5,10,15,20-Tetrakis(4-fluorophenyl)porphyrinatomanganese(III) tetracyanoethenide, [MnTFPP][TCNE], 1F, 5,10,15,20-tetrakis(4-bromophenyl)porphyrinatomanganese(III) tetracyanoethenide, [MnTBrPP][TCNE], 1Br, and 5,10,15,20-tetrakis(4-iodophenyl)porphyrinatomanganese(III) tetracyanoethenide, [MnTIPP][TCNE], 1I, have been prepared and characterized as both the toluene and dichloromethane disolvates and the magnetic, IR, and thermal properties of these solvates, as well as their corresponding desolvated materials, have been determined and are compared to the previously reported [TCNE]˙− salts of 5,10,15,20-tetrakis(4-chlorophenyl)porphyrinatomanganese(III), 1Cl. The νCN absorptions of 1X·2PhMe (X = Cl, Br, I) and 1I·xxCH22Cl22 occur at 2202 ± 1 (m) and 2161 ± 1 (s) cm−1 and 1X·xxCH22Cl22 (X = F, Cl, Br) and 1F·xxPhMe occur at 2195 ± 1 (m) and 2135 ± 2 (s) cm−1. Upon thermolysis at 175 °C the toluene desolvates to form α-[MnTXPP][TCNE] [X = Cl (α-1C1), Br (α-1Br), I (α-1I)] with νCN absorptions maintained at 2201 ± 1 (m) and 2160 ± 1 (s) cm−1. In contrast, unlike 1Cl·2PhMe, desolvation of 1X·2PhMe (X = Br, I) in refluxing n-octane (127 °C) or heated mineral oil (170 °C) slurries does not lead to materials with νCN absorptions characteristic of β-[MnTClPP][TCNE]. Upon facile desolvation of dichloromethane solvates, materials with νCN absorptions characteristic of γ-[MnTClPP][TCNE] form as the νCN absorptions remain essentially unchanged [2195 ± 2 (m) and 2135 ± 2 (s) cm−1]. The magnetic data for the [MnTXPP][TCNE] family are consistent with linear chain ferrimagnets comprised of antiferromagnetically coupled S = 2 MnIII sites and S = 1/2 [TCNE]˙− sites with the antiferromagnetic intrachain coupling, Jintra/kB (kB = Boltzmann’s constant) determined from fits to the Seiden expression for isolated chains comprised of alternating S = 1/2 and S = 2 spins. For the [MnTFPP][TCNE] series, Jintra values of −225, −160, −210, and −177 K were obtained for 1F·xxPhMe, β-1F, 1F·2CH22Cl22, and γ-1F, respectively. While Jintra values of −30, −45, −270, and −75 K were observed for 1Br·2PhMe, α-1Br, 2CH22Cl22, and γ-1Br, respectively. Finally, Jintra values of −53, −35, −35, and −53 K were observed for 1I·2PhMe, α-1I, 1I·2CH22Cl22, and γ-1I, respectively. The ordering temperatures, Tc, determined from the maxima in the 10 Hz χ′(T) ranged from 6.5 K (1I·2PhMe) to 28 K for (1F·xxPhMe). Based on the magnetic behavior, desolvation of 1X·PhMe and 1X·CH22Cl22 increases the magnetic disorder and subsequent spin glass behavior as well as changing the observed interchain magnetic coupling.