Towards a Monolithic, Substrate-Reusable and an All-Epitaxial
Design for III-V-on-Si Solar Cells
Nikhil Jain, Michael Clavel, Patrick Goley, and Mantu Hudait
Virginia Tech, Blacksburg, VA 24060
Abstract - Integration of III-V multi j unction solar cells on
Si substrate can address the future levelized cost of energy by
unifying the high-efciency merits of III-V materials with the
low-cost and abundance of Si.
A
Si-compatible monolithically
integrated 3J InGaP/GaAs/Ge-Si cell design with a hybrid
Ge-Si bottom cell is investigated. Utilizing a combination of
comprehensive modeling and experimental material
characterization techniques, we present our results for ultra
thin epitaxial Ge directly grown on Si substrate using
molecular beam epitaxy. Virtual "Ge-on-Si" substrates could
provide a large-area, low-cost alternative to expensive Ga
A
s
wafers, a promising step towards realizing monolithic, high
efciency and low-cost III-V-on-Si photovoltaics.
Inde Terms - III-V-on-Si, Ge-on-Si, heteroepitaxy,
photovoltaic cells, solar cell design.
I. INTRODUCTION
While the efciency of mainstream Si based solar cells has
almost saturated at �25%, III-V multijunction solar cells have
steadily shown perforance improvement, reaching a recent
record efciency of 46%. Integration of such III-V
multijunction cells with Si can address the fture levelized cost
of energy by unifing the high-effciency merits of III-V
materials with low-cost and abundance of Si. To date,
effciency of 3J III-V/Si tandem solar cells have merely
exceeded 25% [1] even afer employing non-monolithic
techniques such as wafer-bonding [2] and areal current
matching [3]. Challenges associated with material growth,
reliability and reproducibility have limited the success of III
V-on-Si technology. Thus, novel approaches are sought for
realizing the potential of III-V-on-Si multijunction solar cells.
A very promising path for monolithic integration of III-V
solar cells on Si would be to utilize a thin intermediate Ge
buffer layer. Successfl demonstration of virtual "Ge-on-Si"
template could signifcantly reduce the cost per watt attributed
to the large area and low cost of Si substrate. Interestingly,
utilizing Ge intermediate layer de-couples two critical
challenges for GaAs-on-Si growth: (i) polar on non-polar
epitaxy and (ii) lattice-mismatch growth. Owing to a small
band gap, the Ge layer absorbs a wide spectrum of the incident
sunlight beyond the GaAs absorption edge, and therefore the
hybrid Ge-Si subcell does not limit the current in 3J
InGaP/GaAs/Ge-Si solar cells. The Ge intermediate layer
approach for III-V-on-Si integration could be utilized (i) to
create virtual "Ge-on-Si" template for subsequent GaAs
growth (could potentially involve active Ge subcells), (ii)
978-1-4799-7944-8/15/$31.00 ©2015 IEEE
solely as a buffer layer for connecting III-V cells to an active
Si bottom subcell, and (iii) as the emitter layer for bottom Si
base, forming a hybrid Ge-Si subcell.
Utilizing a Si homojunction cell beneath the Ge buffer layer
would likely require a difsion process and a thicker Si
substrate for current-matching in comparison to the hybrid Ge
Si approach. Furthermore, to allow sufcient light penetration
to active Si subcell, extremely thin Ge buffer would be
essential, rendering the subsequent GaAs growth very
challenging. Prior reports on Ge integration on Si substrate for
photovoltaics typically employed graded SixGel-x buffers,
which were several microns thick [4-6], elevating the thermal
mismatch and cost issues. While other approaches utilized a
pattered selective area epitaxy [7, 8], typically involving an
additional pattering and/or chemical polishing step. Here, we
focus on developing a non-selective area Ge-on-Si epitaxial
process with a key goal of realizing thin epitaxial Ge layers
allowing light penetration to the bottom Si substrate cell.
Thus, in this work we focus on the design, modeling and
epitaxial growth for hybrid Ge-Si bottom subcell, wherein the
epitaxial Ge layer serves as a uniforly doped emitter for
bottom Si subcell, thus forming a hybrid Ge-Si subcell. This
approach precludes the need for difsed Si junction, allowing
an in-situ and an all-epitaxial process for subsequent III-V
growth requiring very thin Si « 60Ilm). Such 3J cells with
very thin Si would also be very promising for CPV
applications and could frther beneft fom additional cost
InGaP
I
(1.86eV)
Hybrid
I
Ge-Si ••
Fig. 1 Schematic depiction of tandem 3J InGaP/GaAs/Ge-Si
solar cell utilizing a hybrid Ge-Si bottom subcell.