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001     53865
005     20180211184355.0
024 7 _ |2 DOI
|a 10.1142/S0217979206034315
024 7 _ |2 WOS
|a WOS:000238104400005
037 _ _ |a PreJuSER-53865
041 _ _ |a eng
082 _ _ |a 530
084 _ _ |2 WoS
|a Physics, Applied
084 _ _ |2 WoS
|a Physics, Condensed Matter
084 _ _ |2 WoS
|a Physics, Mathematical
100 1 _ |a Hauck, J.
|b 0
|u FZJ
|0 P:(DE-Juel1)VDB567
245 _ _ |a Interactions from Self-Coordination Numbers - A Physical Relation Without Formula
260 _ _ |a Singapore [u.a.]
|b World Scientific Publ.
|c 2006
300 _ _ |a 2065 - 2084
336 7 _ |a Journal Article
|0 PUB:(DE-HGF)16
|2 PUB:(DE-HGF)
336 7 _ |a Output Types/Journal article
|2 DataCite
336 7 _ |a Journal Article
|0 0
|2 EndNote
336 7 _ |a ARTICLE
|2 BibTeX
336 7 _ |a JOURNAL_ARTICLE
|2 ORCID
336 7 _ |a article
|2 DRIVER
440 _ 0 |a International Journal of Modern Physics B
|x 0217-9792
|0 7945
|v 20
500 _ _ |a Record converted from VDB: 12.11.2012
520 _ _ |a A large number of homogeneous particles A with different A-A interactions like carbon atoms in diamond, CO3 ions in CaCO3, S-6 molecules in rhombic sulphur, colloid or micelle particles are ordered in such a way that the bulk structure can be characterized by the self-coordination numbers T-i, i = 1 - 3 of nearest, second and third neighbors. There are about 500 sets with increased T-i values (aristotypes) and about 500 sets with reduced Ti values, which axe obtained from characteristic lattice complexes. The number k = 1, 2, 3, etc. of the (T-1 T-2 T-3) aristotype is added to the Wyckoff letters of standardized structures like 167-b9a9 or 148-a4 for the Ca(CO3) or (S-6) structures with the centers of (CO3) or (S-6). groups. Two or more particles A, B, etc. can belong to the same aristotype like Na and Cl atoms in NaCl or Li, Ag and Sb atoms in Li2AgSb. All possible structures of an aristotype are within certain limits of Ti values in a Ti, i = 1 - 3 coordinate system, the structure map. The location of A, B, etc. positions on structure maps can be related with repulsive or attractive interactions at high or low T-2 values. The plate- or rod-like habit of single crystals can frequently be related to layered or rod-like packings (T-1 T-2 T-3) of the constituents.
536 _ _ |a Kondensierte Materie
|c P54
|2 G:(DE-HGF)
|0 G:(DE-Juel1)FUEK414
|x 0
588 _ _ |a Dataset connected to Web of Science
650 _ 7 |a J
|2 WoSType
653 2 0 |2 Author
|a characteristic lattice complexes
653 2 0 |2 Author
|a crystal habit
653 2 0 |2 Author
|a Madelung factor
653 2 0 |2 Author
|a structure map
653 2 0 |2 Author
|a Ising model
700 1 _ |a Mika, K.
|b 1
|u FZJ
|0 P:(DE-Juel1)VDB1064
773 _ _ |a 10.1142/S0217979206034315
|g Vol. 20, p. 2065 - 2084
|p 2065 - 2084
|q 20<2065 - 2084
|0 PERI:(DE-600)2086681-1
|t International journal of modern physics / B
|v 20
|y 2006
|x 0217-9792
856 7 _ |u http://dx.doi.org/10.1142/S0217979206034315
909 C O |o oai:juser.fz-juelich.de:53865
|p VDB
913 1 _ |k P54
|v Kondensierte Materie
|l Kondensierte Materie
|b Materie
|z entfällt bis 2009
|0 G:(DE-Juel1)FUEK414
|x 0
914 1 _ |y 2006
915 _ _ |0 StatID:(DE-HGF)0010
|a JCR/ISI refereed
920 1 _ |k IFF-IEM
|l Elektronische Materialien
|d 31.12.2006
|g IFF
|0 I:(DE-Juel1)VDB321
|x 1
920 1 _ |k IFF-TH-III
|l Theorie III
|d 31.12.2006
|g IFF
|0 I:(DE-Juel1)VDB32
|x 0
970 _ _ |a VDB:(DE-Juel1)84536
980 _ _ |a VDB
980 _ _ |a ConvertedRecord
980 _ _ |a journal
980 _ _ |a I:(DE-Juel1)PGI-7-20110106
980 _ _ |a I:(DE-Juel1)PGI-2-20110106
980 _ _ |a UNRESTRICTED
981 _ _ |a I:(DE-Juel1)PGI-7-20110106
981 _ _ |a I:(DE-Juel1)PGI-2-20110106

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