In thermoelectric materials, chemical substitutions are widely used to optimize thermoelectric properties. The Zintl phase compound, Yb 14 MgSb 11 , has been demonstrated as a promising thermoelectric material at high temperatures. It is iso-structural with Ca 14 AlSb 11 with space group I4 1 /acd. Its iso-structural analog, Ca 14 MgSb 11 , was discovered to be a semiconductor and have vacancies on the Sb(3) sites, although in its nominal composition it can be described as consisting of fourteen Ca 2+ cations with one [MgSb 4 ] 9− tetrahedron, one Sb 3 7− linear anion and four isolated Sb 3− anions (Sb(3) site) in one formula unit. When Sn substitutes Sb in Ca 14 MgSb 11 , optimized Seebeck coefficient and resistivity were achieved simultaneously although the Sn amount is small (<2%). This is difficult to achieve in thermoelectric materials as the Seebeck coefficient and resistivity are inversely related with respect to carrier concentration. Thermal conductivity of Ca 14 MgSb 11-x Sn x remains almost the same as Ca 14 MgSb 11. The calculated zT value of Ca 14 MgSb 10.80 Sn 0.20 reaches 0.49 at 1075 K, which is 53% higher than that of Ca 14 MgSb 11 at the same temperature. The band structure of Ca 14 MgSb 7 Sn 4 is calculated to simulate the effect of Sn substitutions. Compared to the band structure of Ca 14 MgSb 11 , the band gap of Ca 14 MgSb 7 Sn 4 is smaller (0.2 eV) and the Fermi-level shifts into the valence band. The absolute values for density of states (DOS) of Ca 14 MgSb 7 Sn 4 are smaller near the Fermi-level at the top of valence band and 5p-orbitals of Sn contribute most to the valence bands near the Fermi-level.