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2
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-
0032561780
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-
Dunitz, J. D.; Harris, K. D. M.; Johnston, R. L.; Kariuki, B. M.; MacLean, E. J.; Psallidas, K.; Schweizer, W. B.; Tykwinski, R. R. J. Am. Chem. Soc., 1998, 120, 13 274.
-
(1998)
J. Am. Chem. Soc.
, vol.120
, pp. 13274
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-
Dunitz, J.D.1
Harris, K.D.M.2
Johnston, R.L.3
Kariuki, B.M.4
MacLean, E.J.5
Psallidas, K.6
Schweizer, W.B.7
Tykwinski, R.R.8
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3
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0344320197
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-
note
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The initial X-ray analysis was based on the assumption of the lower symmetry space group P4/n but the deviation of the derived structure from P4/ nmm was insignificant.
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-
-
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4
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0345614705
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-
note
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Periodic Hartree-Fock calculations with 6-31G** basis set, using the CRYSTAL95 program.
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-
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5
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-
0345182641
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-
University College London
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4NCO: the results reported refer to analysis of the data for the deuterated material. Rietveld refinement of the synchrotron X-ray powder diffracfion data was carried out using the program MPROF (A. D. Murray, A. N. Fitch, University College London, 1989).
-
(1989)
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Murray, A.D.1
Fitch, A.N.2
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6
-
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0344752457
-
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note
-
Although there is usually no difficulty about localizing H atoms in X-ray analysis based on single-crystal diffraction data (apart from the characteristic systematic contraction of apparent X-H bond distances), the reduction of information inherent in powder diffraction pattems can make H atom localization from analysis of X-ray powder diffraction data much more problematic.
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-
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7
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0344752454
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-
unpublished results
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Periodic Hartree-Fock calculations were carried out using the CRYSTAL95 and CRYSTAL98 packages for a range of different basis sets and a range of values of other parameters controlling the calculation (Posada, A.; Johnston, R. L.; Harris, K. D. M., unpublished results), In some cases, a lower energy was obtained for N-H⋯O hydrogen bonding, in others for N-H⋯N. No geometry optimization was carried out, and the positions of all non-hydrogen atoms were fixed at those in the crystal structure. For some calculation conditions, the energetic ordering of the N-H ⋯O and N-H⋯N structures was different depending on whether the coordinates of the non-hydrogen atoms were those determined at 14 K (from the neutron powder diffraction data presented here) or at ambient temperature (reported previously [2] from X-ray powder diffraction data). A more detailed appraisal of computational approaches for investigating this issue is required.
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-
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Posada, A.1
Johnston, R.L.2
Harris, K.D.M.3
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8
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0344320199
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note
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The restrained values were as follows: Situation 1: O-C, 1.174 Å, C-N 1.192 Å: Situation 2: O-C, 1.256 Å, C-N, 1.181 Å. The actual bond lengths obtained in the refinements remained close to these restrained values.
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-
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9
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-
0345614706
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-
note
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wp = 13.71%. The Rietveld difference plots for these refinement calculations are included in the Supporting Information.
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-
-
-
10
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-
0344320198
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-
note
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4, was about 77%.
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-
-
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11
-
-
0345614704
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-
note
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1H and the strong incoherent neutron scattering of the latter.
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-
-
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12
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-
0003727869
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-
4NCO samples were collected at several temperatures (14, 77, 135, 210, 245, 288 K) over the 2θ range 5° to 117°, with a step size of 0.1° and a total data collection time of about 4 h at each temperature. Rietveld refinement of the neutron powder diffraction data was carried out using the program GSAS (Larson, A. C., Von Dreele, R. B., Los Alamos Laboratory Report No. LA-UR-86-748, 1987).
-
(1987)
Los Alamos Laboratory Report No. LA-UR-86-748
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-
Larson, A.C.1
Von Dreele, R.B.2
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13
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0344752455
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note
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-15).
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-
-
-
14
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0344320194
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-
note
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This conclusion was confirmed by Rietveld refinement calculations for a disorder model comprising x % of situation A and (100-x) % of situation B. In such calculations, x refines, within experimental errors, to a value of zero.
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-
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15
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0344320195
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-
note
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Rietveld refinement for situation B was also carried out for the lower space group P4/n but the resulting deviation of the H/D atoms from the mirror planes was insignificant. The description in space group P4/nmm is therefore preferred.
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-
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16
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0344320193
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note
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Crystal data at higher temperatures (77-288 K) are given in Supporting Tables 2-6.
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-
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17
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-
0345614703
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note
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15N NMR chemical shift for the cyanate N without significant change in the isotropic chemical shift for the ammonium N. This may be explained by the fact that hydrogen bonding has a decreased inductive effect on the acceptor N atom of the cyanate anion as the crystal expands. As a consequence, this atom becomes systematically more deshielded as the hydrogen bond distance increases.
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