The
atomic-scale picture of the proton conduction mechanism in
tin pyrophosphate, SnP2O7, has theoretically
been investigated using first-principles calculations, to clarify
the intrinsic proton conductivity in the bulk region. Protons in the
crystal lattice reside around oxide ions and migrate by rotation around
single oxide ions and hopping between adjacent oxide ions by a mechanism
similar to that in other proton-conducting oxides. The calculated
proton conductivity has weak anisotropy reflecting the monoclinic
structure (unique axis: b), particularly in the ca-plane. The main origin of the anisotropic conductivity
is the relatively fast long-range migration pathways along the unique b-axis and in the [101] direction (potential barrier: 0.57
eV) versus that along the [101̅] direction (potential barrier:
0.64 eV). The apparent activation energy of the estimated proton conductivity
is as high as ∼1.1 eV with the proton trapping effect by dopants
(association energy: 0.59 eV), leading to the low proton conductivity
in the bulk region. This suggests that the reported fast proton conductivity
in the literature may be due to other unexpected proton migration
routes, such as surfaces, grain boundaries, and secondary phases with
residual phosphoric acid.