Abstract:High-resolution neutron powder diffraction data were used to determine the crystal structure of the superionic conductor CsDSO4 at 300K (lowconductivity phase) and at 448 K (superionic phase). A full structural analysis was performed, using the Rietveld method, to obtain previously unknown atomic positions, site occupancies and temperature factors for the light atoms. The mechanism of deuterium diffusion is discussed. At 300 K: monoclinic, P2~/c, a = 7.78013 (9), b = 8.13916 (2), c = 7.72187 (9) A, fl = 110.87… Show more
“…The arrangement of Cs cations and XO 4 anions in Cs 2 (HSO 4 )(H 2 PO 4 ) is very similar to that in -Cs 3 (HSO 4 ) 2 (H 2 À x (S x P 1 À x )O 4 ) , -Cs 3 (HSO 4 ) 2 (H 2 PO 4 ) and CsHSO 4 (II) (Belushkin et al, 1991). All three of these compounds are also based on zigzag Cs and XO 4 chains, which again alternate in a checkerboard fashion.…”
Section: Comparison To Related Structuresmentioning
confidence: 73%
“…In CsHSO 4 (II) each XO 4 group is, by de®nition, a sulfate and hydrogen bonds exist only along the chain. The proton to XO 4 group ratio is 1:1 and, accordingly, two hydrogen bonds are formed per tetrahedral unit (Belushkin et al, 1991). InCs 3 (HSO 4 ) 2 (H 2 PO 4 ) every third XO 4 group along the chain is a phosphate group.…”
Section: Comparison To Related Structuresmentioning
Ongoing studies of the CsHSO 4 ±CsH 2 PO 4 system, aimed at developing novel proton conducting solids, resulted in the new compound Cs 2 (HSO 4 )(H 2 PO 4 ) (dicesium hydrogensulfate dihydrogenphosphate). Single-crystal X-ray diffraction (performed at room temperature) revealed Cs 2 (HSO 4 )(H 2 PO 4 ) to crystallize in space group P2 1 /n with lattice parameters a = 7.856 (8), b = 7.732 (7), c = 7.827 (7) A Ê , and = 99.92 (4). The compound has a unit-cell volume of 468.3 (8) A Ê 3 and two formula units per cell, giving a calculated density of 3.261 Mg m
À3. Six non-H atoms and two H atoms were located in the asymmetric unit, with SO 4 and PO 4 groups randomly arranged on the single tetrahedral anion site. Re®nement using all observed re¯ections yielded weighted residuals of 0.0890 and 0.0399 based on F 2 and F values, respectively. Anisotropic temperature factors were employed for all six non-H atoms and ®xed isotropic temperature factors for the two H atoms. The structure contains zigzag chains of hydrogen-bonded anion tetrahedra that extend in the [010] direction. Each tetrahedron is additionally linked to a tetrahedron in a neighboring chain to give a planar structure with hydrogen-bonded sheets lying parallel to (1 Å 01). Thermal analysis of the superprotonic transition in Cs 2 (HSO 4 )(H 2 PO 4 ) showed that the transformation to the high-temperature phase occurs by a two-step process. The ®rst is a sharp transition at 334 K and the second a gradual transition from 342 to 378 K. The heat of transformation for the entire process ($330±382 K) is 44 AE 2 J g
À1. Thermal decomposition of Cs 2 (HSO 4 )(H 2 PO 4 ) takes place at much higher temperatures, with an onset of approximately 460 K.
“…The arrangement of Cs cations and XO 4 anions in Cs 2 (HSO 4 )(H 2 PO 4 ) is very similar to that in -Cs 3 (HSO 4 ) 2 (H 2 À x (S x P 1 À x )O 4 ) , -Cs 3 (HSO 4 ) 2 (H 2 PO 4 ) and CsHSO 4 (II) (Belushkin et al, 1991). All three of these compounds are also based on zigzag Cs and XO 4 chains, which again alternate in a checkerboard fashion.…”
Section: Comparison To Related Structuresmentioning
confidence: 73%
“…In CsHSO 4 (II) each XO 4 group is, by de®nition, a sulfate and hydrogen bonds exist only along the chain. The proton to XO 4 group ratio is 1:1 and, accordingly, two hydrogen bonds are formed per tetrahedral unit (Belushkin et al, 1991). InCs 3 (HSO 4 ) 2 (H 2 PO 4 ) every third XO 4 group along the chain is a phosphate group.…”
Section: Comparison To Related Structuresmentioning
Ongoing studies of the CsHSO 4 ±CsH 2 PO 4 system, aimed at developing novel proton conducting solids, resulted in the new compound Cs 2 (HSO 4 )(H 2 PO 4 ) (dicesium hydrogensulfate dihydrogenphosphate). Single-crystal X-ray diffraction (performed at room temperature) revealed Cs 2 (HSO 4 )(H 2 PO 4 ) to crystallize in space group P2 1 /n with lattice parameters a = 7.856 (8), b = 7.732 (7), c = 7.827 (7) A Ê , and = 99.92 (4). The compound has a unit-cell volume of 468.3 (8) A Ê 3 and two formula units per cell, giving a calculated density of 3.261 Mg m
À3. Six non-H atoms and two H atoms were located in the asymmetric unit, with SO 4 and PO 4 groups randomly arranged on the single tetrahedral anion site. Re®nement using all observed re¯ections yielded weighted residuals of 0.0890 and 0.0399 based on F 2 and F values, respectively. Anisotropic temperature factors were employed for all six non-H atoms and ®xed isotropic temperature factors for the two H atoms. The structure contains zigzag chains of hydrogen-bonded anion tetrahedra that extend in the [010] direction. Each tetrahedron is additionally linked to a tetrahedron in a neighboring chain to give a planar structure with hydrogen-bonded sheets lying parallel to (1 Å 01). Thermal analysis of the superprotonic transition in Cs 2 (HSO 4 )(H 2 PO 4 ) showed that the transformation to the high-temperature phase occurs by a two-step process. The ®rst is a sharp transition at 334 K and the second a gradual transition from 342 to 378 K. The heat of transformation for the entire process ($330±382 K) is 44 AE 2 J g
À1. Thermal decomposition of Cs 2 (HSO 4 )(H 2 PO 4 ) takes place at much higher temperatures, with an onset of approximately 460 K.
“…For example, SO groups may take on multiple orientations, such that different oxygen atoms participate in H bonds in different orientations. Precisely this type of disorder is observed in the high-temperature, superprotonic structure of CsHSO (phase I) (16). Moreover, it is precisely this type of disorder-sulfate groups undergoing rapid reorientation-that facilitates proton transport and results in high conductivity.…”
“…The special attention is paid to the crystals with hydrogen bonds that exhibit transition to superprotonic (superionic) phase with high conductivity that arises due to the motion of protons. Extensive experimental studies of these systems (see [2] for a review) revealed that the charge transfer occurs within the network of hydrogen bonds that connect ionic groups and form, in particular, quasi-one-dimensional (chain-like) [3][4][5] structures. For various crystals it was shown that superionic phase transition is driven by the transformation in proton subsystem (see [2] for review).…”
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