“…To examine whether the elastic properties of Cr‐pyrope at high P and high T can be calculated using the end‐member component elastic properties, we calculated the elastic properties ( ρ , K S , G , V P , and V S ) of Prp‐Cr#12 at high P and high T using the directly measured elastic parameters (Table S4 in Supporting Information ) in this study and then compared the results to those calculated using the elastic parameters interpolated from linear mixing of end‐member elastic parameters (end‐member model; Table S5 in Supporting Information ; Angel et al., 2018; Arimoto et al., 2015; Bass, 1986, 1989; Cameron et al., 1973; Chantel et al., 2016; Dymshits et al., 2014; Faccincani et al., 2021; Fan et al., 2020; Gréaux & Yamada, 2019; Gwanmesia et al., 2014, 2006; Hao et al., 2020; Hugh‐Jones, 1997; Isaak et al., 1992; Jackson et al., 2007; Jacobsen et al., 2010; Jeanloz & Thompson, 1983; Klemme et al., 2005; Kroll et al., 2012; Li & Neuville, 2010; Ma et al., 2009; Z. Mao et al., 2015; Milani et al., 2015, 2017; Ohashi, 1984; Sang & Bass, 2014; Sinogeikin & Bass, 2000, 2002; Soga, 1967; Tribaudino et al., 2008; Wang & Ji, 2001; Xu et al., 2018, 2020, 2022; Yang & Ghose, 1994; Zhang & Bass, 2016a, 2016b; Zhang et al., 1998; Zhao et al., 1997, 1998; Zou, Gréaux, et al., 2012). We calculated the elastic properties at pressures of 3–8 GPa at 1000 and 1600 K, which are the lower and upper bound of typical SCLM P ‐ T conditions where garnet‐peridotite stabilizes.…”