Sigma delta — where it appears
Named by 2 essays across one field — each of them below, with the objects they name alongside it.
Two loops, and the mismatch between them
The rung below marched single loops of second, third and fourth order and found the amplitude at which each stops working, falling with the order — which is why nobody builds a fourth-order single loop. The standard answer is two first-order loops with the first one's error fed to the second and differentiated back out, giving second-order shaping out of parts that cannot be unstable. The cancellation is between an analogue path and a digital one, and it is worth 25 decibels until the two differ by five per cent.
A floor, or five tones
The field's sharpest statement about a one-bit loop is that three quarters of its in-band error sits in five lines, against the 1.953 per cent a white error would put in any five — a factor of thirty-eight. The comparison is to a white error, and a shaping loop exists to make its error anything but white. Measured against the loop's own transfer function, which the loop reproduces line by line to a part in five hundred when it is dithered, the same error is 17.4 times tonal at a fiftieth of full scale and 8.9 times at nine tenths. And 99.5 per cent of it at the quiet end is two harmonics of the input.
Named alongside it
The objects these essays reach for when they reach for this one.
Noise shapingOversamplingQuantisationDesign tradeoffDevice mismatchDynamic rangeIdle tonesMeasurement conditionSpectral densityStabilityTotal harmonic distortionVerification