16 research outputs found
Multipopulation Genetic Algorithm for Simulation of the Crystal Structure from X-Ray Diffraction Data
ΠΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½ ΠΌΡΠ»ΡΡΠΈΠΏΠΎΠΏΡΠ»ΡΡΠΈΠΎΠ½Π½ΡΠΉ ΠΏΠ°ΡΠ°Π»Π»Π΅Π»ΡΠ½ΡΠΉ Π³Π΅Π½Π΅ΡΠΈΡΠ΅ΡΠΊΠΈΠΉ Π°Π»Π³ΠΎΡΠΈΡΠΌ Π΄Π»Ρ ΠΌΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΡ
Π°ΡΠΎΠΌΠ½ΠΎΠΉ ΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΡΡΡΠΊΡΡΡΡ Ρ
ΠΈΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½ΠΈΠΉ ΠΈΠ· Π΄Π°Π½Π½ΡΡ
ΡΠ΅Π½ΡΠ³Π΅Π½ΠΎΠ²ΡΠΊΠΎΠΉ
ΠΏΠΎΡΠΎΡΠΊΠΎΠ²ΠΎΠΉ Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΈ. ΠΠ½Π΄ΠΈΠ²ΠΈΠ΄ΡΠ°Π»ΡΠ½ΡΠ΅ Π³Π΅Π½Π΅ΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ Π°Π»Π³ΠΎΡΠΈΡΠΌΡ Π²ΡΠΏΠΎΠ»Π½ΡΡΡΡΡ Π½Π° ΡΠ°Π·Π½ΡΡ
ΡΠ·Π»Π°Ρ
Π²ΡΡΠΈΡΠ»ΠΈΡΠ΅Π»ΡΠ½ΠΎΠ³ΠΎ ΠΊΠ»Π°ΡΡΠ΅ΡΠ°. ΠΡΡΡΠΈΠ΅ ΡΡΡΡΠΊΡΡΡΠ½ΡΠ΅ ΠΌΠΎΠ΄Π΅Π»ΠΈ ΠΈΠ· Π²ΡΠ΅Ρ
ΡΠ·Π»ΠΎΠ² ΠΏΠΎΠ΄Π²Π΅ΡΠ³Π°ΡΡΡΡ
Π»ΠΎΠΊΠ°Π»ΡΠ½ΠΎΠΉ ΠΎΠΏΡΠΈΠΌΠΈΠ·Π°ΡΠΈΠΈ ΠΏΠΎ ΠΌΠ΅ΡΠΎΠ΄Ρ ΠΏΠΎΠ»Π½ΠΎΠΏΡΠΎΡΠΈΠ»ΡΠ½ΠΎΠ³ΠΎ ΡΡΡΡΠΊΡΡΡΠ½ΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π° ΠΈ Π½Π°ΠΊΠ°ΠΏΠ»ΠΈΠ²Π°ΡΡΡΡ
Π½Π° ΡΠΏΡΠ°Π²Π»ΡΡΡΠ΅ΠΌ ΡΠ·Π»Π΅. ΠΠ½ ΡΠΏΡΠ°Π²Π»ΡΠ΅Ρ ΠΈΡ
Π²ΡΠ±ΠΎΡΠΎΡΠ½ΠΎΠΉ ΠΌΠΈΠ³ΡΠ°ΡΠΈΠ΅ΠΉ ΠΎΠ±ΡΠ°ΡΠ½ΠΎ Π² ΠΏΠΎΠΏΡΠ»ΡΡΠΈΠΈ Π½Π°
Π²ΡΡΠΈΡΠ»ΠΈΡΠ΅Π»ΡΠ½ΡΡ
ΡΠ·Π»Π°Ρ
. Π Π°Π±ΠΎΡΠ° ΠΌΡΠ»ΡΡΠΈΠΏΠΎΠΏΡΠ»ΡΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ Π°Π»Π³ΠΎΡΠΈΡΠΌΠ° ΠΎΠ±ΡΡΠΆΠ΄Π°Π΅ΡΡΡ Π½Π° ΡΠ΅ΡΡΠΎΠ²ΡΡ
ΡΡΡΡΠΊΡΡΡΠ°Ρ
Ρ 9-10 Π½Π΅Π·Π°Π²ΠΈΡΠΈΠΌΡΠΌΠΈ Π°ΡΠΎΠΌΠ°ΠΌΠΈA multipopulation genetic algorithm for a crystal structure solution from the X-ray powder diffraction
data is proposed. Individual genetic algorithms are executed on different units of the computing
cluster. The local optimization is performed periodically by the full-profile structure analysis (Rietveld
method). The best trial structures are accumulated on the control unit for migration back to the routine
compute units. The work of multi-population algorithm is discussed on 3 example of test structures with
9-10 independent atoms. The reliability of the structure search increases in a half order of magnitude
more due to migratio
Possibilities of Neural Network Powder Diffraction Analysis Crystal Structure of Chemical Compounds
