth output terminals gila, lib, ilc, and lld. A first input signal voltage V is applied across the input terminals T1 and T2. The first output terminal ila is connected to the emitter of the transistor QS and the base of the transistor Q1. The second output terminal llb is connected to the emitter of the transistor Q5' and the base of the transistor Q3 The third output terminal lic is connected to the emitter of the transistor Q6 and the base of the transistor Q4.The fourth output terminal lid is connected to the emitter of the transistor Q6' and the base of the transistor Q2.
The V-I converter circuit 11 generates a first pair of differential output currents proportional to the applied first input signal voltage V, and a second pair of differential output currents proportional to the applied first input signal voltage Vx.
When the first pair of differential output currents are defined as Ix+ and I,-, where Ix+ and Ix- have the same current value and opposite polarities, the second pair of differential output currents can be expressed as I. and I..
The output current Ix' of the first pair flows into the converter circuit 11 through the first output terminal Ila. The output current Ix Ix- of the first pair flows into the converter circuit 11 through the second output terminal llb. The output current Ix+ of the second pair flows into the converter circuit 11 through the third output terminal lic. The output current Ix of the second pair flows into the converter circuit 11 through the fourth output terminal lid. If Bases of the transistors Q5 and Q6 of the first transistor pair 13 are coupled together to be connected to a third input terminal T3.Bases of the transistors Q5' and Q6' of the second transistor pair 14 are coupled together to be connected to a fourth input terminal T4. A second input signal voltage V is applied across the third and fourth input terminals T3 and T4.
A positive electrode of a constant voltage source 2 supplying a constant voltage Vp is connected to the fourth input terminal T4. A negative electrode of the voltage source 2 is connected to the ground. Thus, the constant voltage VR is superposed on the second input signal voltage Vy as a bias voltage, and applied across the third and fourth input terminals 3 and T".
Collectors of the transistors Q5, Q5', Q6, and Q6' are applied with the power supply voltage V-c, respectively.
The transistors Q5 and Q6 o the first transistor pair 13 are driven by the first pair of differential output currents I- and I?? of the V-I converter 11, respectively. The transistors Q5' and Q6' of the second transistor pair 14 are driven by the second pair of differential output currents Ix+ and I of the V-I converter 11, respectively.
Next, the operation of the bipolar multiplier according to the first embodiment is explained in detail below.
Here, supposing that thebase-widthmodulation (i.e., the Early voltage) is ignored, a collector current Ic of a unit bipolar transistor is typically expressed as the following equation (1).
BE IC = IS exp ## (1) VT In the equation (1), VSE is the base-to-emitter voltage of the transistor, and Is is the saturation current thereof. Vr is the thermal voltage defined as Vr = kT/a, where k is the Boltzmann '5 constant, T is absolute temperature in degrees Kelvin, and q is the charge of an electron.
In the following analysis, for the sake of simplification, it is supposed that the common-base current gain factor of the transistor is approximately equal to unity and therefore, the base current can be ignored.
The differential output currents Ix and Ix are proportional to the first input signal voltage V, they can be expressed as the following equations (2) and (3), respectively.
Ix+=I0x+GxVx (2) Ix-=I0x-GxVx (3) where I0x is a constant and 2Gx is the conductance of the v-I converter circuit 11.
From the equations (2) and (3), the difference #Ix of the differential output currents Ix+ and Ix is expressed as #Ix=Ix±Ix-=2GxVx (4) On the other hand, since the transistors Q5 and Q6 of the first transistor pair 13 are driven by the first pair of differential output currents I and Ix-, respectively, the following equations (5) and (6) are established by using the above equation (1)
where Ic5 and ICG are the collector currents of the transistors Q5 and Q6, and VBE5 and VBE6 are the base-to-emitter voltages thereof, respectively.
Similarly, since the transistors OS' and Q6' of the second transistor pair 14 are driven by the second pair of differential output currents It and I;, respectively, the following equations (7) and (8) are established by using the above equation (1)
where I, and 1C6' are the collector currents of the transistors Q5' and Q6', and VBE5' and VBE6' are the base-to-emitter voltages thereof, respectively.
The base-to-emitter voltages Vs.-s and VBE6 serves as a first pair of differential output voltages of the first transistor pair 13 of the transistors Q5 and Q6. The base-to-emitter voltages VBE5' and VeKS serves as a second pair of differential output voltages of the second transistor pair 14 of the transistors Q5' and Q6' If the common emitter voltage of the quadritail cell 10 is defined as Ve, the base-to-emitter voltages VBE1, VBE2, VSE3, and VBE4 of the transistors Q1, Q2, Q3, and Q4 of the quadritail cell 10 are expressed as the following equations (9), (10), (11), and (12), respectively.
