scholarly journals 1-(4-Chlorophenyl)-3-(4-methoxyphenyl)prop-2-en-1-one

2006 ◽  
Vol 62 (4) ◽  
pp. o1647-o1649 ◽  
Author(s):  
William T. A. Harrison ◽  
H. S. Yathirajan ◽  
B. K. Sarojini ◽  
B. Narayana ◽  
J. Indira

The geometrical parameters for the title compound, C16H13ClO2, are normal. Packing in a non-centrosymmetric space group, which is consistent with the non-zero second harmonic generation response, may be influenced by a C—H...O interaction.

2019 ◽  
Vol 48 (43) ◽  
pp. 16377-16383 ◽  
Author(s):  
Philip Netzsch ◽  
Harijs Bariss ◽  
Lkhamsuren Bayarjargal ◽  
Henning A. Höppe

Green emitting Tb(HSO4)(SO4) crystallises in the non-centrosymmetric space group P21 and represents a new sulfate non-linear optical material with a SHG response comparable to KH2PO4 (KDP).


2007 ◽  
Vol 63 (11) ◽  
pp. o4367-o4367
Author(s):  
Ray J. Butcher ◽  
Jerry P. Jasinski ◽  
H. J. Ravindra ◽  
S. M. Dharmaprakash

In the title compound, C16H15N3O4, the dihedral angle between the two benzene ring is 16.66 (6)°. The molecule crystallizes in a centrosymmetric space group and hence does not exhibit nonlinear optical second harmonic generation properties. The angle between the mean plane of the 4-nitrophenyl group and the adjacent NCO group is 26.2 (8)°, while the angle between the mean plane of the phenyl ring and its adjacent NCO group is 40.8 (5)°. The dihedral angle between the two NCO groups is 5.2 (3)°. The crystal packing is stabilized by intramolecular C—H...O and intermolecular N—H...O interactions, which link the molecules into chains along the b axis in the bc plane, with the phenyl rings arranged oblique to this plane.


1977 ◽  
Vol 55 (17) ◽  
pp. 3081-3085 ◽  
Author(s):  
K. Ann Kerr ◽  
P. M. Boorman ◽  
B. S. Misener ◽  
J. G. H. van Roode

Crystals of tricyclohexylphosphine sulphide, C18H33PS, are orthorhombic, a = 10.906(2), b = 15.836(2), c = 10.362(2) Å, Z = 4, space group Pn21a. The structure was solved by direct methods and refined by full-matrix least-squares procedures to a final Rω of 0.058 for all 1209 reflexions with sin θ/λ ≤ 0.5377.Although second harmonic generation unambiguously established the correct space group as Pn21a, parameters reported here refer to the centrosymmetric space group Pnma. The geometry at phosphorus is approximately tetrahedral with an average P—C distance of 1.838(2) Å. Angles at phosphorus range from 105.4° to 113.2°. The P=S bond length of 1.966(2) Å is one of the longest bonds of this type so far reported. Rigid body analysis of thermal parameters suggests that the 'true' bond lengths are even longer.


IUCrData ◽  
2017 ◽  
Vol 2 (8) ◽  
Author(s):  
Błażej Dziuk ◽  
Borys Ośmiałowski ◽  
Anna Zakrzewska ◽  
Krzysztof Ejsmont ◽  
Bartosz Zarychta

There is one independent molecule in the asymmetric unit of the title compound, C13H9BF3NO, which crystallizes in the non-centrosymmetric space groupCc. In the molecular structure, the BF2-carrying ring is distorted from planarity and its mean plane makes a dihedral angle of 42.3 (1)° with the 4-fluorophenyl ring. F atoms are involved in all of the short intermolecular contacts of the crystal structure, which link molecules to form chains along [001] and [010].


