
1.1 Basic feedback control theory 3
1.1.2 Frequency response of a feedback servo
The operation of feedback servos is usually described in terms of
the Fourier frequency response; that is, the gain of the feedback
as a function of the frequency of a disturbance. For example, a
common disturbance fmis mains frequency, fm= 50 Hz or 60 Hz.
That disturbance will alter the laser frequency fby some amount,
at a rate of 50 or 60 Hz. The effect of the disturbance on the laser
might be small (e.g. f=f0±1 kHz where f0is the undisturbed laser
frequency) or large (f=f0±1 MHz). Regardless of the size of this
disturbance, the Fourier frequency of the disturbance is either at
50 or 60 Hz. To suppress that disturbance, a feedback servo should
have high gain at 50 and 60 Hz to be able to compensate.
The gain of a servo controller typically has a low-frequency limit,
usually defined by the gain-bandwidth limit of the opamps used in
the servo controller. The gain must also fall below unity gain (0 dB)
at higher frequencies to avoid inducing oscillations in the control
output, such as the familiar high-pitched squeal of audio systems
(commonly called “audio feedback”). These oscillations occur for
frequencies above the reciprocal of the minimum propagation delay
of the combined laser, frequency discriminator, servo and actuator
system. Typically this limit is dominated by the response time of
the actuator. For the piezos used in external cavity diode lasers, the
limit is typically a few kHz, and for the current modulation response
of the laser diode, the limit is around 100 to 300kHz.
Figure 1.3 is a conceptual plot of gain against Fourier frequency for
the FSC. To minimise the laser frequency error, the area under the
gain plot should be maximised. PID (proportional integral and differ-
ential) servo controllers are a common approach, where the control
signal is the sum of three components derived from the one input
error signal. The proportional feedback (P) attempts to promptly
compensate for disturbances, whereas integrator feedback (I) pro-
vides high gain for offsets and slow drifts, and differential feedback
(D) adds extra gain for sudden changes.