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| optical parametric amplification | optical purity |
frequency
)
is partially converted into two coherent beams, the signal and the idler,
with wavelengths
(
,
)
and frequencies
(
,
)
such that
.
By simultaneous rotation of the crystal and adjustment of the optical resonator,
the wavelength of the signal beam is continuously tunable, theoretically from
to
and practically over a
slightly more reduced range.
(3rd
harmonic of a Nd:YAG laser),
can be tuned from
(with
)
up to
(with
).
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