The preparation and optical properties of two new tin-activated calcium metasilicate phosphors are described. The more efficient of these is a ~-CaSiO~: Sn phosphor emitting in the visible at about 520 rn~. The optical properties of the tin-activated species are compared to their lead-activated analogues; and from considerations of crystal structure as affected by firing temperature and activator concentration, it is concluded that changes in spectra result from changes in crystal structure and not from the degree of aggregation of the activator ions. It is suggested that the emission spectra correspond to the 8po.~ ~So and the ~p0_~ ~So transitions of the lead-and tin-activator centers.Calcium metasilicate activated by lead and manganese is a well-known phosphor with a visible emission band at 610 m~ and an ultraviolet emission band at about 350 m~ (1-3). A study of the effect ol crystal structure (4) showed that the inversion temperature of B-CaSiO3 (wollastonite) to a-CaSiO~ (pseudowollastonite) is raised with increasing manganese concentration in agreement with results reported by Voos (5), who showed that MnSiO~ (rhodonite), being an isomorph of fl-CaSiO~, forms mixed crystals with wollastonite. A more recent study (6) of the influence of crystal structure on fl-CaSiO~:Pb + Mn showed that at temperatures where both wollastonite and pseudowollastonite are formed, the manganese crystallizes in the wollastonite lattice to the extent that a red shift is produced by the concentration of manganese in the fiCaSiO~, structure. It was shown also that the addition of magnesium oxide to calcium metasilicate increased the inversion temperature of fi-CaSiO~ to a-CaSiO3, whereas the addition of strontium oxide lowered the inversion temperature thus favoring the formation of pseudowollastonite.The calcium silicates activated by lead alone were studied in detail by Studer and Fonda (7). They found several emission bands in the ultraviolet which they attributed to differences in crystal structure as follows: two bands at 300 m~ and 385 m# to a-CaSiO~: Pb, a 345 m~ band to fl-CaSiO~: Pb, and a 334 m~ band to fl-Ca~SiO4: Pb. The corresponding excitation spectra varied widely with several maxima between 200 and 300 m~. In a later study of the mechanism of sensitized luminescence of solids, Schulman and co-workers (8) claimed that the differences in emission were due to differences in the nature of the lead activator center rather than to changes in crystal structure. Specifically, they claimed that the emission bands at 290 and 390 m~ in CaSiO~:Pb were caused by Pb ~+ singlet centers, i.e., Pb "~ § activator ions which had no otherPb ~+ nearest neighbors; whereas the single-band emission at 340 m~ observed at higher lead concentrations was attributed to the occurrence of Pb~+-Pb ~+ doublets or higher aggregates of Pb ~+ ions, i. e., centers which had 2 or more Pb =+ ions in neighboring cation positions.Due to the similarities in electronic configuration between lead and tin and the resulting similarities in chemical behavior, i...