An industrial ultrashort pulse thin slab laser amplifier.
Abstract
A laser amplifier has been designed and constructed for use in a Master Oscillator – Power
Amplifier configuration for the amplification of the output from a low average power, high
beam quality ultrashort pulse oscillator. The aim of the project was to design and construct an
amplifier module that could provide a technology platform for products that would satisfy the
growing market requirements for high average laser systems beyond 50 W of average output
power with pulse duration of 0.5-5 picoseconds.
The design was based around a Yb:YAG thin slab crystal gain medium that utilised a novel
pump scheme delivering up to 321 W of ~ 940 nm wavelength pump light. At maximum pump
power, the small-signal gain coefficient of the amplifier was measured to be ~ 1.6 cm-1
.
Measurements of the pump-induced lens strength of the amplifier at various pump powers
provided the necessary optical data which enabled a multi-fold mirror arrangement to be
designed that folded the seed beam through the thin slab in order to maximise extracted power.
This design included the novel implementation of both the pre-amplifier and power amplifier
functions from a single Yb:YAG crystal gain cell. This approach facilitated the input seed
power to be as low as 12 mW without the onset of parasitic oscillations.
Integrating a 3.5 W, 55 MHz ultrashort pulse oscillator to the amplifier resulted in a maximum
output power of 91 W with pulse durations of 710 fs, whilst the inclusion of a pulse-picker
resulted in an output power of 87.5 W with pulse durations of 905 fs at 4.5 MHz with 316 mW
of input power. This demonstrated that the novel use of the pre-amplifier yielded a unique
feature; that at high pump powers, there is only a small percentage change in output power for a
large percentage change in average input power. In essence, the average output was near
constant over a large range of pulse-picked frequencies maximising the dynamic range of pulse
energy and pulse frequency combinations. The beam quality in both regimes was measured to
give an M2
value of ~ 1.1 in the y-axis and ~ 1.5 in the x-axis, reducing to ~ 1.2 in the x-axis
after spatial filtering with a loss of ~10% - 15% of average output power.
Power scalability was demonstrated by cascading two additional amplifier modules and resulted
in a maximum output power of 230 W at 4 MHz, yielding pulse energies in excess of 57 µJ.