Some possibilities of using convolutional artificial neural networks (ANN) for powder diffraction
structural analysis of crystalline substances have been investigated. First, ANNs are used to classify
crystalline systems and space groups according to calculated full-profile diffractograms calculated from
the crystal structures of the ICSD database (2017 year). The ICSD database contains 192004 structures,
of which 80% was used for in-depth network training, and 20% for independent testing of recognition
accuracy. The accuracy of classification by a network of crystalline systems was 87.9%, and that of
space groups was 77.2%. Secondly, the ANN is used for a similar classification of structural models
generated by the stochastic genetic algorithm in the search processes for triclinic crystal structures of
test compound K4SnO4 according to their full-profile diffraction patterns. The classification criterion
was the entry of one or several atoms into their crystallographic positions in the structure of a substance.
Independent deep network training was performed on 120 thousand structural models of the K4PbO4
triclinic structure generated in several runs of the genetic algorithm. The accuracy of the classification
of K4SnO4 structural models exceeded 50%. The results show that deeply trained convolutional ANNs
can be effective for classifying crystal structures according to the structural characteristics of their
powder diffraction patterns
Modeling of the Crystal Structure of Platinum Metalβs Complex Compounds by Using Parallel Computing Based on Genetic Algorithms and X-ray Diffraction Data
ΠΠΎΠ΄Π΅Π»ΠΈ ΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΡΡΡΠΊΡΡΡΡ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ½ΡΡ
ΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½ΠΈΠΉ [Pd(CH3NH2)4][PdBr4] (ΠΏΡ.Π³Ρ.
P4/mnc (128), a=10.6866(7) Γ
, c=6.7262(3) Γ
, V=768.16(10) Γ
3) ΠΈ [Pt(NH3)5Cl]Br3 (ΠΏΡ. Π³Ρ. I41/a (88),
ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΡ ΡΡΠ΅ΠΉΠΊΠΈ a=17.2587(5) Γ
; c=15.1164(3) Γ
, V=4502,61(10) Γ
3) ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½Ρ Ρ ΠΏΠΎΠΌΠΎΡΡΡ
ΡΠ°Π·ΡΠ°Π±ΠΎΡΠ°Π½Π½ΠΎΠ³ΠΎ ΠΌΡΠ»ΡΡΠΈΠΏΠΎΠΏΡΠ»ΡΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΏΠ°ΡΠ°Π»Π»Π΅Π»ΡΠ½ΠΎΠ³ΠΎ Π³Π΅Π½Π΅ΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π°Π»Π³ΠΎΡΠΈΡΠΌΠ° (ΠΠΠΠ)
ΠΈ Π΄Π°Π½Π½ΡΡ
ΡΠ΅Π½ΡΠ³Π΅Π½ΠΎΠ²ΡΠΊΠΎΠΉ ΠΏΠΎΡΠΎΡΠΊΠΎΠ²ΠΎΠΉ Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΈ. ΠΠ±ΡΡΠΆΠ΄Π°ΡΡΡΡ ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠ° ΠΈ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ
ΡΡΡΡΠΊΡΡΡΠ½ΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π° ΡΡΠΈΡ
ΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½ΠΈΠΉ ΠΏΠΎ ΠΠΠΠCrystal structure models of complex compounds [Pd(CH3NH2)4][PdBr4] (sp. gr. P4/mnc (128),
a=10.6866(7) Γ
, c=6.7262(3) Γ
, V=768.16(10) Γ
3) and [Pt(NH3)5Cl]Br3 (sp. gr. I41/a (88),
a=17.2587(5) Γ
; c=15.1164(3) Γ
, V=4502,61(10) Γ
3) has been determined by using the developed
multipopulational parallel genetic algorithm (MPGA) and x-ray powder diffraction data. This
paper presents the methodology and results of the structural analysis of these compounds obtained
by application of the MPG
Multipopulation Genetic Algorithm for Simulation of the Crystal Structure from X-Ray Diffraction Data
ΠΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½ ΠΌΡΠ»ΡΡΠΈΠΏΠΎΠΏΡΠ»ΡΡΠΈΠΎΠ½Π½ΡΠΉ ΠΏΠ°ΡΠ°Π»Π»Π΅Π»ΡΠ½ΡΠΉ Π³Π΅Π½Π΅ΡΠΈΡΠ΅ΡΠΊΠΈΠΉ Π°Π»Π³ΠΎΡΠΈΡΠΌ Π΄Π»Ρ ΠΌΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΡ
Π°ΡΠΎΠΌΠ½ΠΎΠΉ ΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΡΡΡΠΊΡΡΡΡ Ρ
ΠΈΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½ΠΈΠΉ ΠΈΠ· Π΄Π°Π½Π½ΡΡ
ΡΠ΅Π½ΡΠ³Π΅Π½ΠΎΠ²ΡΠΊΠΎΠΉ
ΠΏΠΎΡΠΎΡΠΊΠΎΠ²ΠΎΠΉ Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΈ. ΠΠ½Π΄ΠΈΠ²ΠΈΠ΄ΡΠ°Π»ΡΠ½ΡΠ΅ Π³Π΅Π½Π΅ΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ Π°Π»Π³ΠΎΡΠΈΡΠΌΡ Π²ΡΠΏΠΎΠ»Π½ΡΡΡΡΡ Π½Π° ΡΠ°Π·Π½ΡΡ
ΡΠ·Π»Π°Ρ
Π²ΡΡΠΈΡΠ»ΠΈΡΠ΅Π»ΡΠ½ΠΎΠ³ΠΎ ΠΊΠ»Π°ΡΡΠ΅ΡΠ°. ΠΡΡΡΠΈΠ΅ ΡΡΡΡΠΊΡΡΡΠ½ΡΠ΅ ΠΌΠΎΠ΄Π΅Π»ΠΈ ΠΈΠ· Π²ΡΠ΅Ρ
ΡΠ·Π»ΠΎΠ² ΠΏΠΎΠ΄Π²Π΅ΡΠ³Π°ΡΡΡΡ
Π»ΠΎΠΊΠ°Π»ΡΠ½ΠΎΠΉ ΠΎΠΏΡΠΈΠΌΠΈΠ·Π°ΡΠΈΠΈ ΠΏΠΎ ΠΌΠ΅ΡΠΎΠ΄Ρ ΠΏΠΎΠ»Π½ΠΎΠΏΡΠΎΡΠΈΠ»ΡΠ½ΠΎΠ³ΠΎ ΡΡΡΡΠΊΡΡΡΠ½ΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π° ΠΈ Π½Π°ΠΊΠ°ΠΏΠ»ΠΈΠ²Π°ΡΡΡΡ
