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000053865 041__ $$aeng
000053865 082__ $$a530
000053865 084__ $$2WoS$$aPhysics, Applied
000053865 084__ $$2WoS$$aPhysics, Condensed Matter
000053865 084__ $$2WoS$$aPhysics, Mathematical
000053865 1001_ $$0P:(DE-Juel1)VDB567$$aHauck, J.$$b0$$uFZJ
000053865 245__ $$aInteractions from Self-Coordination Numbers - A Physical Relation Without Formula
000053865 260__ $$aSingapore [u.a.]$$bWorld Scientific Publ.$$c2006
000053865 300__ $$a2065 - 2084
000053865 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article
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000053865 440_0 $$07945$$aInternational Journal of Modern Physics B$$v20$$x0217-9792
000053865 500__ $$aRecord converted from VDB: 12.11.2012
000053865 520__ $$aA 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.
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000053865 650_7 $$2WoSType$$aJ
000053865 65320 $$2Author$$acharacteristic lattice complexes
000053865 65320 $$2Author$$acrystal habit
000053865 65320 $$2Author$$aMadelung factor
000053865 65320 $$2Author$$astructure map
000053865 65320 $$2Author$$aIsing model
000053865 7001_ $$0P:(DE-Juel1)VDB1064$$aMika, K.$$b1$$uFZJ
000053865 773__ $$0PERI:(DE-600)2086681-1$$a10.1142/S0217979206034315$$gVol. 20, p. 2065 - 2084$$p2065 - 2084$$q20<2065 - 2084$$tInternational journal of modern physics / B$$v20$$x0217-9792$$y2006
000053865 8567_ $$uhttp://dx.doi.org/10.1142/S0217979206034315
000053865 909CO $$ooai:juser.fz-juelich.de:53865$$pVDB
000053865 9131_ $$0G:(DE-Juel1)FUEK414$$bMaterie$$kP54$$lKondensierte Materie$$vKondensierte Materie$$x0$$zentfällt   bis 2009
000053865 9141_ $$y2006
000053865 915__ $$0StatID:(DE-HGF)0010$$aJCR/ISI refereed
000053865 9201_ $$0I:(DE-Juel1)VDB321$$d31.12.2006$$gIFF$$kIFF-IEM$$lElektronische Materialien$$x1
000053865 9201_ $$0I:(DE-Juel1)VDB32$$d31.12.2006$$gIFF$$kIFF-TH-III$$lTheorie III$$x0
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