In the drawings:
FIG. 1 is a diagram of circuitry for receiving binary input signals and for producing output currents representative of such binary input signals;
FIG. 2 illustrates waveforms of voltages and currents produced by the circuitry shown in FIG. 1; and
FIG. 3 is a schematic electrical diagram of a servo system which may be used in conjunction with the circuitry shown in FIG. 1.
FIG. 1 illustrates circuitry for receiving binary input signals and for producing an output current representative of the binary input signals. The circuitry of FIG. 1 is particularly adapted to be used in a digital-to-analog converter. The circuitry shown in FIG. 1 includes an input line 100 for receiving the binary input signals. The input line 100 is connected to the gate of a transistor 102 such as a MOS transistor of the p-type. The drain of the transistor 102 is connected through a line 103 to a reference potential such as ground. The source of the transistor 102 is common with the source of a transistor 104 and with the drain of a transistor 106. The transistors 104 and 106 may be MOS transistors of the p-type.
The source of the transistor 106 receives an energizing potential such as approximately 5 volts. The gate of the transistor 106 receives a substantially constant bias voltage through a circuit which is shown in FIG. 3 and which will be described in detail subsequently. The gate of the transistor 104 receives a suitable biasing voltage such as a voltage of approximately 1.2 volts on a line 108. The output from the circuitry shown in FIG. 1 is produced on a line 110 which is connected to the drain of the transistor 104.
Distributed capacitances 112 (shown in broken lines in FIG. 1) exist between the gate and the source of the transistor 102 and distributed capacitances 114 (shown in broken lines in FIG. 1) exist between the gate and the drain of the transistor. These distributed capacitances are charged during the time that the transistor 102 is nonconductive and they become discharged when the transistor 102 becomes conductive.
In output circuitry of the prior art, the discharge of a distributed capacitance corresponding to the capacitance 112 occurs through a circuit including the source and gate of a transistor and the discharge of a distributed capacitor corresponding to the capacitance 114 occurs through a circuit including the gate and drain of the transistor. However, in the prior art, such a transistor is an n-type rather than being the p-type shown for the transistor 102 in FIG. 1. As a result of the charge and discharge of such distributed capacitances, a current signal on the line 110 in FIG. 1 is produced in the n-type of transistor in the prior art with characteristics such as indicated at 116 in FIG. 2. This signal has a blip 118 which is produced upon a change from a non-conductive state to a conductive state in the operation of the n-type of transistor of the prior art. Similarly, the n-type of transistor corresponding in the prior art to the transistor 102 (p-type in this invention) produces a slow edge 119 when the state of the transistor changes from a conductive to a non-conductive state. This results from the fact that the drain of the transistor in the prior art (corresponding to the transistor 106) must swing over a larger voltage range than this invention requires. The parasitic capacitances corresponding to the capacitances 112 and 114 and the large voltage swings interfere with the operation of the output circuitry in the prior art and they slow the response of such circuitry.
A signal 122 in FIG. 2 may be introduced to the line 100 (FIG. 1). This causes the transistor 102 to become conductive. The production of a conductive state in the transistor 102 is also facilitated because it is in series with the transistor 106. The current through the transistor 106, and therefore through the transistor 102, has a predetermined value because of the fixed bias introduced to the base of the transistor 106 through the circuitry shown in FIG. 3. When the transistor 102 becomes conductive, the charges in its parasitic capacitances 112 and 114 facilitate the flow of current through the transistor 102. The distributed capacitances 112 and 114 accordingly aid the switching of the output transistor 104 from the conductive state to the non-conductive state, thus increasing the switching speed of the transistor 104. Furthermore, the voltage swing at the drain of the transistor 106 is reduced and this further increases the speed of switching the transistor 104. This results in the current wave forms 124 (FIG. 2) in the line 110 in FIG. 1.
At the end of the signal on the line 100, the transistor 102 becomes non-conductive and the transistor 104 becomes conductive because of the bias voltage on the gate of the transistor 104. The resultant flow of current through the transistors 106 and 104 produces a rise in voltage on the drain of the transistor 106 and on the source of the transistor 104. Since this rise in voltage is from a value of approximately +1 volts which is produced on the sources of the transistors 102 and 104 when the transistor 102 is conductive, the rise in voltage on the drain of the transistor 104 is quite fast. This results in part from the fact that the voltage of approximately +1 volts on the source of the transistor 104 is quite close to the voltage of approximately +1.2 volts on the gate of the transistor. This is particularly true since the corresponding voltage on the source of the n-type of transistor in the prior art to the transistor corresponding 102 (p-type in this invention) is approximately 0 volts. The production of a positive voltage on the source of the transistor 104 is facilitated by the charging of the distributed capacitances 112 and 114 when the transistor 102 becomes non-conductive.
