I. Introduction
The solar cell devices made up of III-V semiconductors report highest efficiency values [1]. However, the cost of producing these cells is high and hence, limiting their use in concentrated photovoltaic (CPV) and space applications. In this high cost; the cell cost is acritical; however, the substrate cost is the main contributing factor [2], [3]. On the other hand, the Si-based photovoltaics is inexpensive due to the mature Si-technology. Therefore, an alternative to achieve the low-cost III-V semiconductor-based photovoltaics devices, is to use Si as a substrate [4]– [6]. However, the lattice mismatch between Si substrate and III-V semiconductors like GaAs introduces defects and dislocations densities. These defects and dislocations cause a degradation in the device performance [7], [8]. A potential solution to overcome this problem is to use Ge-on-Si substrate. The lattice constant of Ge (5.658 Å) perfectly matches with the GaAs. It enables the fabrication and integration of GaAs based solar cell devices on low-cost Si platform. However, the growth of defect-free Ge directly over Si-substrate is difficult due to a lattice mismatch of ~ 4% [9]. The high strain values associated with ~ 4% lattice mismatch leads to dislocation densities as high as 1010-1012 cm−2 [10]. These dislocation densities lie to few nanometers from the Si/Ge interface and extend to the surface acting as recombination centers for carriers, and hence killing the device efficiency [11]. The use of a buffer layer between Si and Ge is a potential solution to reduce the dislocation densities as low as 106 cm−2 [12]. However, this approach requires a thicker buffer layer (10 μm) [13] and multiple-steps for its deposition; which makes it a costly and extensive affair.