A study of the known and hypothetical crystal structures of pyridine: why are there four molecules in the asymmetric unit cell?

CrystEngComm ◽  
2002 ◽  
Vol 4 (62) ◽  
pp. 348-355 ◽  
Author(s):  
A. T. Anghel ◽  
G. M. Day ◽  
S. L. Price
2014 ◽  
Vol 70 (a1) ◽  
pp. C336-C336
Author(s):  
Marcin Kowiel ◽  
Mariusz Jaskolski ◽  
Andrzej Gzella ◽  
Zbigniew Dauter

Unique choice of the unit cell and the asymmetric unit are well defined and described in the International Tables for Crystallography vol. A. Unfortunately, the placement of molecules within the unit cell is not standardized. Since structure solution programs often use random numbers in their algorithms, the selected set of atomic coordinates may be different even with successive runs of the same program. Although formally correct, an arbitrary choice of molecular placement within the unit cell is confusing and may lead to interpretation errors [1]. With the use of the anti-Cheshire unit cell introduced by Dauter [2], for all space groups without inversion symmetry, it is possible to transform the molecular model such that its center of gravity falls within the anti-Cheshire asymmetric unit cell. It means that for macromolecular crystal structures it should be possible to standardize the placement of the molecules within the unit cell. In consequence, it should be easier for crystallographers and non-crystallographers to compare similar or related crystal structures. An implementation of the anti-Cheshire concept has been programmed in Python as a web service, aCHESYM. The aCHESYM program takes a PDB file as input and transforms the macromolecular model into the desired anti-Cheshire region. The program can also handle structure factor CIF files if the transformation used requires reindexing of the reflection data. The unit cell, coordinates and displacement parameters of all atoms after transformation are saved in a new PDB file. All the calculated transformations are reversible, so there is no danger of data loss. Moreover, the program helps the user to find the most compact assembly of the molecules (chains) in the structure when there are several chains in the asymmetric unit.


Crystals ◽  
2021 ◽  
Vol 11 (8) ◽  
pp. 857
Author(s):  
Nabyl Merbouh ◽  
Simon Cassegrain ◽  
Wen Zhou

The crystal structures are reported for two unsubstituted arylnaphthalene lactones, 4-phenylnaphtho[2,3-c]furan-1(3H)-one (2), 9-phenylnaphtho[2,3-c]furan-1(3H)-one (3) and a non-aromatic dihydro arylnaphthene lactone, 3a,4-dihydro-9-phenylnaphtho[2,3-c]furan-1(3H)-one (5). There are only minor differences in the geometrical parameters of these structures. However, in certain cases, both isomers of arylnaphthalene lactones (termed Type I and Type II) were found in the same asymmetric unit cell.


2011 ◽  
Vol 99 (24) ◽  
pp. 243504 ◽  
Author(s):  
V. V. Popov ◽  
D. V. Fateev ◽  
T. Otsuji ◽  
Y. M. Meziani ◽  
D. Coquillat ◽  
...  

2021 ◽  
Author(s):  
K.V. Mashinsky ◽  
V.V. Popov ◽  
D.V. Fateev

Problem formulating. Lasing on strong («radiative») plasmon resonance mode in graphene structure with dual grating gate with asymmetric unit cell requires strong gain. It is possible to achieve lasing in a weak ("non-radiative") mode at a lower gain rate. Goal. Theoretical study of laser generation on weak plasmonic resonance mode in single layer graphene structure screened by dual grating gate with asymmetric unit cell. Result. Laser generation on weak plasmonic resonance mode in single layer graphene structure screened by dual grating gate with asymmetric unit cell is reached. Excitation of a weak plasmon resonance mode requires less gain than excitation of a radiative one. Practical meaning. Results can be used to create sources of terahertz waves.


1996 ◽  
Vol 29 (3) ◽  
pp. 301-303 ◽  
Author(s):  
W. Kraus ◽  
G. Nolze

The main component of this program is a simultaneous representation of the unit cell and the calculated powder pattern. It allows the manipulation of the crystal structure by moving selected atoms of the asymmetric unit. The resulting powder pattern can be directly compared to experimental data in order to obtain reliable starting values for further computations in refinement programs.


Author(s):  
Van-Viet Nguyen ◽  
Hyohyun Nam ◽  
Bok-Hyung Lee ◽  
Muk-Kyo Lee ◽  
Sun-Youl Choi ◽  
...  

1999 ◽  
Vol 101 (1-3) ◽  
pp. 490-491 ◽  
Author(s):  
Denis Jacquemin ◽  
Rendît Champagne ◽  
Jean-Marie André

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