VBE1=VR+VY-VBE5 Iox+GxVx (9) =VR+VY-VT#ln##-VE IS VBE2=VR-VBE6' I0x-GxVx (10) =VR-VT#ln##-VE IS VBE3=VR-VBE5 Iox+GxVx (11) =VR-VT#ln##-VE is VBE4=VR+Vy-VBE6 Iox-GxVx (12) =VR+Vy-VT#ln##-VE IS Accordingly, by using the above equations (1) and (9) to (12), the collector currents Ic1, Ic2, Ic3, and Icr of the transistors Q1, Q2, Q3, and Q4 are expressed as the following equations (13), (14), (15), and (16), respectively.
Since the transistors Q1, Q2, Q3, and Q4 are driven by the common constant current sink 1, the following equation (17) is established Ic1+Ic2+Ic3+Ic4=αFIo (17) where aF is the common-base current gain factor.
Here, the differential output current Al of the multiplier of Fig. 2 is defined as the difference between the first output current Ior (= Ic1 + Icr) and the second output current Io2 (= Ic2 + Ic2), i.e., #I = (Ic1 + Ic4) - (Ic2 + Ic3) Then, by substituting the above equations (13), (14), (15), and (16) into the equation (17), the differential output current #I of the multiplier of Fig. 2 is expressed as the following equation (18=) #I=(Ic1+Ic4)-(Ic2+Ic3)
The equation (18a) can be approximated to the following equation (18b) as
where |Vy| 2VT.
It is seen from the equation (18b) that the differential output current Al includes the multiplication result of the first and second input signal voltages Vx and Vy and that the multiplication behavior is completely linear with respect to the first input signal voltage Vx.
Additionally, one of the first output current Ioi (= Ici T Ic4) and the second output current Io2 (= 1c2 + Ic3) may be used as an output of the multiplier of Fig. 2, because each of them contains the multiplication result as shown in the following equations (lSc) and (18d).
Io1=(Ic1+Ic4)
The bipolar multiplier according to the first embodiment of Fig. 2 is applicable, for example, to a frequency mixer, where the local signal input requires no completely linear behavior and the radio-frequency signal input requires the completely linear behavior. In this case, the first input signal voltage V is used as the radio-frequency signal input and the second input signal V, is used as the local signal input. / Additionally, if first and second output voltages are defined as Vo1 and Vo@, respectively, V01 and Vo are expressed as Vo1 = Io1#RL, and Vo2 = Io2#RL.
A differential output voltage #Vo is defined as AV; = V01 - VO2 = RL#(Io1 - Io2) With the bipolar multiplier according to the first embodiment of FIg. 2, the first input signal voltage Vx is converted to the first pair of differential output currents Ix+ and Ix@ and the second pair of differential output currents Ix+ and Ix- by the voltage-current converter circuit 11.
The transistors Q5 and Q6 forming the first transistor pair 13 are respectively driven by the first pair of differential output currents Ix+ and Ix thus generated. The transistors QS' and Q6' forming the second transistor pair 14 are respectively driven by the second pair of differential output currents Ix+ and Ix thus generated.
Further, the first pair of output voltages of the transistor pair 13 are differentially applied across the bases of the transistors Q1 and Q4. Similarly, the second pair of output voltages of the transistorsQ5' and Q6' are differentially applied across the bases of the transistors Q3 and Q2.
From the above equaticn (4), it is seen that the difference Al of the differential output currents Ix+ and I=. does not contain any hyperbolic tangent (tanh) term of V This means that the V-I converter circuit 11 has a tanh function characteristic. Thus, each of the output voltages is proportional to a value of an tanh of the first input signal voltage V.
Therefore, the tanh transfer characteristic of the quadritail cell 10 are canceled by the tanh-1 characteristic or the first and second pair of output voltages, respectively.
As a result, the multiplication operation of the multiplier according to the first embodiment of Fig. 2 is completely linear with respect to the first input voltage Vx. This means that this multiplier is capable of completely linear operation within the entire operable input range with respect to one of two input signals to be multiplied.
Additionally, since the tanh-1 conversion of the first input voltage V is performed with the use of the V-I converter circuit 11 and the first transistor pair 13 of the transistors Q5 and Q6, and the second transistor Fair 14 of the transistors Q5' and Q6', the necessary power supply voltage can be decreased.
As a result, the multiplier according to the first embodiment is operable at a low supply voltage such as approximately 1.9 V.
Next, the V-I converter circuit 11 is explained in detail below.
Fig. 4 shows an example of the VJI converter circuit 11 used in the multiplier according to the first embodiment of Fig.
2. In Fig. 4, this V-I converter circuit 11 has a balanced differential pair of npn bipolar transistors 421 and Q22 whose emitter areas are equal to each other.
Emitters of the transistors Q21 and Q22 are coupled together through a common emitter resistor R21 having a resistance R. The emitter of the transistor Q21 is further connected to the ground through a first current mirror circuit 21 formed by npn bipolar transistors Q23, Q25, Q26, and Q29. The emitter of the transistor Q22 is further connected to the ground through a second current mirror circuit 22 formed by npn bipolar transistors Q24, Q27, Q28, and Q30.
Each of the first and second current mirror circuits 21 and 22 is here a type of an emi.ter-'ollower-âucmented current mirror. It is needless to say that any other type of current mirror circuits may be used.
