1. Technical Field
The present disclosure relates to current setting circuits such as current minors, and more particularly, to voltage and temperature invariant current setting circuits such as those used to control the gain in HBT (heterojunction bipolar transistor)-based designs.
2. Background
Current mirrors are used to accurately set currents in circuits. In multi-stage amplifier circuits that are HBT (heterojunction bipolar transistor)—based designs such as that shown in
As described herein, a current supply circuit having an input node connectable to a voltage supply and an output node operable to provide an output current includes a current source circuit coupled to a reference voltage node and configured to provide the output current at the output node, wherein a voltage at the reference voltage node controls current output of the current source circuit. The current supply circuit also includes a reference-setting circuit coupled to the reference voltage node and operable to establish a reference current level of the current source circuit, a common-emitter circuit coupled to the input node, and an emitter-follower circuit coupled to the input node, the emitter-follower circuit having an input coupled to an output of the common-emitter circuit and an output coupled to the reference voltage node.
Also described herein is a current supply circuit having an input node connectable to a voltage supply and an output node operable to provide an output current, the current supply circuit including means coupled to a reference voltage node for providing the output current at the output node, wherein a voltage at the reference voltage node controls current output of the means for providing the output current, means coupled to the reference voltage node for setting a reference current level of the means for providing the output current, an amplifying means coupled to the input node, and means for buffering voltage from the input node and having an input coupled to an output of the amplifying means and an output coupled to the reference voltage node.
The accompanying drawings, which are incorporated into and constitute a part of this specification, illustrate one or more examples of embodiments and, together with the description of example embodiments, serve to explain the principles and implementations of the embodiments.
The description herein is provided in the context of a current control mechanism for low voltage applications. Those of ordinary skill in the art will realize that the following detailed description is illustrative only and is not intended to be in any way limiting. Other embodiments will readily suggest themselves to such skilled persons having the benefit of this disclosure. Reference will now be made in detail to implementations as illustrated in the accompanying drawings. The same reference indicators will be used throughout the drawings and the following detailed description to refer to the same or like parts.
In the interest of clarity, not all of the routine features of the implementations described herein are shown and described. It will, of course, be appreciated that in the development of any such actual implementation, numerous implementation-specific decisions must be made in order to achieve the developer's specific goals, such as compliance with application- and business-related constraints, and that these specific goals will vary from one implementation to another and from one developer to another. Moreover, it will be appreciated that such a development effort might be complex and time-consuming, but would nevertheless be a routine undertaking of engineering for those of ordinary skill in the art having the benefit of this disclosure.
As used herein, the symbol n+ indicates an n− doped semiconductor material typically having a doping level of n− type dopants on the order of 1020 atoms per cubic centimeter or more. The symbol n− indicates an n−doped semiconductor material (such a silicon (Si), germanium (Ge), Gallium Arsenide (GaAs), and the like) typically having a doping level on the order of 1017 atoms per cubic centimeter for n− doped wells and on the order of 1015 atoms per cubic centimeter for n− substrate material. The symbol p+ indicates a p− doped semiconductor material typically having a doping level of p-type dopants on the order of 1020 atoms per cubic centimeter or more. The symbol p− indicates a p− doped semiconductor material typically having a doping level on the order of 1017 atoms per cubic centimeter for p− doped wells and on the order of 1015 atoms per cubic centimeter for p− substrate material. Those of ordinary skill in the art will now realize that a range of doping concentrations around those described above will also work. Furthermore, the devices described herein may be formed on a conventional semiconductor substrate or they may as easily be formed as a thin film transistor (TFT) above the substrate, or in silicon on an insulator (SOI) such as glass (SOG), sapphire (SOS), or other substrates as known to those of ordinary skill in the art. Essentially, any process capable of forming pFETs and nFETs will work. Doped regions may be diffusions or they may be implanted. When it is said that something is doped at approximately the same level as something else, the doping levels are within a factor of ten of each other, e.g., 1016 is within a factor of ten of 1015 and 1017.
Circuit 200 includes a linear common-emitter circuit comprising resistors RC (collector) and RE (emitter) and transistor Q1 coupled therebetween. The linear common-emitter circuit operates as a means for amplifying voltage. In the example embodiment of
As mentioned above, RC and RE provide bias voltage compensation. Specifically, if voltage source VCC varies by a voltage amount ΔVCC, the current through transistor Q1 changes by ΔVCC/RE. The change in current through transistor Q1 is expressed as ΔIQ1 and is substantially equivalent to ΔVCC/RE. The voltage VREF1 at the output 208 of the linear common-emitter circuit can be maintained constant if ΔIQ1×RC is ΔVCC, or, in other words, if
ΔVCC/RE×RC=ΔVCC, or
RC=RE
with the assumption that the beta β (common-emitter current gain) of transistor Q1 is high, so that collector current is substantially the same as emitter current. Of course, while expressed in terms of two resistors RC and RE having equal values, each of these passive devices may itself comprise for example multiple resistors or other means for providing electrical resistance, or, more generally, impedance.
VREF1 at node 208 operates as the input to an emitter-follower circuit comprising transistor QEF and resistor REF, the output of which is coupled to VREF at node 210. QEF, in this example embodiment, is an HBT (heterojunction bipolar transistor). A constant VREF1 helps to maintain a constant voltage at reference voltage node VREF in spite of changes in VCC. The constant VREF keeps the reference current through QREF constant. The device QREF operates as the means for setting the reference current for the current sources, and is not limited to a transistor configured in the manner shown, but can be a diode instead. In the specific example embodiment depicted in
The emitter-follower QEF, REF is used to minimize the loading effect on VREF1 due to the diode current of the reference QREF and base currents for QREFX,QREFX2. The resistor REF is used to adjust the reference current through the reference diode QREF. RREF operates along with QREF to set the reference current for I1, I2 (and any other current sources) by appropriate scaling of QREFX, QREFX2 and RREFX1, RREFX2.
It may also be desired to achieve temperature compensation so that the circuit is temperature invariant as well as voltage invariant. With reference to
With section 300, the voltage change at the base of Q1 is determined by the ratio between Rtemp and RD (voltage divider circuit). RD/(RD+Rtemp) sets the percentage of ΔVCC (change in VCC) that leads to a change in the current through Q1—that is ΔIQ1. The current change through Q1 (ΔIQ1) due to ΔVCC will be
RD/(RE+Rtemp)×ΔVCC/RE
In order to keep VREF1 constant, the voltage across RC should also change by ΔVCC. This then leads to the following equations:
ΔIQ1×RC=RC×RD/(RD+Rtemp)×ΔVCC/RE=ΔVCC, or
RC/RE=(RD+Rtemp)/RD
In the this manner, in the circuit of
The transistor QCTRL, also an HBT in these example embodiments, is provided for changing the value (that is, amplitude) of I1 and I2 by changing the voltage Vctrl. Such current amplitude control may be desired depending on the specific application.
The above are exemplary modes of carrying out the invention and are not intended to be limiting. It will be apparent to those of ordinary skill in the art that modifications thereto can be made without departure from the spirit and scope of the invention as set forth in the following claims.
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