### 4.2 Signal demodulation

A typical application of light modulation, is its use in a modulation-demodulation scheme, which applies
an electronic demodulation to a photodiode signal. A ‘demodulation’ of a photodiode signal at a
user-defined frequency , performed by an electronic mixer and a low-pass filter, produces a
signal, which is proportional to the amplitude of the photo current at DC and at the frequency
. Interestingly, by using two mixers with different phase offsets one can also reconstruct the
phase of the signal, or to be precise the phase difference of the light at with respect
to the carrier light. This feature can be very powerful for generating interferometer control
signals.
Mathematically, the demodulation process can be described by a multiplication of the output with a
cosine: ( is the demodulation phase), which is also called the ‘local oscillator’. After the
multiplication was performed only the DC part of the result is taken into account. The signal is

Multiplied with the local oscillator it becomes
With and we can write
When looking for the DC components of we get the following [20]:
This would be the output of a mixer and a subsequent low-pass filter. The results for and
are called in-phase and in-quadrature, respectively (or also first and second quadrature). They
are given by
If only one mixer is used, the output is always real and is determined by the demodulation phase. However,
with two mixers generating the in-phase and in-quadrature signals, it is possible to construct a complex
number representing the signal amplitude and phase:
Often several sequential demodulations are applied in order to measure very specific phase information.
For example, a double demodulation can be described as two sequential multiplications of the signal with
two local oscillators and taking the DC component of the result. First looking at the whole signal, we can
write:

This can be written as
and thus reduced to two single demodulations. Since we now only care for the DC component we can use
the expression from above (Equation (82)). These two demodulations give two complex numbers:
The demodulation phases are applied as follows to get a real output (two sequential mixers)
In a typical setup, a user-defined demodulation phase for the first frequency (here ) is given. If
two mixers are used for the second demodulation, we can reconstruct the complex number
More demodulations can also be reduced to single demodulations as above.