Π½Π° ΡΠΏΡΠ°Π²Π»ΡΡΡΠ΅ΠΌ ΡΠ·Π»Π΅. ΠΠ½ ΡΠΏΡΠ°Π²Π»ΡΠ΅Ρ ΠΈΡ
Π²ΡΠ±ΠΎΡΠΎΡΠ½ΠΎΠΉ ΠΌΠΈΠ³ΡΠ°ΡΠΈΠ΅ΠΉ ΠΎΠ±ΡΠ°ΡΠ½ΠΎ Π² ΠΏΠΎΠΏΡΠ»ΡΡΠΈΠΈ Π½Π°
Π²ΡΡΠΈΡΠ»ΠΈΡΠ΅Π»ΡΠ½ΡΡ
ΡΠ·Π»Π°Ρ
. Π Π°Π±ΠΎΡΠ° ΠΌΡΠ»ΡΡΠΈΠΏΠΎΠΏΡΠ»ΡΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ Π°Π»Π³ΠΎΡΠΈΡΠΌΠ° ΠΎΠ±ΡΡΠΆΠ΄Π°Π΅ΡΡΡ Π½Π° ΡΠ΅ΡΡΠΎΠ²ΡΡ
ΡΡΡΡΠΊΡΡΡΠ°Ρ
Ρ 9-10 Π½Π΅Π·Π°Π²ΠΈΡΠΈΠΌΡΠΌΠΈ Π°ΡΠΎΠΌΠ°ΠΌΠΈA multipopulation genetic algorithm for a crystal structure solution from the X-ray powder diffraction
data is proposed. Individual genetic algorithms are executed on different units of the computing
cluster. The local optimization is performed periodically by the full-profile structure analysis (Rietveld
method). The best trial structures are accumulated on the control unit for migration back to the routine
compute units. The work of multi-population algorithm is discussed on 3 example of test structures with
9-10 independent atoms. The reliability of the structure search increases in a half order of magnitude
more due to migratio
[Pb2F2](SeO4): a heavier analogue of grandreefite, the first layered fluoride selenate
Π’Π΅ΠΊΡΡ ΡΡΠ°ΡΡΠΈ Π½Π΅ ΠΏΡΠ±Π»ΠΈΠΊΡΠ΅ΡΡΡ Π² ΠΎΡΠΊΡΡΡΠΎΠΌ Π΄ΠΎΡΡΡΠΏΠ΅ Π² ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²ΠΈΠΈ Ρ ΠΏΠΎΠ»ΠΈΡΠΈΠΊΠΎΠΉ ΠΆΡΡΠ½Π°Π»Π°.Co-precipitation of PbF 2 and PbSeO 4 in weakly acidic media results in the formation of [Pb 2 F 2 ](SeO 4 ), the selenate analogue of the naturally occurring mineral grandreefite, [Pb 2 F 2 ](SO 4 ). The new compound is monoclinic, C2/c, a = 14.0784(2) Γ
, b = 4.6267(1) Γ
, c = 8.8628(1) Γ
, Ξ² = 108.98(1)Β°, V = 545.93(1) Γ
3 . Its structure has been refined from powder data to R B = 1.55%. From thermal studies, it is established that the compound is stable in air up to about 300 Β°C, after which it gradually converts into a single phase with composition [Pb 2 O](SeO 4 ), space group C2/m, and lattice parameters a = 14.0332(1) Γ
, b = 5.7532(1) Γ
, c = 7.2113(1) Γ
, Ξ² = 115.07(1)Β°, V = 527.37(1) Γ