Author(s):  
Julian Radtke ◽  
Hans-Wolfram Lerner ◽  
Michael Bolte

We have encountered two polymorphs of the title compound, C24H16B2OS2, both of which display almost the same unit-cell parameters. Compound (I) crystallizes in the non-centrosymmetric space group P21 with four molecules in the asymmetric unit. These molecules are related by pseudosymmetry. As a result, the space group looks like P21/c, but the structure cannot be refined successfully in that space group. Compound (II) on the other hand crystallizes in the centrosymmetric space group P21/c with only two molecules in the asymmetric unit. The crystals studied for (I) and (II) were both non-merohedral twins.


2019 ◽  
Vol 43 (24) ◽  
pp. 9354-9363
Author(s):  
Peng Ren ◽  
Yun Yang ◽  
Hao Li ◽  
Zhihua Yang ◽  
Shilie Pan

KCa4B3O9 and K0.59Rb0.41Ca4B3O9 crystallize in the polar space group with moderate SHG responses. Calculations were performed to elucidate the structure–property relationships.


2017 ◽  
Vol 41 (2) ◽  
pp. 79-81 ◽  
Author(s):  
Gui-Mei Tang ◽  
Rui-Hai Chi ◽  
Wen-Zhu Wan ◽  
Yong-Tao Wang ◽  
Yue-Zhi Cui ◽  
...  

Two 3,6-diiodocarbazole derivatives were prepared from the iodination of the corresponding phenylcarbazole. 3,6-Diiodo-9-phenylcarbazole crystallises in the chiral space group P21 and shows good second-harmonic generation effects. Thermogravimetric analysis of the two compounds shows high thermal stabilities, in which the decomposition temperature for 1 and 2 are 273 and 308 °C, respectively.


2006 ◽  
Vol 62 (4) ◽  
pp. o1659-o1661 ◽  
Author(s):  
Ray J. Butcher ◽  
H. S. Yathirajan ◽  
H. G. Anilkumar ◽  
B. K. Sarojini ◽  
B. Narayana

The title compound, C17H15BrOS, crystallizes in a non-centrosymmetric space group and shows significant nonlinear optical activity.


2006 ◽  
Vol 62 (4) ◽  
pp. o1633-o1635 ◽  
Author(s):  
Ray J. Butcher ◽  
H. S. Yathirajan ◽  
H. G. Anilkumar ◽  
B. K. Sarojini ◽  
B. Narayana

The title compound, C17H15FO3, crystallizes in a centrosymmetric space group and thus does not show any non-linear optical activity. There are two molecules in the asymmetric unit.


2001 ◽  
Vol 57 (2) ◽  
pp. 142-150 ◽  
Author(s):  
Karen Friese ◽  
Mois I. Aroyo ◽  
Cesar L. Folcia ◽  
Gotzon Madariaga ◽  
Tomasz Breczewski

The crystal structure of the glaserite-related compound dithallium(I)–molybdate(VI), which at 293 K crystallizes monoclinic, space group C121 with lattice parameters a = 10.565 (3), b = 6.418 (1), c = 8.039 (2) Å, β = 91.05 (4)°, has been determined. The structure was refined as an inversion twin to a final R(F all) value of 0.0611 for 1006 unique reflections [R(F obs) = 0.0285 for 644 observed reflections]. Second-harmonic generation measurements led to a value of d eff = 5.5 ± 0.5 pm V−1 as an estimation of the second-harmonic conversion efficiency at phase matching. Symmetry mode analysis shows that, in general, primary modes have the highest amplitudes, yet surprisingly some of the secondary modes assume amplitudes of comparable magnitude. A comparison of the phase at 293 K with that at 350 K (space group P\overline{3}m1) shows that the main change can be described as a rotation of the molybdate tetrahedra around the trigonal a(b) axis. The molybdate tetrahedra as well as the octahedra around one of the symmetry-independent Tl atoms are more strongly distorted in the monoclinic phase. The coordination number for the other two Tl atoms is decreased from 12 and 10 in the high-symmetry phase to 10 and 9 in the monoclinic phase. Furthermore, the number of common edges between the Tl and Mo coordination polyhedra is reduced and the common face which is observed between them in the high-temperature phase is changed to a common edge in the low-temperature phase. The contribution of the primary symmetry modes leads exactly to this change in the coordination spheres of the atoms.


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