### 3.5 Sidebands as phasors in a rotating frame

A common method of visualising the behaviour of sideband fields in interferometers is to
use phase diagrams in which each field amplitude is represented by an arrow in the complex
plane.
We can think of the electric field amplitude as a vector in the complex plane, rotating
around the origin with angular velocity . To illustrate or to help visualise the addition of several light
fields it can be useful to look at this problem using a rotating reference frame, defined as follows. A
complex number shall be defined as so that the real part is plotted along the x-axis,
while the y-axis is used for the imaginary part. We want to construct a new coordinate system
(, ) in which the field vector is at a constant position. This can be achieved by defining

or
Figure 17 illustrates how the transition into the rotating frame makes the field vector to appear
stationary. The angle of the field vector in a rotating frame depicts the phase offset of the field.
Therefore these vectors are also called phasors and the illustrations using phasors are called phasor
diagrams. Two more complex examples of how phasor diagrams can be employed is shown in
Figure 18 [11].
Phasor diagrams can be especially useful to see how frequency coupling of light field amplitudes can
change the type of modulation, for example, to turn phase modulation into amplitude modulation. An
extensive introduction to this type of phasor diagram can be found in [39].