The first and second current mirror circuits 21 and 22 serve as active loads of the transistors Q21 andQ22, respectively.
The first pair of differential output currents with the same current value Ix+ are derived from the first current mirror circuit 21. The second pair of differential output currents with the same current value Ix- are derived from the second current mirror circuit 22.
A collector of the transistor Q21 is applied with a power supply voltage Vce through a constant current source 21 supplying a constant current Io:(. The transistor Q21 is driven by the constant current Io.
A collector of the transistor Q22 is applied with the same power supply voltage Vc, through a constant current source 22 supplying the same constant current Iox as that of the current source 21. The transistor Q22 is driven by the constant current lox.
A base of the transistor Q21 is connected to the input terminal T1. Abase of the transistor Q22 is connected to the input terninal-T2. A first input voltage V is differentially applied across the input terminals T1 and T2.
A current i will flow through the emitter resistor R21 according to the value of the first input voltage Vx.
In the first current mirror circuit 21, bases of the transistors Q23, Q25, and Q26 are coupled together. Emitters of the transistors Q23, Q25, and Q26 are connected to the ground.
A collector of the transistor Q23 is connected to the emitter of the transistor Q21. Collectors of the transistors Q25 and Q26 are connected to the first and second output terminals lla and llb, respectively. The transistor Q29 serves as an emitter-follower transistor.
In the second current mirror circuit 22, bases of the transistors Q2t, Q27, and Q28 are coupled together. Emitters of the transistors Q24, Q27, and Q28 are connected to the ground. A collector of the transistor Q24 is connected to the emitter of the transistor Q22. Collectors of the transistors Q27 and Q28 are connected to the third and fourth output terminals llc and lld, respectively. The transistor Q30 serves as an emitter-follower transistor.
The emitter areas of the transistors Q23, Q24, Q25, Q26, Q27, Q28, 029, and Q30 are equal to each other.
With the V-I converter circuit shown in Fig. 4, since the transistors Q21 and Q22 are driven by the same constant current I, the base-to-emitter voltages VBE21 and VBE22 are equal to each other, thereby shifting the voltages at the input terminals Tl and T2 by the equal voltages VBE21 and VBE22, respectively. Therefore, the first input signal voltage V is applied across the emitter resistor R21. This means that the emitter resistor R21 serves as a "floating resistor".
Accordingly, the current i s expressed as @x i= (19) Rx Thus, the output currents Ix+ and Ix- outputted from the first and second current mirror circuits 21 and 22 are given by the following equations (20) and (21), respectively.
Vx Ix+=Iox+i=Iox+ (20) Rx Vx Ix-=Iox-i=Iox- (21) Rx If the conductance of (1/Rx) is defined as Gx in the equations (20) and (21), the above equations (2) and (3) are obtained.
It is seen from the equations (20) and (21) that the linearity of the V-I converter circuit 11 is dominantly determined by the linearity of the emitter resistor R21.
With the V-I converter circuit 11 shown in Fig. 4, the transistors Q21 and Q22 constituting the differential pair are respectively driven by the corresponding constant current sources 21 and 22, respectively. Therefore, the voltage applied across the emitter resistor R21 is equal to the first input voltage V3, which means that the resistor R21 is equivalent to a "floating resistor".
Also, the current i flowing through the resistor R21 is taken out with the use of the first and second current mirror circuits, without logarithmical compression nor exponential expansion. As a result, a completely1 or perfectly linear conversion operation can be obtained within a specific voltage range of the input voltage V. with a simple circuit configuration.
Further, no circuit for logarithmical compression and exponential expansion is required and therefore, the necessary power supply voltage Vcc can be decreased. Thus, the converter circuit 11 of Fig. 4 is operable at a low supply voltage such as approximately 1.9 V.
Fig. 5 shows the dc transfer (V-I) characteristics of the converter circuit Ilof Fig. 4, which was obtained by inventor's tests. In Fig. 5, the differential output current of the circuit 11 is indicated in voltage. The testing condition is as follows.
The power supply voltage Vice is 1. 9V, the driving current I,, i5 approximately 50 A, the load resistance is 18 kQ. The voltage applied across the resistor R21 is 1.4V.
It is seen from Fig. S that the linear input voltage range is approximately equal to 600 mVp-p, and that the Total Harmonic Distortion (THD) at 1 kHz of the frequency of Vx is equal to 0.1 % or less.
A bipolar multiplier according to a second embodiment is shown in Fig. 3, which is equivalent to one obtained by adding a second V-I converter 12 for converting the applied second input voltage Vy to a third pair of differential: ontput currents Iy' and Iy-, and a third transistor pair 15 of npn bipolar transistors Q7 and Q8 driven by the third pair of differential output currents Iy+ and I,-, respectively.
Therefore, the description relating to the same configuration is omitted here by adding the same reference numerals/characters as those in the multiplier according to the first embodiment of Fig. 2 for the sake of simplification of description.
