Elastic neutron scattering in electric-field-biased deuterated betaine calcium chloride dihydrate

1992 ◽  
Vol 46 (5) ◽  
pp. 3098-3100 ◽  
Author(s):  
M. R. Chaves ◽  
A. Almeida ◽  
J. M. Kiat ◽  
W. Schwarz ◽  
J. Schneck ◽  
...  
1993 ◽  
Vol 141 (1) ◽  
pp. 13-17 ◽  
Author(s):  
A. Almeida ◽  
M. R. Craves ◽  
J. L. Ribeiro ◽  
A. Klopperpieper ◽  
H. E. Muser ◽  
...  

1996 ◽  
Vol 52 (5) ◽  
pp. 810-816 ◽  
Author(s):  
J. M. Ezpeleta ◽  
F. J. Zúñiga ◽  
W. Paulus ◽  
A. Cousson ◽  
J. Hlinka ◽  
...  

The structures of the room-temperature and the lowest-temperature ferroelectric phases of fully deuterated betaine (trimethylammonioacetate) calcium chloride dihydrate have been determined by means of elastic neutron diffraction. In previous structural studies the structural distortions of the incommensurate phase at 130 K and the fourfold phase at 90 K were analyzed in terms of symmetry modes. The same approach has been applied in the present case and, as a result, a quantitative comparison of the distortions at different temperatures can be performed. This shows that the Λ 3 (for q ≠ 0) and B 2u (for q = 0) modes, corresponding to the order parameter, are predominant for the three phases. In addition, it has been found that the structure of this primary mode remains essentially unaltered in the three phases. There is only an increase in its global amplitude as the temperature decreases. Accordingly, it can be expected that the structures of the remaining intermediate modulated phases in the transition sequence are similar to that of the first incommensurate phase, except for the change of wavevector values and greater amplitude of the distortion. Crystal data: (CD3)3NCD2COOCaCl2.2D2O, Mr = 279.0, λ = 0.8308 Å, Z = 4, F(000) = 552. At room temperature: Pnma, a = 10.95 (1), b = 10.15 (1), c = 10.82 (1) Å, V = 1203 (2) Å3, Dx = 1.54 g cm−3, μ = 0.10 cm−1, final R = 0.048 for 748 unique observed reflections. At 35 K: Pn21 a, a = 10.905 (9), b = 10.00 (1), c = 10.80 (1) Å, V = 1178 (2) Å3, Dx = 1.57 g cm−3, μ = 0.11 cm−1, final R = 0.042 for 1726 unique observed reflections.


1995 ◽  
Vol 73 (11-12) ◽  
pp. 687-696 ◽  
Author(s):  
Myer Bloom ◽  
Thomas M. Bayerl

After reviewing some of the basic measurements that characterize the study of physical properties of matter using neutron scattering and nuclear magnetic resonance (NMR), connections between information obtained in current research on fluid membranes using these two complementary techniques are explored in two major chapters. In the first, the type of information on the structure of fluid membranes obtained from coherent elastic neutron scattering is compared with that from NMR spectral characteristics. Then, the type of information obtained on dynamical properties from NMR relaxation (T1 and T2) measurements is compared with that from quasi-elastic neutron scattering. Examples of such connections are given with an emphasis on relationships between the time and distance scales intrinsic to neutron scattering and NMR.


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