HIGH-PRESSURE, LOW-TEMPERATURE, SINGLE-CRYSTAL NEUTRON-DIFFRACTION STUDY OF DEUTERATED AND HYDROGENOUS AMMONIUM HEXAAQUACOPPER(II) SULFATE (TUTTONS SALT) - A PRESSURE-SWITCHABLE JAHN-TELLER DISTORTION

Citation
Cj. Simmons et al., HIGH-PRESSURE, LOW-TEMPERATURE, SINGLE-CRYSTAL NEUTRON-DIFFRACTION STUDY OF DEUTERATED AND HYDROGENOUS AMMONIUM HEXAAQUACOPPER(II) SULFATE (TUTTONS SALT) - A PRESSURE-SWITCHABLE JAHN-TELLER DISTORTION, Journal of the American Chemical Society, 115(24), 1993, pp. 11304-11311
Citations number
41
Categorie Soggetti
Chemistry
ISSN journal
00027863
Volume
115
Issue
24
Year of publication
1993
Pages
11304 - 11311
Database
ISI
SICI code
0002-7863(1993)115:24<11304:HLSNS>2.0.ZU;2-W
Abstract
The first example of a pressure-induced Jahn-Teller distortion switch has been observed in a single-crystal time-of-flight neutron diffracti on study of the Tutton salt (ND4)2[CuD2O6](SO4)2 at T = 15 K, P = 1 ba r (D(L) and T = 15 K, P = 1.5 kbar (D(H)). Also studied was the hydrog enous salt (NH4)2[Cu(H2O)6](SO4)2 at T = 14 K, P = 1.4 kbar (H(H)). Th e unit cell parameters are as follows: D(L), a = 9.451(2) angstrom, b = 12.736(3) angstrom, c = 6.096(1) angstrom, beta = 107.13(2)degrees, Z = 2, V = 701.2(3) angstrom3, space group = P2(1)/a; D(H), a = 9.136( i) angstrom, b = 12.285(2) angstrom, c = 6.371(1) angstrom, beta = 106 .28(2)degrees, Z = 2, V = 686.4(2) angstrom3, space group = P2(1)/a; H (H), a = 9.068(2) angstrom, b = 12.232(2) angstrom, c = 6.340(1) angst rom, beta = 106.44(2), Z = 2, V = 674.5(2) angstrom3, space group = P2 (1)/a. Application of 1.5 kbar of pressure to the deuterated crystal p roduces a decrease in the lengths of the a and b axes by 0.315(2) and 0.451(4) angstrom, respectively, whereas the c axis increases by 0.275 (1) angstrom. Comparison of the D(L) and D(H) structures shows that th e long axis of the Jahn-Teller distortion has switched by 90-degrees, i.e., Cu(1)-O(7) = 2.022(2) and Cu(1)-O(8) = 2.310(2) angstrom for D(L ) vs Cu(1)-O(7) = 2.290(2) and Cu(1)-O(8) = 2.014(2) angstrom for D(H) , so that the D(H) and H(H) structures are similar. For H(H) Cu(1)-O(7 ) = 2.272(2) and Cu(1)-O(8) = 2.005(2) angstrom. The switching of the long axis of the Jahn-Teller distortion appears to be associated with the rotation of the ND4+ ion with a concomitant change in the hydrogen bonding of the coordinated water molecules with the SO42- ions. The r esulting adiabatic potential energy surfaces are calculated using tetr agonal and orthorhombic strain parameters estimated from the temperatu re variation of the Cu-O bond lengths.