3 . It is the selenate analogue of lanarkite, [Pb 2 O](SO 4 ), and phoenicochroite, [Pb 2 O](CrO 4 ), and its crystal structure was refined to R B = 1.21%. The formation of a single decomposition product upon heating in air suggests that this happens by a thermal hydrolysis mechanism, i.e., Pb 2 F 2 SeO 4 + H 2 O (vapor) β Pb 2 OSeO 4 + 2HFβ
[Pb2F2](SeO4): a heavier analogue of grandreefite, the first layered fluoride selenate
Π’Π΅ΠΊΡΡ ΡΡΠ°ΡΡΠΈ Π½Π΅ ΠΏΡΠ±Π»ΠΈΠΊΡΠ΅ΡΡΡ Π² ΠΎΡΠΊΡΡΡΠΎΠΌ Π΄ΠΎΡΡΡΠΏΠ΅ Π² ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²ΠΈΠΈ Ρ ΠΏΠΎΠ»ΠΈΡΠΈΠΊΠΎΠΉ ΠΆΡΡΠ½Π°Π»Π°.Co-precipitation of PbF 2 and PbSeO 4 in weakly acidic media results in the formation of [Pb 2 F 2 ](SeO 4 ), the selenate analogue of the naturally occurring mineral grandreefite, [Pb 2 F 2 ](SO 4 ). The new compound is monoclinic, C2/c, a = 14.0784(2) Γ
, b = 4.6267(1) Γ
, c = 8.8628(1) Γ
, Ξ² = 108.98(1)Β°, V = 545.93(1) Γ
3 . Its structure has been refined from powder data to R B = 1.55%. From thermal studies, it is established that the compound is stable in air up to about 300 Β°C, after which it gradually converts into a single phase with composition [Pb 2 O](SeO 4 ), space group C2/m, and lattice parameters a = 14.0332(1) Γ
, b = 5.7532(1) Γ
, c = 7.2113(1) Γ
, Ξ² = 115.07(1)Β°, V = 527.37(1) Γ
3 . It is the selenate analogue of lanarkite, [Pb 2 O](SO 4 ), and phoenicochroite, [Pb 2 O](CrO 4 ), and its crystal structure was refined to R B = 1.21%. The formation of a single decomposition product upon heating in air suggests that this happens by a thermal hydrolysis mechanism, i.e., Pb 2 F 2 SeO 4 + H 2 O (vapor) β Pb 2 OSeO 4 + 2HFβ
Pb6O5(NO3)2: A Nonlinear Optical Oxynitrate Structurally Based on Lead Oxide Framework
Π’Π΅ΠΊΡΡ ΡΡΠ°ΡΡΠΈ Π½Π΅ ΠΏΡΠ±Π»ΠΈΠΊΡΠ΅ΡΡΡ Π² ΠΎΡΠΊΡΡΡΠΎΠΌ Π΄ΠΎΡΡΡΠΏΠ΅ Π² ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²ΠΈΠΈ Ρ ΠΏΠΎΠ»ΠΈΡΠΈΠΊΠΎΠΉ ΠΆΡΡΠ½Π°Π»Π°.A high second harmonic generation response is demonstrated by a Pb6O5(NO3)2 lead oxynitrate whose identity was verified upon reinvestigation of the PbOβPb(NO3)2 system. Its crystal structure exhibits a unique cationic [Pb6O5]2+ framework hosting orientationally ordered NO3β triangles in the channels. Easy preparation and high thermal stability (until βΌ500 Β°C in air) suggest it to be a new promising NLO material