The second V-I converter circuit 12 has the third and fourth input terminals T3 and T4 and fifth and sixth output terminals l2aandl2b. The second input signal voltage Vïisapplied across the input terminals T3 and T4. The fifth output terminal 12a is connected to the emitter of the transistor Q7 and the bases of the transistors QS' and Q6'. The sixth output terminal 12b is connected to the emitter of the transistor Q8 and the bases or the transistors Q.
The second V-I converter circuit 12 generates the third pair of differential output currents proportional to the applied second input voltage V The third pair of differential output currents are expressed as Iy+ and 17, where I,+ and Iy- have opposite polarities.
The output current Iy of the third pair flows into the second converter circuit 12 through the fifth output terminal 12a.
The output current I of the third pair flows into the second converter circuit 12 through the sixth output terminal 12b.
An emitter of the transistor Q7 is connected to the bases of the transistors Q5' and Q6'of the second transistor pair 14.
An emitter of the transistor Q8 is connected to the bases of the transistors Q5 and Q6 of the first transistor pair 13. Collectors of the transistors Q7 and Q8 are applied with a power supply voltage Vcc' . Bases of the transistors Q7 and Q8 are coupled together to be applied with the power supply voltage Vcc'.
The transistors Q7 and Q8 of the third transistor pair 15 are driven by the third pair of differential output currents It and Iy-, respectively. Therefore, the following equations (22) and (23) are established in the same way as that of the transistors Q5 and Q6
where Ict and Is are the collector currents of the transistors Q7 and Q8, VBE7 and VBE8 are the base-to-emitter voltages thereof, respectively, loy is a constant, and 2Gy as a conductance of the second V-I converter circuit 12.
From the equations (22) and (23), the difference Alp of the differential output currents IN, and Iy- is expressed as #Iy=Iy±Iy-=2GyVy (24) Then, in the similar way as that of the first embodiment, the differential output current Al of the multiplier of Fig. 3 is expressed as the following equation (25) #I=(Ic1+Ic4)-(Ic2+Ic3)
It is seen from the equation (25) that the differential output current Al includes the multiplication result of the first and second input signal voltages V and Vy, and that the multiplication behavior is completely linear with respect to both of the first and second input signal voltage Vx and Vy.
With the bipolar multiplier according to the second embodiment of Fig. 3, since the second input uoltage V, is converted to the third pair of differential output currents Iy+ and Iy-, the third differential output voltage has a value proportional to an tanh-1 of the second initial input voltage. The tanh-1-converted second input voltage Vy is then differentially inputted into the quadritail cell through the first transistor pair of the transistors Q5 and Q6 and the second transistor pair of the transistors Q5' and Q6'.
As a result, the multiplication operation of the multiplier according to the second embodiment is completely linear with respect to the first and second input voltages V and Vy. This means that this multiplier is capable of completely linear operation within the entire operable input range with respect to both two input signals to be multiplied.
Further, the tanh; conversion of the first and second input voltages Vx and Vy are performed with the use of the first and second V-I converter circuits 11 and 12, and the first transistor pair of the transistors Q5 and Q6, the second transistor pair of the transistors Q5' and Q6', and the third transistor pair of the transistors Q7 and Q8. Consequently, the multiplier according to the second embodiment is operable at low supply voltage such as approximately 1.9 V for Vcc and 2.8 V for Vcc'.
Fig. 6 shows the dc transfer (V-I) characteristics of the multiplier according to the second embodiment of Fig. 3 with V as a parameter where Vy = 0, t 200 mV, or + 400 mV, which was obtained by inventor's tests. In Fig. 6, the differential output current of the multiplier is indicated In voltage The testing condition is as follows.
The power supply voltage Vcc is 1.9 V, Vcc' is 2.8 V, the driving current Iax is approximately 100 WA, the load resistance R; is 8.2 kQ.
It is seen from Fig. 6 that the multiplication operation of the multplier according to the second embodiment is completely linear with respect to the first and second input voltages Vx and Vy, thereby realizing an ideal multiplication characteristics.
It is preferred that the V-I converter circuit 11 in the multiplier according to the first embodiment of Fig. 2 is capable of completely-linear multiplication operation. However, if the circuit configuration is drastically simplified, the linear operation may be degraded until a level where the severe iinearity is not necessary during the practical operation.
A bipolar multiplier according to a third embodiment of Fig. 7 is applicable to such cases.
The multiplier according to a third embodiment of Fig.
7 has the same configuratIon as that of the multiplier according to the first e.Ebodiment of Fig. 2, except for the configuration of the V-I converter 11. Therefore, for the sake of simplification, the description relating to the same configuration is omitted here by adding the same reference numerals/characters as those in the multiplier according to the first embodiment of Fig. 2.
