Real Time Optics of
Photovoltaic Materials and Structures:
From Mueller Matrices to
Phase Diagrams
Robert W. Collins
Department of Physics, Materials Research Institute,
and Center for Thin Film Devices
The Pennsylvania State University, University Park, PA 16802
A set of spectroscopic probes based
on ellipsometric principles has been developed with the goal being to
characterize thin film photovoltaic materials and device structures in situ and in real time during their
fabrication. In these optical probes,
polarized white light from a polarization generation system is directed through
a reactor window onto the film surface during growth. The obliquely reflected beam exits the reactor through a second
window and is analyzed by a multichannel polarization detection system.
Instruments of increasing complexity
have been designed to characterize thin film structures of increasing
complexity. Incorporating a single
rotating polarizer as the polarization detection system leads to an instrument
that provides the tilt and ellipticity angles of the reflected beam
polarization ellipse versus wavelength and time. This approach is sufficient for determining the time evolution of
optical properties and layer thicknesses for uniform, isotropic materials. If instead a rotating compensator (phase
shifter) followed by a fixed polarizer is incorporated as the detection system,
information on the degree of polarization of the reflected beam can be
obtained, as well. This is a useful
parameter in characterizing the growth of inhomogeneous, isotropic
materials. Finally, if rotating
compensators are incorporated on both the polarization generation and detection
sides of the instrument, then the 4x4 Mueller matrix of the growing film is
accessible versus wavelength and time.
This is the ultimate measurement, and is useful in characterizing the
evolution of optical properties and microstructure of materials that are both
inhomogeneous and anisotropic.
We have applied the single rotating
compensator version of real time spectroscopic ellipsometry to characterize the
time and thickness evolution of the optical properties and microstructure of
silicon thin films from spectra collected during deposition. From the optical
properties, one can easily distinguish hydrogenated amorphous silicon (a-Si:H)
growth from microcrystalline silicon (mc-Si:H)
growth. In fact, depth profiles in the
volume fraction of microcrystallinity can be determined. This capability has led to the development
of deposition phase diagrams that can guide the fabrication of silicon thin films
at low temperatures (<300°C) for highest performance solar cells. The simplest phase diagrams identify a
single transition from an amorphous growth regime to a mixed-phase (amorphous +
microcrystalline) growth regime versus accumulated film thickness [the a®(a+mc)
transition]. These phase diagrams have
shown that optimization of a‑Si:H intrinsic layers for solar cell
applications is achieved by rf plasma-enhanced chemical vapor deposition using
the maximum possible flow ratio of H2 to SiH4 that can be
sustained while avoiding the a®(a+mc)
transition.