People inevitably will ask how this relates to bridged amplifiers in general, and the balanced amplifier offerings of other companies. It is similar only in that both terminals of the output to the speaker are “live”; neither of them is grounded. You could in fact “bridge” two X1000’s together to give you an 8 kilowatt peak into 8 ohms. Actually, when bridging two such amplifiers together, we would generally recommend also paralleling yet another pair to get 16 kW peak into 4 ohms, and yet four more for 32 kW peak into 2 ohms, and so on.
The supersymmetric amplifier is a special subset of balanced amplifiers, unique and covered by U.S. patent. Supersymmetry is an approach that truly takes advantage of balanced operation like no other and requires a balanced input to retain the precisely matched behavior.
Supersymmetry is ideally used to obtain high quality performance from very simple circuit topologies, avoiding the high order distortion character and feedback instabilities of complex circuits. A single gain stage amplifier using this approach can perform as well as a two gain stage design, and a two gain stage version of this topology can outperform the four or five stages of a conventional amplifier.
Here is some more explanation of the details of its operation:
The supersymmetry topology does not use operational amplifiers as building blocks, nor can it be represented with operational amplifiers. It has two negative inputs and two positive outputs and consists of two matched gain blocks coupled at one central point where the voltage is ideally zero. The topology is unique in that at this point, the distortion contributed by each half appears out of phase with the signal, and we use this to reinforce the desired signal and cancel noise and distortion. This occurs mutually between the two halves of the circuit, and the result is signal symmetry with respect to both the voltage and current axis, and anti- symmetry for distortion and noise. This means that the distortion and noise of each half appears identically and cancels.
The diagram on the patent cover sheet shows an example of this topology. Each of the two input devices 20 and 21 are driven by an input signal, and their outputs run through a folded cascode formed by devices 30 and 31 to develop voltages across current sources 34 and 35. The sources 20 and 21 are coupled through resistor 40 which is the sole connection between the two halves and which also sets the gain of the circuit.
The gates of the input devices 20, 21 are virtual grounds, and ideally would be at absolutely zero voltage. However, as the gain stage is not perfect, finite distortion and noise voltages appear at these points. These appear at the other side through resistor 40, in phase at the output of the other half of the system, where they match the distortion and noise of the first half.
By actual measurement, this circuit does essentially nothing to reduce the distortion and noise in each half. Distortion curves before and after supersymmetry is applied are nearly identical. The distortion curves of the circuit from the patent cover sheet show: (a) the intrinsic distortion of each half of the example circuit, (b) the distortion of the differential output lowered due to the intrinsic matching between the circuits, (c) the distortion of each half with supersymmetry, and
(d) the differential distortion with supersymmetry.
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