The low-temperature structure of cis-cisoid-cis-perhydroanthracene, C14H24

1984 ◽  
Vol 40 (8) ◽  
pp. 1463-1465 ◽  
Author(s):  
H. van Koningsveld ◽  
J. M. A. Baas ◽  
B. van de Graaf
Keyword(s):  
Low Temperature ◽  
Temperature Structure

Low-Temperature Structure (T = 235 K) and Structural Phase Transition in [(C2H5)4N]2SnCl6

1987 ◽  
Vol 103 (1) ◽  
pp. 73-78 ◽  
Author(s):  
H. Ketata ◽  
M. H. Ben Ghozlen ◽  
A. Daoud ◽  
I. Pabst
Keyword(s):  
Phase Transition ◽  
Low Temperature ◽  
Structural Phase Transition ◽  
Structural Phase ◽  
Temperature Structure

Single-Crystal X-Ray Scattering Study of Superstructures and Phase Transitions in Graphite-Hno3 and Graphite-Br2 Intercalation Compounds

1982 ◽  
Vol 20 ◽  
Author(s):  
R. Moret ◽  
R. Comes ◽  
G. Furdin ◽  
H. Fuzellier ◽  
F. Rousseaux
Keyword(s):  
Phase Transitions ◽  
Low Temperature ◽  
Room Temperature ◽  
Temperature Phase ◽  
Temperature Structure ◽  
X Ray ◽  
X Ray Scattering ◽  
Scattering Study ◽  
Temperature Liquid ◽  
Low Temperature Phase

ABSTRACTIn α-C5n-HNO3 the condensation of the room-temperature liquid-like diffuse ring associated with the disorder-order transition around 250 K is studied and the low-temperature. superstructure is examined.It is found that β-C8n-HNO3 exhibits an in-plane incommensurate order at room temperature.Two types of graphite-Br2 are found. Low-temperature phase transitions in C8Br are observed at T1 ≍ 277 K and T2 ≍ 297 K. The room-temperature structure of C14Br is reexamined. Special attention is given to diffuse scattering and incommensurability.

scholarly journals Low-temperature structure ofξ′-Al-Pd-Mn optimized byab initiomethods

2011 ◽  
Vol 84 (18) ◽  
Author(s):  
Benjamin Frigan ◽  
Alejandro Santana ◽  
Michael Engel ◽  
Daniel Schopf ◽  
Hans-Rainer Trebin ◽  
...  
Keyword(s):  
Low Temperature ◽  
Temperature Structure

The role of hydrogen bonds in order-disorder transition of a new incommensurate low temperature phase β-[Zn-(C7H4NO4)2]·3H2O

2018 ◽  
Vol 233 (1) ◽  
pp. 17-25 ◽  
Author(s):  
Masoumeh Tabatabaee ◽  
Morgane Poupon ◽  
Václav Eigner ◽  
Přemysl Vaněk ◽  
Michal Dušek
Keyword(s):  
Low Temperature ◽  
Hydrogen Bonds ◽  
Dicarboxylic Acid ◽  
Room Temperature ◽  
Temperature Phase ◽  
Temperature Structure ◽  
Modulated Structure ◽  
Q Vector ◽  
Low Temperature Phase

AbstractThe room temperature structure withP21/csymmetry of the zinc(II) complex of pyridine-2,6-dicarboxylic acid was published by Okabe and Oya (N. Okabe, N. Oya, Copper(II) and zinc(II) complexes of pyridine-2,6-dicarboxylic acid.Acta Crystallogr. C.2000,56, 305). Here we report crystal structure of the low temperature phaseβ-[Zn(pydcH)2]·3H2O, pydc=C7H3NO4, resulting from the phase transition around 200K. The diffraction pattern of the low temperature phase revealed satellite reflections, which could be indexed with q-vector 0.4051(10)b* corresponding to (3+1)Dincommensurately modulated structure. The modulated structure was solved in the superspace groupX21/c(0b0)s0, whereXstands for a non-standard centring vector (½, 0, 0, ½), and compared with the room temperature phase. It is shown that hydrogen bonds are the main driving force of modulation.

scholarly journals Two polymorphs of 1,8-dichloroanthracene

2013 ◽  
Vol 69 (2) ◽  
pp. 199-203 ◽  
Author(s):  
Peter Müller ◽  
Frank R. Fronczek ◽  
Stacey J. Smith ◽  
Teresa Mako ◽  
Mindy Levine
Keyword(s):  
Low Temperature ◽  
Crystal Packing ◽  
Three Dimensional ◽  
Crystal Form ◽  
Temperature Structure ◽  
Orthorhombic Crystal ◽  
Acta Cryst ◽  
Monoclinic Form ◽  
Compound C ◽  
Dimensional Network

A second, monoclinic, polymorph of the title compound, C14H8Cl2, has been found. In addition to the structure of this monoclinic form, the structure of the previously described orthorhombic form [Desvergne, Chekpo & Bouas-Laurent (1978).J. Chem. Soc. Perkin Trans. 2, pp. 84–87; Benites, Maverick & Fronczek (1996).Acta Cryst.C52, 647–648] has been redetermined at low temperature and using modern methods. The low-temperature structure of the orthorhombic form is of significantly higher quality than the previously published structure and additional details can be derived. A comparison of the crystal packing of the two forms with a focus on weak intermolecular C—H...Cl interactions shows the monoclinic structure to have one such interaction linking the molecules into infinite ribbons, while two crystallographically independent C—H...Cl interactions give rise to an interesting infinite three-dimensional network in the orthorhombic crystal form.

Fermi surface and low temperature structure in (DMET-TSeF)2Au(CN)2

2003 ◽  
Vol 135-136 ◽  
pp. 577-578 ◽  
Author(s):  
K. Kato ◽  
K. Oshima ◽  
T. Kambe ◽  
Y. Nogami ◽  
T. Sasaki ◽  
...  
Keyword(s):  
Low Temperature ◽  
Fermi Surface ◽  
Temperature Structure
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