The
mixed cation compounds Na1–x
K
x
AsSe2 (x = 0.8,
0.65, 0.5) and Na0.1K0.9AsS2 crystallize
in the polar noncentrosymmetric space group Cc. The AAsQ
2 (A =
alkali metals, Q = S, Se)
family features one-dimensional (1D) 1/∞[AQ
2
–] chains comprising
corner-sharing pyramidal AQ
3 units in
which the packing of these chains is dependent on the alkali metals.
The parallel 1/∞[AQ
2
–] chains interact via short As···Se
contacts, which increase in length when the fraction of K atoms is
increased. The increase in the As···Se interchain distance
increases the band gap from 1.75 eV in γ-NaAsSe2 to
2.01 eV in Na0.35K0.65AsSe2, 2.07
eV in Na0.2K0.8AsSe2, and 2.18 eV
in Na0.1K0.9AsS2. The Na1–x
K
x
AsSe2 (x = 0.8, 0.65) compounds melt congruently at approximately
316 °C. Wavelength-dependent second harmonic generation (SHG)
measurements on powder samples of Na1–x
K
x
AsSe2 (x = 0.8, 0.65, 0.5) and Na0.1K0.9AsS2 suggest that Na0.2K0.8AsSe2 and
Na0.1K0.9AsS2 have the highest SHG
response and exhibit significantly higher laser-induced damage thresholds
(LIDTs). Theoretical SHG calculations on Na0.5K0.5AsSe2 confirm its SHG response with the highest value
of d
33 = 22.5 pm/V (χ333
(2) = 45.0 pm/V).
The effective nonlinearity for a randomly oriented powder is calculated
to be d
eff = 18.9 pm/V (χeff
(2) = 37.8 pm/V),
which is consistent with the experimentally obtained value of d
eff = 16.5 pm/V (χeff
(2) = 33.0 pm/V). Three-photon
absorption is the dominant mechanism for the optical breakdown of
the compounds under intense excitation at 1580 nm, with Na0.2K0.8AsSe2 exhibiting the highest stability.