As a result of the discharge of the distributed capacitances 112 and 114 through the transistor 102 in the circuitry shown in FIG. 1 when the transistor 102 becomes conductive, the slope of the signal produced if the distributed capacitors 112 and 114 did not discharge through the transistor 102. This may be seen from a comparison of the leading edge of the signal 124 (FIG. 2) produced on the line 110 by the circuitry shown in FIG. 1 in comparison to the leading edge of a signal 126 produced on the same line by the circuitry of the prior art. Furthermore, as will be seen from the signal 124, no blips are produced in the leading and trailing edges of the signal.
The trailing edge of the output signal 124 produced by the circuitry shown in FIG. 1 is also sharper than the signal 126 produced by the circuitry of the prior art. This results from the reduced time, in comparison to the prior art, for the voltage on the drain of the transistor 104 to reach the proper value when the transistor 104 changes from a non-conductive state to a conductive state in the circuitry of this invention.
As will be seen from the above discussion, the circuitry shown in FIG. 1 and described above has certain advantages over the prior art. It provides on the output line 110 the signal 124 at a frequency in excess of eighty-five megahertz (85 mhz). It also provides the signal 124 with relatively sharp characteristics. This is in contrast to the prior art since the prior art provides the output signal 126 at a maximum frequency of approximately twenty-five megahertz (25 mhz) and with characteristics not nearly as sharp as those of the signal 124.
FIG. 3 illustrates circuitry for regulating the biasing voltages introduced to the gates of the transistors 104 and 106. The circuitry shown in FIG. 3 is disposed on an integrated circuitry chip. The circuitry shown in FIG. 3 includes a pad 150 outside of the chip 60 for providing a reference voltage such as approximately 1.2 volts and a pad 152 outside of the chip 60 for providing a reference voltage such as approximately -1.2 volts. A resistance 154 is disposed electrically between the pad 150 and a reference potential such as ground.
Input terminals of an operational amplifier 156 are respectively connected to the pads 150 and 152. The output from the operational amplifier 156 is introduced to the gate of a transistor 158 such as a MOS transistor of the p-type. The source of the transistor 158 receives an energizing voltage such as approximately +5 volts. The drain of the transistor 158 and a source of a transistor 160 are common. Connections are respectively made from the gate and the drain of the transistor 160 to the pads 152 and 150. The transistor 160 may be a MOS transistor of the p-type.
The output of the operational amplifier 156 is introduced to the gates of transistors 106a, 106b, etc. corresponding to the transistor 106 in FIG. 1. Similarly, connections are made from the pad 152 to the gates of transistors 104a, 104b, etc. corresponding to the transistor 104 in FIG. 1. Transistors 102a, 102b, etc. (corresponding to the transistor 102 in FIG. 10) are respectively connected to the transistors 104a and 106a and to the transistors 104b and 104b in a manner shown in FIG. 1. Lines 110a, 110b, etc. are connected to the line 110 also shown in FIG. 1. Lines 103a, 103b, etc. correspond to the line 103 in FIG. 1.
A substantially constant current flows through a circuit including the pad 150, the resistance 154 and the reference potential such as ground. This current is balanced in the operational amplifier 156 by the current produced in the amplifier as the result of the introduction of the voltage from the pad 152 to the amplifier. The current in the operational amplifier biases the transistor 158 to a state of conductivity so that current flows through the transistors 158 and 160 to the pad 150 to correct for any imbalances between the current flowing through the operational amplifier 156 and the current flowing through the resistance 154. In this way, the bias introduced from the operational amplifier 156 to the gate of the transistor 158 is substantially constant.
The transistors 158 and 160 correspond respectively to the transistors 106a, 106b, etc., and the transistors 104a, 104b, etc. As a result, the same current flows through the transistors 106a and 104a and through the transistors 106b and 104b as flows through the transistors 158 and 160. As a result, each of the circuits 106a and 104a, 106b and 104b, etc., provides a substantially constant current to the output line 110 in FIGS. 1 and 3 when a signal is introduced to the gate of the associated one of the transistors 102a, 102b, etc., to make these transistors conductive. The magnitude of the cumulative current on the output line 110 indicates the analog value corresponding to the value of digital signals introduced to the gates of the transistors 102a, 102b, etc. in FIG. 3. The analog indication represented by the current on the line 110 is monotonic and provides minimal integral and differential non-linearities.
Although this invention has been disclosed and illustrated with reference to particular embodiments, the principles involved are susceptible for use in numerous other embodiments which will be apparent to persons skilled in the art. The invention is, therefore, to be limited only as indicated by the scope of the appended claims.