As shown in Fig. 7, the V-I converter 11 includes a differential pair of npn bipolar transistors Q37 and Q38, and another differential pair of npn bipolar transistors Q39 and Q40 connected in parallel to the different~ial pair of the transistors Q37 and Q38.
Emitters of the transistors Q37 and Q38 are coupled together through a common emitter resistor R31 with a resistance Rx. Emitters of the transistors Q39 and Qa0 are coupled together through the common emitter resistor R31. The resistor R31 serves to expand the lInear input voltage range of V due to the emitter degeneration.
The coupled emitters of the transistors Q37 and Q39 are connected to the ground through a constant current sink 31 sinking a constant current 2iso. The transistors Q37 and Q39 are driven by the current sink 31. The coupled emitters of the transistors Q38 and Qt0 are connected to the ground through a constant current sink 32 sinking the same constant current 21oX as that of the current sink 31. The transistors Q38 and Q0 are driven by the current sink 32.
The first input signal voltage Vx is applied across bases of the transistors Q37 and Q38 and across the bases of the transistors Q39 and Q40 through the first and second input terminals T1 and T2.
A collector of the transistor Q37, which serves as the first output terminal lla, is connected to the emitter of the transistor Q5. A collector of the transistor Q40, which serves as the third output terminal llc, is connected to the emitter of the transistor Q6. A collector of the transistor 439, which serves as the second output terminal Ila, is connected to the emitter of the transistor QS'. A collector of the transistor Q38, which serves as the fourth output terminal 1lid, is connected to the emitter of the transistor Q6' With the multiplier according to the third embodiment of Fig. 7, the transistors Q37, 438, Q39, and Q40 constituting the respective differential pairs have the V-I conversion function and the tanh-? conversion function and therefore, the same advantage as those in the first embodiment is obtained, except that the linearity of the multiplication operation is approximately equal to that of the well-known Gilbert multiplier using the well-knohn Gilbert gain cell as the predistortion circuit.
A bipolar multiplier according to a fourth embodiment is shown in Fig. 8, which is the same in configuration as the multiplier according to the third embodiment of Fig. 7, except for the configuration of te V-I converter 11.
As shown in Fig. 8, the V-I converter 11 includes a differential pair of npn bipolar transistors Q47 and 448, and another differential pair of npn bipolar transistors Q49 and QS0 connected in parallel to the differential pair of the transistors Q47 and Q48.
Emitters of the transistors Q47 and Qa8 are coupled together through two common emitter resistors R41 and R42 with a same resistance R. The resistors R41 and R42 are connected in series. Emitters of the transistors Qu9 and Q50 are coupled together through the common emitter resistors R41 and R42. The resistors R41 and R42 serve to expand the linear input voltage range of Vx due to the emitter degeneration.
The connection point of the resistors R41 andR42 is connected to the ground through a constant current sink 41 sinking a constant current 4Iox. The transistors Q37, Q38, Q39, and B40 are driven by the common current sink 41.
The first input signal voltage Vx is applied across bases of the transistors Q47 and Q48 and across the bases of the transistors Q49 and Q50 through the first and second input terminals T1 and T2.
A collector of the transistor Q97, which serves as the first output terminal Ila, is connected to the emitter of the transistor Q5. A collector of the transistor QS0, which serves as the third output terminal llc, is connected to the emitter of 1/ the transistor G6. Collector of the transistor Q49, which serves as the second output terminal lla, is connected to the emitter of the transistor Q5'. A collector of the transistor Q48, which serves as the fourth output terminal Ild, is connected to the emitter of the transistor Q6'.
With the multiplier according to the fourth embodiment of Fig. 8, the transistors Q47, Q48, Q49, and Q50 constituting the respective differential pairs have the V-I conversion function and the tanh~l conversion function and therefore, the same advantage as those in the first embodiment is obtained. The linearity of the multiplication operation is approximately equal to that of the well-known Gilbert multiplier using the well-known Gilbert gain cell as the predistortion circuit with respect to the first and second input signal voltages V and Vy.
A bipolar multiplier according to a fifth embodiment is shown in Fig. 9, which corresponds to one obtained by adding the second V-I converter circuit 12 and the third transistor pair 15 to the multiplier according to the third embodiment of Fig. 7.
In other words, the bipolar multiplier according to the fifth embodiment of Fig. 9 corresponds to one where the first and second V-I converter circuits 11 and 12 in the multiplier according to the second embodiment of Fig. 3 are embodied.
Specifically, the second V-I /,converter circuit 12 includes a differential transistor pair of npn bipolar transistors Q51 and Q52, and a common emitter resistor Ras1. The third transistor pair 15 is formed by npn bipolar transistors Q7 and Q8.
