Structure and dynamics of associated molecular systems. IV. The orientationally disordered phase I of solid DCl

1980 ◽  
Vol 73 (1) ◽  
pp. 532-537 ◽  
Author(s):  
Ian R. McDonald ◽  
David G. Bounds ◽  
Michael L. Klein
2020 ◽  
Vol 11 (1) ◽  
Author(s):  
Hongxiang Zong ◽  
Heather Wiebe ◽  
Graeme J. Ackland

Abstract The hydrogen phase diagram has several unusual features which are well reproduced by density functional calculations. Unfortunately, these calculations do not provide good physical insights into why those features occur. Here, we present a fast interatomic potential, which reproduces the molecular hydrogen phases: orientationally disordered Phase I; broken-symmetry Phase II and reentrant melt curve. The H2 vibrational frequency drops at high pressure because of increased coupling between neighbouring molecules, not bond weakening. Liquid H2 is denser than coexisting close-packed solid at high pressure because the favored molecular orientation switches from quadrupole-energy-minimizing to steric-repulsion-minimizing. The latter allows molecules to get closer together, without the atoms getting closer, but cannot be achieved within in a close-packed layer due to frustration. A similar effect causes negative thermal expansion. At high pressure, rotation is hindered in Phase I, such that it cannot be regarded as a molecular rotor phase.


2021 ◽  
Author(s):  
Y. Cohen ◽  
Sarit Slovak ◽  
Liat Avram

NMR has been instrumental in studies of both the structure and dynamics of molecular systems for decades, so it is not surprising that NMR has played a pivotal role in...


1979 ◽  
Vol 71 (9) ◽  
pp. 3673-3682 ◽  
Author(s):  
Michael L. Klein ◽  
Ian R. McDonald ◽  
Roberto Righini

2012 ◽  
Vol 68 (4) ◽  
pp. 389-400 ◽  
Author(s):  
Maxime A. Siegler ◽  
Sean Parkin ◽  
Carolyn Pratt Brock

A sequence of four phases has been found for an acetonitrile-solvated co-crystal with 15-crown-5 of the nickel complex [acetonitrilediaqua-κ1 O-nitrato-κ2 O-nitratonickel(II)]. The structure could be determined at intervals of ca 10 K in the range 90–273 K because crystals remain single through the three transitions. In phase (I) (T ≥ ca 240 K; P21/m, Z′ = ½), there is extensive disorder, which is mostly resolved in phase (III) (ca 230–145 K; P21/c, Z′ = 1). Phase (IV) (ca 145–90 K, and probably below; P\overline 1, Z′ = 2) is ordered. Phase (II) (ca 238–232 K) is modulated, but the satellite reflections are too weak to allow the structure to be determined within its stability range by standard methods. Most crystals that were flash-cooled from room temperature to 90 K have a metastable P21, Z′ = 5 superstructure that (at least in a commensurate approximation) was identified as similar to the structure of phase (II) by comparison of reconstructed reciprocal-lattice slices and by analogy with the phase behavior of the very similar compound [Ni(H2O)6](NO3)2·(15-crown-5)·2H2O [Siegler et al. (2011). Acta Cryst. B67, 486–498]. In the phase (II) structure slab-like regions that are like the disordered phase (I) structure alternate with regions of similar shape and size that are like the more ordered phase (III) structure.


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