Photoelectrons, which are produced by solar Extreme Ultraviolet (EUV) and X-ray ionization of various neutrals, are an important component of the dayside Martian upper atmosphere (e.g. Coates et al., 2011; Fox et al., 2008). The ionization process generates well-defined, unique features in the photoelectron energy distribution, characterized by several distinctive peaks at 22-27 eV related to the He II 30.4 nm line, which is the most intensive EUV emission line in the solar spectrum (e.g. Frahm et al., 2006b; 2006a). In addition, a reduction in photoelectron intensity occurs around 60-70 eV due to the rapid drop in solar radiation at wavelengths shorter than 17 nm (e.g. Peterson et al., 2016; Sakai et al., 2015). The above spectral features have been extensively observed over the past four decades (e.g.