Possibilities of Neural Network Powder Diffraction Analysis Crystal Structure of Chemical Compounds
ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Ρ Π½Π΅ΠΊΠΎΡΠΎΡΡΠ΅ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΠΈ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΡ ΡΠ²Π΅ΡΡΠΎΡΠ½ΡΡ
ΠΈΡΠΊΡΡΡΡΠ²Π΅Π½Π½ΡΡ
Π½Π΅ΠΉΡΠΎΠ½Π½ΡΡ
ΡΠ΅ΡΠ΅ΠΉ (ΠΠΠ‘) Π΄Π»Ρ ΠΏΠΎΡΠΎΡΠΊΠΎΠ²ΠΎΠ³ΠΎ Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ ΡΡΡΡΠΊΡΡΡΠ½ΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π° ΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΈΡ
Π²Π΅ΡΠ΅ΡΡΠ². ΠΠΎ-ΠΏΠ΅ΡΠ²ΡΡ
, ΠΠΠ‘ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½Ρ Π΄Π»Ρ ΠΊΠ»Π°ΡΡΠΈΡΠΈΠΊΠ°ΡΠΈΠΈ ΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠΈΡΡΠ΅ΠΌ ΠΈ
ΠΏΡΠΎΡΡΡΠ°Π½ΡΡΠ²Π΅Π½Π½ΡΡ
Π³ΡΡΠΏΠΏ ΡΠΈΠΌΠΌΠ΅ΡΡΠΈΠΈ ΠΏΠΎ ΡΠ°ΡΡΠ΅ΡΠ½ΡΠΌ ΠΏΠΎΠ»Π½ΠΎΠΏΡΠΎΡΠΈΠ»ΡΠ½ΡΠΌ Π΄ΠΈΡΡΠ°ΠΊΡΠΎΠ³ΡΠ°ΠΌΠΌΠ°ΠΌ,
Π²ΡΡΠΈΡΠ»Π΅Π½Π½ΡΠΌ ΠΈΠ· ΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΡΡΡΠΊΡΡΡ Π±Π°Π·Ρ Π΄Π°Π½Π½ΡΡ
ICSD 2017 Π³. ΠΠ°Π·Π° ICSD ΡΠΎΠ΄Π΅ΡΠΆΠΈΡ
192004 ΡΡΡΡΠΊΡΡΡΡ, ΠΈΠ· ΠΊΠΎΡΠΎΡΡΡ
80 % ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π»ΠΎΡΡ Π΄Π»Ρ Π³Π»ΡΠ±ΠΎΠΊΠΎΠ³ΠΎ ΠΎΠ±ΡΡΠ΅Π½ΠΈΡ ΡΠ΅ΡΠΈ, Π° 20 %
Π΄Π»Ρ Π½Π΅Π·Π°Π²ΠΈΡΠΈΠΌΠΎΠ³ΠΎ ΡΠ΅ΡΡΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΡΠΎΡΠ½ΠΎΡΡΠΈ ΡΠ°ΡΠΏΠΎΠ·Π½Π°Π²Π°Π½ΠΈΡ. Π’ΠΎΡΠ½ΠΎΡΡΡ ΠΊΠ»Π°ΡΡΠΈΡΠΈΠΊΠ°ΡΠΈΠΈ
ΡΠ΅ΡΡΡ ΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠΈΡΡΠ΅ΠΌ ΡΠΎΡΡΠ°Π²ΠΈΠ»Π° 87,9 %, Π° ΠΏΡΠΎΡΡΡΠ°Π½ΡΡΠ²Π΅Π½Π½ΡΡ
Π³ΡΡΠΏΠΏ β 77,2 %. ΠΠΎ-
Π²ΡΠΎΡΡΡ
, Π΄ΡΡΠ³Π°Ρ ΠΠΠ‘ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½Π° Π΄Π»Ρ ΠΊΠ»Π°ΡΡΠΈΡΠΈΠΊΠ°ΡΠΈΠΈ ΡΡΡΡΠΊΡΡΡΠ½ΡΡ
ΠΌΠΎΠ΄Π΅Π»Π΅ΠΉ, ΡΠ³Π΅Π½Π΅ΡΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
ΡΡΠΎΡ
Π°ΡΡΠΈΡΠ΅ΡΠΊΠΈΠΌ Π³Π΅Π½Π΅ΡΠΈΡΠ΅ΡΠΊΠΈΠΌ Π°Π»Π³ΠΎΡΠΈΡΠΌΠΎΠΌ Π² ΠΏΡΠΎΡΠ΅ΡΡΠ°Ρ
ΠΏΠΎΠΈΡΠΊΠ° ΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΡΡΡΠΊΡΡΡ
ΡΠ΅ΡΡΠΎΠ²ΡΡ
ΡΡΠΈΠΊΠ»ΠΈΠ½Π½ΡΡ
ΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½ΠΈΠΉ K4SnO4 ΠΈ K4SnO4, ΠΏΠΎ ΠΈΡ
ΠΏΠΎΠ»Π½ΠΎΠΏΡΠΎΡΠΈΠ»ΡΠ½ΡΠΌ Π΄ΠΈΡΡΠ°ΠΊΡΠΎΠ³ΡΠ°ΠΌΠΌΠ°ΠΌ.
