“…Many molecular observations have verified that the temperature (T ¼ 33-100 K) and density [n ¼ ð1 8Þ Â 10 5 cm À3 ] are in accord with OH (1720 MHz) theory (Turner et al 1992;Dickman et al 1992;Ziurys, Snell, & Dickman 1989;van Dishoeck, Jansen, & Phillips 1993;Cesarsky et al 1999;Rho et al 2001). The OH (1720 MHz) masers occur in '' clump G '' of the shocked molecular interaction regions in IC 443 (DeNoyer 1979b;Huang, Dickman, & Snell 1986) and, specifically, subclump G1 as resolved by submillimeter and interferometric observations (van Dishoeck et al 1993;Tauber et al 1994). Nonetheless, an important observational constraint that is still required is the transverse size of the region of OH inversion.…”