Fn emitter of the transistor Q51 is connected to the ground through a constant current sink 51 sinking a constant current 21o An emitter of the transistor Q52 is connected to the ground through a constant current sink 52 sinking the same constant current 2Io as that of the current sink 51. The emitters of the transistors Q51 and Q52 are coupled together through the emitter resistor R51.
The transistors Q51 and Q52 are driven by the same constant currents 2IC, respectively. The resistor R51 serves to expand the linear input voltage range of V4 due to the emitter degeneration.
Bases of the transistors Q51 and Q52 are connected to the third and fourth input terninals T3 and Ta., respectively. The second input voltage Vy is applied across the bases of the transistors through the terminals T3 and T4.
A collector of the transistor Q51 is connected to an emitter of the transistor Q7 of the third transistor pair 15. A collector of the transistor Q52 is connected to an emitter of the transistor Q8 of the third transistor pair 15.
With the multiplier according to the fifth embodiment of Fig. 9, the transistors QS1 and Q52 constituting the second V-I converter circuit 12 have the V-I conversion function and the tanh'' conversion function and therefore, the same advantage as those in the third embodiment of Fig. 7 is obtained.
The inearity of the multiplication operation is approximately equal to that of the well-known Gilbert multiplier using the well-known Gilbert gain cell as the predistortion circuit with respect to both of the first and second input voltages Vx and Vy.
A bipolar multiplier according to a sixth embodiment is shown in Fig. 10, which corresponds to one obtained by adding the second V-I converter circuit 12 and the third transistor pair 15 to the multiplier according to the fourth embodiment of Fig. 8.
In other words, the bipolar multiplier according to the sixth embodiment of Fig. 10 corresponds to one where the first and second V-I converter circuits 11 and 12 in the multiplier according to te second embodiment of Fig. 3 are embodied.
Specifically, the second V-I converter circuit 12 includes a differential transistor pair of npn bipolar transistors QEl and Q62, and common emitter resistors R61 and R62.
The third transistor pair 15 is formed by npn bipolar transistors Q7 and Q8.
Emitters of the transistors Q61 and Q62 are coupled together through serially-connected emitter resistors R61 and R62.
The connection point of the resistors R61 and R62 is connected to the ground through a constant current sink 61 sinking a constant current 4Ioy. The transistors Q61 and Q62 are driven by the same constant current 4Ioy respectively. The resistors R61 and R62 serve to expand the linear input voltage range of V due to the emitter degeneration.
Bases of the transistors Q61 and Q52 are connected to the third and fourth input terminals T3 and T4, respectively. The second input voltage V7 is applied across the bases of the transistors Q61 and Q62 through the terminals T3 and T4.
A collector of the transistor Q61 is connected to an emitter of the transistor Q7 of the third transistor pair 15. A collector of the transistor Q62 is connected to an emitter of the transistor Q8 of the third transistor pair 15.
With the multiplier according to the sixth embodiment of Fig. 10, the transistors Q61 and Q62 constituting the second V-I converter circuit 12 have the V-I conversion function and the tanh~l conversion function and therefore, the same advantage as those in the fourth embodiment of Fig. 8 is obtained.
The linearity of the multiplication operation is approximately equal to that of the well-known Gilbert multiplier using the well-known Gilbert gain cell as the predistortion circuit with respect to both of the first and second input voltages V and Vy.
While the preferred forms of the present invention have been described, it is to be understood that modifications will be apparent to those skilled in the art without departing from the invention. The scope of the invention, therefore, is to be determined solely by the following claims.
Each feature disclosed in this specification (which term includes the claims) and/or shown in the drawings may be incorporated in the invention independently of other disclosed and/or illustrated features.
The text of the abstract filed herewith is repeated here as part of the specification.
A bipolar multiplier is provided, which is capable of completely linear operation with respect to at least one of two input voltages to be multiplied. A quadritail cell is formed by emitter-coupled first to fourth bipolar transistors driven by a single constant current source/sink. A voltage-current converter is provided for converting an applied first input voltage to first and second pairs of differential output currents. A first transistor pair of fifth and sixth bipolar transistors are driven by the first pair of differential output currents, respectively. A second transistor pair of seventh and eighth bipolar transistors are driven by the second pair of differential output currents, respectively. A second input voltage is applied across bases of the fifth and seventh transistors and across bases of the sixth and eighth transistors, respectively. An output of the multiplier including the multiplication result of the first and second input voltages is differentially derived from the first and second output terminals.

