The structure of α, β, γ, δ-tetraphenylporphinatodihydroxytin(IV) (TPPSn(OH) 2) has been determined as its bis(chloroform)-bis(carbon tetrachloride) solvate by Patterson and Fourier techniques to a final ‘R’-factor of 15.14% for 4380 independent reflections. Purple crystals of the material are triclinic, space group P1, with a = 12.229(6), b = 12.310(9), c = 9.592(8) Å, α = 102.58(1), β = 109.64(5), γ = 91.78(8)°, and are composed of stacks of non-interacting TPPSn(OH) 2 molecules, with the solvate molecules occupying spaces in the lattice. The geometry at the tin is only slightly distorted from regular octahedral, with SnN bonds of normal length (2.09(5) Å), but with very short bonds to oxygen (2.00(3) and 2.03(5) Å). Tin-119 Mössbauer resonance area data have been collected in the temperature range 77 ⩽ T ⩽ 153 K, and a semi-logarithmic plot of resonance area versus temperature is linear in this temperature range, yielding values of the logarithmic temperature coefficient of the recoil-free fraction, a, and of the characteristic Mössbauer temperature, θ M, of −0.01193 K −1 and 122.3 K, respectively. The data have also been used to evaluate the isotropic mean-square amplitudes of vibration, <x iso(T) 2>, of the tin atom, normalised to the value at 298 K available from the crystallographic study, in the same temperature range. Root-mean-square values of the vibrational amplitude range from 0.125 Å at 77 K to 0.148 Å at 153 K. From the Goldanskii-Karyagin effect data, it was concluded that the sign of the electric field gradient, V zz, assumed to be coincident with the pseudo-four-fold axis of the molecule, is negative, and that the tin atom vibrates with greater amplitude in the plane of the porphyrin residue (perpendicular to V zz). The temperature coefficient of the root-mean-square amplitude of vibration is significantly larger in the out-of-plane direction (along the OSnO axis) (4.184 × 10 −4 Å K −1 than in the in-plane direction (2.618 × 10 −4 Å K −1), reflecting the constraining nature of the porphyrin residue. Absolute values of the recoil-free fraction, f a were estimated to be 0.100 at 77 K reducing to 0.0404 at 153 K.
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