ΠΡΠ»ΠΎ ΡΠ³Π΅Π½Π΅ΡΠΈΡΠΎΠ²Π°Π½ΠΎ ΠΎΠΊΠΎΠ»ΠΎ 150 ΡΡΡΡΡ ΡΡΡΡΠΊΡΡΡΠ½ΡΡ
ΠΌΠΎΠ΄Π΅Π»Π΅ΠΉ ΠΊΠ°ΠΆΠ΄ΠΎΠΉ ΠΈΠ· ΡΡΠΈΡ
ΡΡΡΡΠΊΡΡΡ. ΠΠ»ΡΠ±ΠΎΠΊΠΎΠ΅
ΠΎΠ±ΡΡΠ΅Π½ΠΈΠ΅ ΡΠ΅ΡΠΈ Π²ΡΠΏΠΎΠ»Π½ΡΠ»ΠΎΡΡ Π½Π° Π΄ΠΈΡΡΠ°ΠΊΡΠΎΠ³ΡΠ°ΠΌΠΌΠ°Ρ
ΡΡΡΡΠΊΡΡΡΠ½ΡΡ
ΠΌΠΎΠ΄Π΅Π»Π΅ΠΉ K4PbO4. ΠΠ±ΡΡΠ΅Π½Π½Π°Ρ ΡΠ΅ΡΡ
Π±ΡΠ»Π° ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½Π° Π΄Π»Ρ ΠΊΠ»Π°ΡΡΠΈΡΠΈΠΊΠ°ΡΠΈΠΈ ΡΡΡΡΠΊΡΡΡΠ½ΡΡ
ΠΌΠΎΠ΄Π΅Π»Π΅ΠΉ K4SnO4 ΠΏΠΎ ΠΈΡ
Π΄ΠΈΡΡΠ°ΠΊΡΠΎΠ³ΡΠ°ΠΌΠΌΠ°ΠΌ.
ΠΡΠΈΡΠ΅ΡΠΈΠ΅ΠΌ ΠΊΠ»Π°ΡΡΠΈΡΠΈΠΊΠ°ΡΠΈΠΈ ΡΠ²Π»ΡΠ»ΠΎΡΡ ΠΏΠΎΠΏΠ°Π΄Π°Π½ΠΈΠ΅ Π°ΡΠΎΠΌΠΎΠ² Π² ΠΈΡ
ΠΊΡΠΈΡΡΠ°Π»Π»ΠΎΠ³ΡΠ°ΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΏΠΎΠ·ΠΈΡΠΈΠΈ
Π² ΡΡΡΡΠΊΡΡΡΠ΅. Π’ΠΎΡΠ½ΠΎΡΡΡ ΠΊΠ»Π°ΡΡΠΈΡΠΈΠΊΠ°ΡΠΈΠΈ Π°Π΄Π΅ΠΊΠ²Π°ΡΠ½ΡΡ
ΠΏΠΎΠ·ΠΈΡΠΈΠΉ Π°ΡΠΎΠΌΠΎΠ² Π² ΡΡΡΡΠΊΡΡΡΠ½ΡΡ
ΠΌΠΎΠ΄Π΅Π»ΡΡ
K4SnO4 ΠΏΡΠ΅Π²ΡΡΠΈΠ»Π° 50 %.Some possibilities of using convolutional artificial neural networks (ANN) for powder diffraction
structural analysis of crystalline substances have been investigated. First, ANNs are used to classify
crystalline systems and space groups according to calculated full-profile diffractograms calculated from
the crystal structures of the ICSD database (2017 year). The ICSD database contains 192004 structures,
of which 80% was used for in-depth network training, and 20% for independent testing of recognition
accuracy. The accuracy of classification by a network of crystalline systems was 87.9%, and that of
space groups was 77.2%. Secondly, the ANN is used for a similar classification of structural models
generated by the stochastic genetic algorithm in the search processes for triclinic crystal structures of
test compound K4SnO4 according to their full-profile diffraction patterns. The classification criterion
was the entry of one or several atoms into their crystallographic positions in the structure of a substance.