Claims (13)

1. A bipolar multiplier comprising: a quadritail cell formed by emitter-coupled first, second, third, and fourth bipolar transistors adapted to be driven by a single constant current source/sink; collectors of said first and fourth transistors being coupled together to form a first output terminal, said first and fourth transistors constituting a differential pair; collectors of said second and third transistors being coupled together to form a second output terminal, said second and third transistors constituting another differential pair; a voltage to current convertor for converting an applied first input voltage into a first pair of output currents and a second pair of output currents; a first transistor pair of fifth and sixth bipolar transistors adapted to be driven respectively by said first pair of output currents to generate a first pair of output voltages; and a second transistor pair of seventh and eighth bipolar transistors adapted to be driven respectively by said second pair of output currents to generate a second pair of output voltages; bases of said fifth and seventh transistors and bases of said sixth and eighth transistors being adapted to receive a second input voltage applied thereacross; bases of said first and fourth transistors of said quadritail cell being adapted to receive said first pair of output voltages differentially applied thereacross; bases of said second and third transistors of said quadritail cell being adapted to receive said second pair of output voltages differentially applied thereacross; whereby an output of said multiplier comprising the result of multiplying said first and second input voltages is derivable from at least one of said first and second output terminals.
2. A multiplier as claimed in Claim 1, wherein said voltage to current converter includes a differential pair of ninth and tenth bipolar transistors and an emitter resistor connected to emitters of said ninth and tenth transistors.
3. A multiplier as claimed in Claim 2, wherein said voltage to current converter further includes first and second current mirror circuits, said first pair of output currents and said second pair of output currents being derivable through said first and second current mirror circuits, respectively.
4. A multiplier as claimed in Claim 3, wherein each of said first and second current mirrors includes an emitter follower bipolar transistor.
5. A multiplier as claimed in Claim 1, wherein said voltage to current convertor includes a differential pair of ninth and tenth bipolar transistors and serially-connected first and second emitter resistors, said first and second emitter resistors being connected to emitters of said ninth and tenth transistors, respectively.
6. A multiplier as claimed in Claim 1, wherein said voltage to current convertor includes a differential pair of ninth and tenth bipolar transistors, a differential pair of eleventh and twelfth bipolar transistors connected in parallel, and serially-connected first and second emitter resistors, said first and second emitter resistors being connected to emitters of said ninth and tenth transistors and emitters of said eleventh and twelfth transistors, respectively.
7. A bipolar multiplier comprising: a quadritail cell formed by emitter-coupled first, second, third and fourth bipolar transistors adapted to be driven by a single constant current source/sink; collectors of said first and fourth transistors being coupled together to form a first output terminal; said first and fourth transistors constituting a differential pair; collectors of said second and third transistors being coupled together to form a second output terminal; said second and third transistors constituting another differential pair; a first voltage to current converter for converting an applied first input voltage into a first pair of output currents and a second pair of output currents; a first transistor pair of fifth and sixth bipolar transistors adapted to be driven by said first pair of output currents respectively to generate a first pair of output voltages; and a second transistor pair of seventh and eighth bipolar transistors adapted to be driven by said second pair of output currents respectively to generate a second pair of output voltages; a second voltage to current converter for converting an applied second input voltage into a third pair of output currents; a third transistor pair of ninth and tenth bipolar transistors adapted to be driven by said third pair of differential output currents respectively to generate a third pair of output voltages; bases of said first and fourth transistors of said quadritail cell being adapted to receive said first pair of output voltages differentially applied thereacross; bases of said second and third transistors of said quadritail cell being adapted to receive said second pair of output voltages differentially applied thereacross;; bases of said fifth and sixth transistors and bases of said seventh and eight transistors being adapted to receive said third pair of output voltages differentially applied thereacross; an output of said multiplier comprising the result of multiplying said first and second input voltages being derivable from at least one of said first and second output terminals.
8. A multiplier as claimed in Claim 7, wherein said first voltage to current converter includes a differential pair of ninth and tenth bipolar transistors and an emitter resistor connected to emitters of said ninth and tenth transistors.
9. A multiplier as claimed in Claim 8, wherein said first voltage to current converter further includes first and second current mirror circuits, said first pair of output currents and said second pair of output currents being derivable through said first and second current mirror circuits respectively.
10. A multiplier as claimed in Claim 9, wherein each of said first and second current mirrors includes an emitter follower bipolar transistor.
11. A multiplier as claimed in Claim 7, wherein said first voltage to current converter includes a differential pair of eleventh and twelfth bipolar transistors and serially-connected first and second emitter resistors, wherein said first and second emitter resistors being connected to emitters of said eleventh and twelfth transistors, respectively.
12. A multiplier as claimed in Claim 7, wherein said first voltage to current converter includes a differential pair of eleventh and twelfth bipolar transistors, connected in parallel, and serially-connected first and second emitter resistors, said first and second emitter resistors being connected to emitters of said ninth and tenth transistors and emitters of said eleventh and twelfth transistors, respectively.
13. A bipolar multiplier substantially as herein described with reference to and as shown in any of Figures 2, 3, 7, 8, 9 and 10 of the accompanying drawings.
GB9704931A 1996-03-08 1997-03-10 Bipolar multiplier Withdrawn GB2310941A (en)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
JP8077696 1996-03-08
JP8312988A JP2888212B2 (en) 1996-03-08 1996-11-08 Bipolar multiplier

