Two different approaches to plasma
deposition technology were explored
for the fabrication of photoactive GaP(N) layers at 390 °C, namely,
conventional plasma-enhanced chemical vapor deposition (PECVD) and
plasma-enhanced atomic layer deposition (PE-ALD). The structural properties
of GaP films deposited by PECVD using a gas mixture of phosphine (PH3), trimethylgallium (TMG), and hydrogen (H2) depend
on dilution and plasma power. Strong H2 dilution of the
gas mixture and high RF power are required to reach the growth of
microcrystalline GaP films; otherwise, the films are amorphous. However,
even the PECVD process, which provides the growth of microcrystalline
GaP, with additional N2 flow leads to effective incorporation
of nitrogen into amorphous GaPN ternary alloy with a significant growth
rate increase. In contrast, the PE-ALD process allows one easily to
control the structural properties by plasma power variation and stoichiometric
composition due to self-limitation of surface reaction. PE-ALD process
with Ar plasma activation, which provides the initial epitaxial growth
for the first 20–30 nm of GaP on Si substrates with subsequent
growth of microcrystalline GaP, was used for further GaPN growth.
Microcrystalline GaPN films with precise control of nitrogen incorporation
were obtained by the PE-ALD process using the sub-monolayer digital
alloy approach, which means that the growth of a few GaP monolayers
is sequenced by the growth of GaN sub-monolayer. First GaP/GaPN p–i–n
structures grown on Si substrates using PE-ALD demonstrate spectral
response in the range of 300–600 nm, being of potential interest
for multijunction solar cells. However, for photovoltaic applications,
further technology development is required to reduce the defect density
in the GaPN layers and improve the quality of the doped layers including
the GaP/Si interface.