Electronic circuit for voltage to current amplification
The present invention relates generally to amplifiers and, more particularly to voltage to current amplifiers for high frequency signals.
High frequency amplifiers are used for various applications, such as for cable antenna television (CATV) systems. CATV systems require wide-band amplifiers that amplify signals across a broad frequency bandwidth. However, high frequency amplifier applications extend operation into areas where parasitic effects of inter-electrode capacitance, wire inductance, stored charge and even operating frequency wave length begins to adversely affect circuit behavior. Minimizing distortion is particularly important when a series of amplifiers is cascaded over a signal transmission path, such as a series of high frequency amplifiers in a CATV transmission network. In an ideal communication system it is preferable that the components that comprise the system are linear. However, as a practical reality, there are many non linearities that are typically introduced by the high frequency amplifiers. The distortions created by a high frequency (RF) amplifier which are of primary concern are second order and higher even-order harmonic distortions and third order harmonic distortion components. Prior art amplifier designs have attempted to ameliorate the effects of even- order distortions by employing push-pull amplifier topologies, since the maximum even- order cancellation occurs when the proper 180 degree phase relationship is maintained over the entire bandwidth. This is often achieved through equal gain in both push-pull (halves) by matching the operating characteristics of the active devices. Such a push-pull wide band amplifier is disclosed in US patent no. 6,01 1,438. This amplifier includes a divider which divides the input signal to be amplified into two signals of differing phase and two identical amplifying circuits for amplification of the two divided signals. After amplification a combiner combines the two signals of the amplifying circuits into one signal and outputs the result signal.
It is a disadvantage of such prior art push-pull wide band amplifiers that a divider and a combiner as well as two identical amplifiers are required for cancellation of second-order distortion products. This substantially adds to the complexity and cost of such prior art amplifiers.
The present invention provides for an electronic circuit for voltage to current amplification of a high frequency signal. The electronic circuit comprises two transistors which are substantially identical and have equivalent electrical properties. Preferably field effect transistors are used as these are produced with lower tolerances in comparison to bipolar transistors. One of the transistors receives the high frequency signal to be amplified at its control terminal. The drain terminal of this transistor is coupled to virtual ground. Preferably this is accomplished by connecting the drain terminal to a supply voltage via a decoupling capacitor. The other transistor provides the amplified output signal at its drain terminal. The control terminal of this transistor is AC coupled to ground. The source terminals of both transistors are connected to a common point where a high impedance current source is applied. An inductance is coupled between the drain terminal which provides the supply voltage. By means of the inductance it is prevented that high frequency signal components of the amplified high frequency signal are added to the supply voltage which would otherwise negatively impact the linearity of the amplification. It is a particular advantage of the present invention that second-order and higher even-order harmonic distortions are cancelled out without a need to divide the input signal to be amplified, without a need for two separate amplifiers and without having to recombine the separately amplified signals. In comparison to the prior art the electronic circuit of the invention can thus be realized with a minimal number of components.
In the following preferred embodiments of the invention will be described in greater detail by making reference to the drawings in which: Fig. 1 is a circuit diagram of a preferred embodiment of an electronic circuit of the invention,
Fig. 2 is an equivalent circuit diagram of the electronic circuit of figure 1 illustrating the cancellation of even-order harmonic distortions.
Figure 1 shows electronic circuit 100. Electronic circuit 100 has transistor Q\ and transistor Q . Transistor Qi has control terminal 102 for applying a RF signal Vιnι to be amplified. Drain terminal 104 of transistor Qi is coupled to supply voltage Vcc and is AC decoupled by means of capacitor 106. This way drain terminal 104 is coupled to virtual ground. Transistor Q2 provides the amplified output signal Vout at its drain terminal
108. Control terminal 110 of transistor Q2 is AC coupled to ground. DC current source 112 is coupled to the source terminals of both transistors Qi and Q2, i.e. source terminal 114 and source terminal 116. DC current source 112 has high impedance RE. Drain terminal 108 of transistor Q2 is coupled to the supply voltage Vcc by means of inductance 118. It is to be noted that transistors Qi and Q2 are identical and have thus equivalent electrical and thermal properties. Preferably transistors Qi and Q2 are field effect transistors as field effect transistors are more ideal voltage to current amplifiers, resulting to better DC matching of transistors Ql and Q2 in comparison to bipolar transistors. Besides the better equal DC settings for FET's, also the better voltage to current amplification in FET's yields in a substantially better common mode cancellation behavior. In operation input voltage Vιnι is applied between control terminal 102 and ground. A peak to peak (p-p) voltage swing of input voltage V,„ι which is applied at control terminal 102 is illustrated in figure 1. DC current source 112 draws a total current I from the transistors Qi and Q2.
As the transistors Qi and Q2 are substantially identical the current I is split in half such that current 1/2 is drawn from source terminal 114 and current 1/2 is drawn from source terminal
1 16. As a consequence there is a voltage drop of V,„ι/2 between control terminal
102 and source terminal 114 of transistor Qi and a voltage drop having the same magnitude but opposite direction at transistor Q, i.e. voltage drop V,„ι/2 between source terminal 1 16 and control terminal 110.
This results in identical second order harmonic distortions, i.e. error signals e, which are produced by the non linear behavior of transistor Ql and Q2 though are cancelled in the virtual common mode point, the source terminals 114 and 116 of transistors Qi and Q2 respectively or the drain terminal of current source 112 in case source degeneration resistance's are used in the source terminals of transistor Ql and Q2 respectively . These second order harmonic distortions are cancelled out which provides the linear amplification of input signal V,nι. The resulting peak to peak wave form of the resulting amplified output signal Vout is also illustrated in the drawing. When transistor Q] and Q2 are exactly matching also higher even-order harmonic distortions are cancelled out. Another advantage is that the cancellation is accomplished even in case of temperature variations as the voltage drops between the control and source terminals of transistors Qi and Q2 are of opposite direction. It is a further advantage that power dissipation is minimized in comparison to prior art push-pull high frequency amplifiers. It is to be noted that the output provided at drain terminal 108 is non-inverting, which is an advantage for most applications. However, if an inverting output is required this can be obtained at the drain terminal 104 of transistor Qi, though then the required inductance 1 18 will be placed between Vcc and drain 104 where drain terminal 108 will be connected to Vcc and will be AC decoupled by capacitor 106.. The equivalent circuit diagram of figure 2 shows equivalent transformer 120 which has primary winding 122 and secondary winding 124. Transistor Qi provides half the amplified output signal Vout /2 and second order harmonic distortion signal e whereas transistor Q2 provides the inverted output signal Vout /2 and substantially the same second order harmonic distortion signal e. The signals provided by transistors Qi and Q2 are applied to terminals 126 and
128, respectively, of transformer 120. As the second order harmonic distortion signals e provided by transistors Qi and Q
2 are in phase but applied to different terminals 126 and 128 of transformer 120 they are cancelled out such that the resulting second order harmonic distortion e in the output signal V
out is substantially zero. The same applies analogously to higher even-order harmonic distortions in case transistors
and Q
2 match precisely.
LIST OF REFERENCE NUMERALS:
100 Electronic circuit 102 Control terminal 104 Drain terminal 106 Capacitor 108 Drain terminal 110 Control terminal 112 DC current source 114 Source terminal 116 Source terminal 118 Inductance 120 Transformer 122 Primary winding 124 Secondary winding 126 Terminal 128 Terminal