Publications (2)

Publication Number Publication Date
GB9704931D0 GB9704931D0 (en) 1997-04-30
GB2310941A true GB2310941A (en) 1997-09-10

Family

ID=26421751

Family Applications (1)

Application Number Title Priority Date Filing Date
GB9704931A Withdrawn GB2310941A (en) 1996-03-08 1997-03-10 Bipolar multiplier

Country Status (3)

Country Link
JP (1) JP2888212B2 (en)
AU (1) AU712618B2 (en)
GB (1) GB2310941A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2003009078A2 (en) * 2001-07-17 2003-01-30 Infineon Technologies Ag Multiplier circuit

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5994959A (en) * 1998-12-18 1999-11-30 Maxim Integrated Products, Inc. Linearized amplifier core
CN108872747B (en) * 2018-06-27 2023-07-04 南京信息工程大学 Surge protector resistive current extraction device and method based on correlation coefficient

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5019444A (en) * 1973-06-20 1975-02-28

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5019444A (en) * 1973-06-20 1975-02-28

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2003009078A2 (en) * 2001-07-17 2003-01-30 Infineon Technologies Ag Multiplier circuit
WO2003009078A3 (en) * 2001-07-17 2003-04-03 Infineon Technologies Ag Multiplier circuit
US7026857B2 (en) 2001-07-17 2006-04-11 Infineon Technologies Ag Multiplier circuit

Also Published As

Publication number Publication date
GB9704931D0 (en) 1997-04-30
JPH09298423A (en) 1997-11-18
JP2888212B2 (en) 1999-05-10
AU1518897A (en) 1997-09-11
AU712618B2 (en) 1999-11-11

Similar Documents

Publication Publication Date Title
US6111463A (en) Operational transconductance amplifier and multiplier
AU719000B2 (en) Differential circuit and multiplier
US4560920A (en) Voltage to current converting circuit
EP0196906B1 (en) Automatic gain control detection circuit
KR100304773B1 (en) Window camparator
GB2272090A (en) Analog multiplier
JPS60146511A (en) High speed multilication digital/analog converter
GB2310941A (en) Bipolar multiplier
KR20030057278A (en) Gain control circuit for controlling a gain in a variable gain cell
US4352057A (en) Constant current source
JPH0770935B2 (en) Differential current amplifier circuit
GB2301214A (en) Bipolar multiplier
US5463309A (en) Variable voltage to current conversion circuit
US6265909B1 (en) Three-valued switching circuit
US4529946A (en) Differential amplifier circuit
US5977760A (en) Bipolar operational transconductance amplifier and output circuit used therefor
US5796243A (en) Current multiplier/divider circuit
KR100307834B1 (en) Voltage-current converter
KR930007795B1 (en) Amp circuit operable at low power amplification
US6198333B1 (en) Analog multiplier with thermally compensated gain
JP3022339B2 (en) Multiplier
JP2900879B2 (en) Bipolar multiplier
JPH02244309A (en) Fine current source
GB2316785A (en) Analog multiplier
US20030094989A1 (en) Multiplier

Legal Events

Date Code Title Description
WAP Application withdrawn, taken to be withdrawn or refused ** after publication under section 16(1)