New insights into the compressibility and high-pressure stability of Ni(CN)2: a combined study of neutron diffraction, Raman spectroscopy, and inelastic neutron scattering

Nickel cyanide is a layered material showing markedly anisotropic behaviour. High-pressure neutron diffraction measurements show that at pressures up to 20.1 kbar, compressibility is much higher in the direction perpendicular to the layers, c, than in the plane of the strongly chemically bonded metal-cyanide sheets. Detailed examination of the behaviour of the tetragonal lattice parameters, a and c, as a function of pressure reveal regions in which large changes in slope occur, for example, in c(P) at 1 kbar. The experimental pressure dependence of the volume data is fitted to a bulk modulus, B0, of 1050 (20) kbar over the pressure range 0–1 kbar, and to 124 (2) kbar over the range 1–20.1 kbar. Raman spectroscopy measurements yield additional information on how the structure and bonding in the Ni(CN)2 layers change with pressure and show that a phase change occurs at about 1 kbar. The new high-pressure phase, (Phase PII), has ordered cyanide groups with sheets of D4h symmetry containing Ni(CN)4 and Ni(NC)4 groups. The Raman spectrum of phase PII closely resembles that of the related layered compound, Cu1/2Ni1/2(CN)2, which has previously been shown to contain ordered C≡N groups. The phase change, PI to PII, is also observed in inelastic neutron scattering studies which show significant changes occurring in the phonon spectra as the pressure is raised from 0.3 to 1.5 kbar. These changes reflect the large reduction in the interlayer spacing which occurs as Phase PI transforms to Phase PII and the consequent increase in difficulty for out-of-plane atomic motions. Unlike other cyanide materials e.g. Zn(CN)2 and Ag3Co(CN)6, which show an amorphization and/or a decomposition at much lower pressures (~100 kbar), Ni(CN)2 can be recovered after pressurising to 200 kbar, albeit in a more ordered form.

[1]  M. Zbiri,et al.  Chemistry and structure by design: ordered CuNi(CN)4 sheets with copper(ii) in a square-planar environment. , 2015, Dalton transactions.

[2]  M. Cliffe,et al.  Negative area compressibility in silver(I) tricyanomethanide. , 2013, Chemical communications.

[3]  V. Michaelis,et al.  Local and average structure in zinc cyanide: toward an understanding of the atomistic origin of negative thermal expansion. , 2013, Journal of the American Chemical Society.

[4]  A. Goodwin,et al.  Structural disorder in molecular framework materials. , 2013, Chemical Society reviews.

[5]  Chiu C Tang,et al.  Homologous critical behavior in the molecular frameworks Zn(CN)2 and Cd(imidazolate)2. , 2013, Journal of the American Chemical Society.

[6]  C. Parlak FT-IR and Raman spectroscopic analysis of some Hofmann type complexes. , 2012, Spectrochimica acta. Part A, Molecular and biomolecular spectroscopy.

[7]  Aihua Yuan,et al.  Ligand-concentration-dependent self-organization of Hoffman- and PtS-type frameworks from one-pot crystallization , 2011 .

[8]  A. K. Tyagi,et al.  Raman spectroscopic study of high-pressure behavior of Ag 3 [Co(CN) 6 ] , 2011 .

[9]  R. Mittal,et al.  Relationship between phonons and thermal expansion in Zn(CN)2 and Ni(CN)2 from inelastic neutron scattering and ab initio calculations , 2010, 1009.5540.

[10]  Yi-zhi Li,et al.  Three unique two-fold interpenetrated three-dimensional networks with PtS-type topology constructed from [M(CN)4]2− (M = Ni, Pd, Pt) as “square-planar” building blocks , 2010 .

[11]  A. Goodwin,et al.  Aperiodicity, structure, and dynamics in Ni(CN)(2) , 2009 .

[12]  J. Chervin,et al.  Hydrostatic limits of 11 pressure transmitting media , 2009 .

[13]  R. Mittal,et al.  Measurement of anharmonicity of phonons in negative thermal expansion compound Zn(CN)2 by high pressure inelastic neutron scattering , 2009, 0901.3760.

[14]  H. K. Poswal,et al.  Structural phase transitions in Zn(CN)2 under high pressures , 2009 .

[15]  Matthew G. Tucker,et al.  Large negative linear compressibility of Ag3[Co(CN)6] , 2008, Proceedings of the National Academy of Sciences.

[16]  J. Cezar,et al.  Pressure-induced magnetic switching and linkage isomerism in K0.4Fe4[Cr(CN)6]2.8 x 16 H2O: X-ray absorption and magnetic circular dichroism studies. , 2008, Journal of the American Chemical Society.

[17]  T. Hansen,et al.  The D20 instrument at the ILL: a versatile high-intensity two-axis neutron diffractometer , 2008 .

[18]  S. Hibble,et al.  Surprises from a simple material--the structure and properties of nickel cyanide. , 2007, Angewandte Chemie.

[19]  E. Kaxiras,et al.  Semiconducting cyanide-transition-metal nanotubes. , 2007, Small.

[20]  A. Goodwin,et al.  Negative thermal expansion and low-frequency modes in cyanide-bridged framework materials , 2005 .

[21]  A. Cowley,et al.  Copper(I) cyanide: a simple compound with a complicated structure and surprising room-temperature reactivity. , 2004, Angewandte Chemie.

[22]  S. Hibble,et al.  Structure of AuCN determined from total neutron diffraction. , 2003, Inorganic chemistry.

[23]  S. Hibble,et al.  CuCN: a polymorphic material. Structure of one form determined from total neutron diffraction. , 2002, Inorganic chemistry.

[24]  S. Hibble,et al.  Beyond Bragg scattering: the structure of AgCN determined from total neutron diffraction. , 2002, Inorganic chemistry.

[25]  D. E. Partin,et al.  The Disordered Crystal Structures of Zn(CN)2and Ga(CN)3 , 1997 .

[26]  W. G. Marshall,et al.  High pressure neutron diffraction using the paris-edinburgh cell: Experimental possibilities and future prospects , 1996 .

[27]  Juan Rodríguez-Carvajal,et al.  Recent advances in magnetic structure determination by neutron powder diffraction , 1993 .

[28]  Price,et al.  Correlated motions in glasses studied by coherent inelastic neutron scattering. , 1985, Physical review letters.