Rigid unit modes and the phase transition and structural distortions of zeolite rho

1998 ◽  
Vol 25 (1-3) ◽  
pp. 193-200 ◽  
Author(s):  
Anna Bieniok ◽  
Kenton D. Hammonds
2011 ◽  
Vol 25 (20) ◽  
pp. 1671-1681 ◽  
Author(s):  
YURI APARECIDO OPATA ◽  
ANDERSON ROSA KURELO ◽  
LINCOLN BRUM DE LEITE ◽  
GUSMÃO PINHEIRO ◽  
PEDRO RODRIGUES ◽  
...  

A detailed study of the effect caused by the partial substitution of Er by Ce on fluctuation conductivity of the Er 1-x Ce x Ba 2 Cu 3 O 7-δ; 0 ≤ x ≤ 0.10; is presented. The combined experimental results of structural and electrical measurements indicate that Ce substitutes Er for x ≤ 0.10 with no significant structural distortions. However, there is suppression of the superconducting state with zero-resistance state at temperatures ≥ 86.3 K. The results were analyzed in terms of the temperature derivative of the resistivity and the logarithmic temperature derivative of the conductivity to identify power-law divergences of the conductivity. The data revealed the occurrence of a two-stage intragranular-intergranular transition. Above the critical temperature, the Gaussian and critical regimes were observed. Also, from the critical exponents analysis, we observed a splitting of the pairing transition for Ce -doped samples, suggesting the occurrence of a phase separation. On approaching the zero resistance state, our results showed a power-law behavior that corresponds to a phase transition from a paracoherent to a coherent state of the granular array and which does not depend on Ce doping.


2000 ◽  
Vol 27 (4) ◽  
pp. 285-290 ◽  
Author(s):  
S. A. Hayward ◽  
A. K. A. Pryde ◽  
R.F. de Dombal ◽  
M. A. Carpenter ◽  
M. T. Dove

1995 ◽  
Vol 59 (397) ◽  
pp. 629-639 ◽  
Author(s):  
Martin T. Dove ◽  
Volker Heine ◽  
Kenton D. Hammonds

AbstractWe describe a model for framework silicates in which the SiO4 (and AlO4) tetrahedra are treated as perfectly rigid and freely jointed. From this model we are able to identify low-energy modes of distortion of the structure, which we call Rigid unit modes. These modes can act as soft modes to allow easy distortions at phase transition. We discuss three forces that will operate at a phase transition in conjunction with the candidate soft modes to determine which of the rigid unit modes will actually precipitate a phase transition, and illustrate these ideas by detailed discussions of the phase transitions in quartz, leucite and cristobalite. The model can also be used to estimate the transition temperature, and the theory highlights an important role for the stiffness of the tetrahedra.


1994 ◽  
Vol 72 (19) ◽  
pp. 3132-3132
Author(s):  
B. Rechav ◽  
Y. Yacoby ◽  
E. A. Stern ◽  
J. J. Rehr ◽  
M. Newville

2001 ◽  
Vol 57 (4) ◽  
pp. 507-516 ◽  
Author(s):  
Aibing Xia ◽  
John P. Selegue ◽  
Alberto Carrillo ◽  
Brian O. Patrick ◽  
Sean Parkin ◽  
...  

Structures of two derivatives of the curved fluoradene ring system (C19H12) have been determined. Both have phases that are highly pseudosymmetric. At room temperature crystals of 7b-triisopropylsilylfluoradene (C28H32Si) have a P\bar 1 cell that contains two independent molecules (Z′ = 2) and that is almost centered. Crystals of 7b-(2,4-dinitrophenyl)fluoradene (C25H14N2O4) have both a P21/c cell with Z′ = 1 and a P21/c cell with Z′ = 2. The molecular volumes in these two P21/c structures differ by 0.7%, but the structures are otherwise virtually the same; the two independent molecules in the larger cell are related by a pseudotranslation. Some of the atomic ellipsoids in the P21/c, Z′ = 1 structure are very large and eccentric, and there are some hints in the diffraction pattern of an incipient phase transition, but the Z′ = 1 and Z′ = 2 phases are clearly different. The P21/c, Z′ = 2 crystal at 295 K probably contains some volume fraction of the Z′ = 1 phase; when the temperature is lowered to 273 K this fraction is decreased markedly. The pronounced pseudosymmetry in the P\bar 1 and P21/c structures that have Z′ = 2 has been investigated by analysing the atomic coordinates, by performing refinements in the smaller pseudocells and by making separate Wilson plots for the classes of reflections which are systematically strong and systematically weak. All three approaches are informative, but they reveal different information. Least-squares fits of coordinates of corresponding atoms measure the similarity of the molecular conformations. The Wilson plots allow a quantitative comparison of the intensities of the strong and weak reflections and thus an assessment of the deviations of the true structure from the smaller pseudocell structure. Comparison of the atomic displacements obtained in the full and pseudocell refinements shows where the structural distortions are largest and provides an indication of their directions."


2001 ◽  
Vol 123 (34) ◽  
pp. 8418-8419 ◽  
Author(s):  
Yongjae Lee ◽  
Joseph A. Hriljac ◽  
Thomas Vogt ◽  
John B. Parise ◽  
Michael J. Edmondson ◽  
...  

2021 ◽  
Vol 12 (1) ◽  
Author(s):  
Christoph G. Salzmann ◽  
John S. Loveday ◽  
Alexander Rosu-Finsen ◽  
Craig L. Bull

AbstractIce is a material of fundamental importance for a wide range of scientific disciplines including physics, chemistry, and biology, as well as space and materials science. A well-known feature of its phase diagram is that high-temperature phases of ice with orientational disorder of the hydrogen-bonded water molecules undergo phase transitions to their ordered counterparts upon cooling. Here, we present an example where this trend is broken. Instead, hydrochloric-acid-doped ice VI undergoes an alternative type of phase transition upon cooling at high pressure as the orientationally disordered ice remains disordered but undergoes structural distortions. As seen with in-situ neutron diffraction, the resulting phase of ice, ice XIX, forms through a Pbcn-type distortion which includes the tilting and squishing of hexameric clusters. This type of phase transition may provide an explanation for previously observed ferroelectric signatures in dielectric spectroscopy of ice VI and could be relevant for other icy materials.


MRS Advances ◽  
2016 ◽  
Vol 1 (9) ◽  
pp. 609-614 ◽  
Author(s):  
Venkateswara rao Mannepalli ◽  
Ranjith Ramadurai

ABSTRACTYCrO3 (YCO) is known to be a multiferroic with orthorhombic, Pnma, structure with center of inversion. However, the local structural inhomogeneity in this compound is believed to give rise to ferroelectric behavior. In this study we explore high temperature Raman investigations of YCO and observed that one of its Raman mode B3g (3) (CrO6 Octahedral tilt mode) softens around the structural phase transition which could be the origin of ferroelectric nature in YCO. In addition, we substitute bismuth (Bi) in YCO to understand the structural distortions that lead to local structural inhomogeneity. Besides B3g (3) mode softening with composition and high temperature studies in Y1-xBixCrO3 the study reveals the structural distortions and the structural tunability Bi offers in such systems.


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