Independent deep network training was performed on 120 thousand structural models of the K4PbO4
triclinic structure generated in several runs of the genetic algorithm. The accuracy of the classification
of K4SnO4 structural models exceeded 50%. The results show that deeply trained convolutional ANNs
can be effective for classifying crystal structures according to the structural characteristics of their
powder diffraction pattern
Synthesis, crystal structure, spectroscopic properties, and thermal behavior of rare-earth oxide selenates, Ln2O2SeO4 (Ln = La, Pr, Nd): The new perspectives of solid-state double-exchange synthesis
Π’Π΅ΠΊΡΡ ΡΡΠ°ΡΡΠΈ Π½Π΅ ΠΏΡΠ±Π»ΠΈΠΊΡΠ΅ΡΡΡ Π² ΠΎΡΠΊΡΡΡΠΎΠΌ Π΄ΠΎΡΡΡΠΏΠ΅ Π² ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²ΠΈΠΈ Ρ ΠΏΠΎΠ»ΠΈΡΠΈΠΊΠΎΠΉ ΠΆΡΡΠ½Π°Π»Π°.Three rare-earth oxide selenates Ln2O2SeO4 (Ln = La, Pr, Nd) have been prepared via double-exchange solid-state reactions between respective LnOCl oxyhalides and potassium selenate. This approach succeeded to obtain singlephase specimens of La2O2SeO4 and Nd2O2SeO4, previously known as transients upon thermal decomposition of the corresponding selenates, as well as a new compound Pr2O2SeO4. Refinement of their crystal structures from powder X-ray diffraction data confirmed previous attributions to the grandreefite (Pb2F2SO4) structure type observed also for the Ln2O2SO4 oxide sulfates. According to polythermic X-ray studies, La2O2SeO4 is stable until at least 700 C. All compounds were characterized by infrared and X-ray photoelectron spectroscopy
Modeling of the Crystal Structure of Platinum Metalβs Complex Compounds by Using Parallel Computing Based on Genetic Algorithms and X-ray Diffraction Data
ΠΠΎΠ΄Π΅Π»ΠΈ ΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΡΡΡΠΊΡΡΡΡ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ½ΡΡ
ΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½ΠΈΠΉ [Pd(CH3NH2)4][PdBr4] (ΠΏΡ.Π³Ρ.
P4/mnc (128), a=10.6866(7) Γ
, c=6.7262(3) Γ
, V=768.16(10) Γ
3) ΠΈ [Pt(NH3)5Cl]Br3 (ΠΏΡ. Π³Ρ. I41/a (88),
ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΡ ΡΡΠ΅ΠΉΠΊΠΈ a=17.2587(5) Γ
; c=15.1164(3) Γ
, V=4502,61(10) Γ
3) ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½Ρ Ρ ΠΏΠΎΠΌΠΎΡΡΡ
ΡΠ°Π·ΡΠ°Π±ΠΎΡΠ°Π½Π½ΠΎΠ³ΠΎ ΠΌΡΠ»ΡΡΠΈΠΏΠΎΠΏΡΠ»ΡΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΏΠ°ΡΠ°Π»Π»Π΅Π»ΡΠ½ΠΎΠ³ΠΎ Π³Π΅Π½Π΅ΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π°Π»Π³ΠΎΡΠΈΡΠΌΠ° (ΠΠΠΠ)
ΠΈ Π΄Π°Π½Π½ΡΡ
ΡΠ΅Π½ΡΠ³Π΅Π½ΠΎΠ²ΡΠΊΠΎΠΉ ΠΏΠΎΡΠΎΡΠΊΠΎΠ²ΠΎΠΉ Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΈ. ΠΠ±ΡΡΠΆΠ΄Π°ΡΡΡΡ ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠ° ΠΈ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ
ΡΡΡΡΠΊΡΡΡΠ½ΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π° ΡΡΠΈΡ
ΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½ΠΈΠΉ ΠΏΠΎ ΠΠΠΠCrystal structure models of complex compounds [Pd(CH3NH2)4][PdBr4] (sp. gr. P4/mnc (128),
a=10.6866(7) Γ
, c=6.7262(3) Γ
, V=768.16(10) Γ
3) and [Pt(NH3)5Cl]Br3 (sp. gr. I41/a (88),
a=17.2587(5) Γ
; c=15.1164(3) Γ
, V=4502,61(10) Γ
3) has been determined by using the developed
multipopulational parallel genetic algorithm (MPGA) and x-ray powder diffraction data. This
paper presents the methodology and results of the structural analysis of these compounds obtained
by application of the MPG