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Subsolidus phase relations and structures of solid solutions in the systems K 2 MoO 4 –Na 2 MoO 4 –MMoO 4 (M = Mn, Zn). / Gulyaeva, Oksana A.; Solodovnikova, Zoya A.; Solodovnikov, Sergey F. и др.

в: Journal of Solid State Chemistry, Том 272, 01.04.2019, стр. 148-156.

Результаты исследований: Научные публикации в периодических изданияхстатьяРецензирование

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Gulyaeva OA, Solodovnikova ZA, Solodovnikov SF, Yudin VN, Zolotova ES, Komarov VY. Subsolidus phase relations and structures of solid solutions in the systems K 2 MoO 4 –Na 2 MoO 4 –MMoO 4 (M = Mn, Zn). Journal of Solid State Chemistry. 2019 апр. 1;272:148-156. doi: 10.1016/j.jssc.2019.02.010

Author

Gulyaeva, Oksana A. ; Solodovnikova, Zoya A. ; Solodovnikov, Sergey F. и др. / Subsolidus phase relations and structures of solid solutions in the systems K 2 MoO 4 –Na 2 MoO 4 –MMoO 4 (M = Mn, Zn). в: Journal of Solid State Chemistry. 2019 ; Том 272. стр. 148-156.

BibTeX

@article{c971e5354e1b4883ae7a1502030e09ea,
title = "Subsolidus phase relations and structures of solid solutions in the systems K 2 MoO 4 –Na 2 MoO 4 –MMoO 4 (M = Mn, Zn)",
abstract = " Study of phase formation in the system K 2 MoO 4 –Na 2 MoO 4 at 500 °C showed the existence of the only double molybdate K 2-x Na x MoO 4 (0.4 ≤ x ≤ 1) of the glaserite-related type. Using these data, the subsolidus phase relations in the systems K 2 MoO 4 –Na 2 MoO 4 –MMoO 4 (M = Mn, Zn) were studied at 470–560 °C and the extended solid solutions based on the alluaudite-type Na 4−2x M 1+x (MoO 4 ) 3 were found. In the structure of K 1.71 Na 1.71 Mn 1.29 (MoO 4 ) 3 (sp. gr. C2/c, Z = 4, a = 13.0595(3) {\AA} b = 13.7892(3) {\AA} c = 7.2973(2) {\AA} β = 111.339(1)° R = 0.0134), the potassium ions partially replace Na + in the channels running along c-axis. The structure of K 1.84 Na 2.11 Zn 1.02 (MoO 4 ) 3 (sp. gr. P1̅ Z = 2, a = 7.3258(8) {\AA} b = 9.4128(10) {\AA} c = 9.4302(10) {\AA} α = 93.104(3)° β = 104.573(3)° γ = 104.432(3)° R = 0.0220) is isotypic with alluaudite-related α-K 4 Zn(WO 4 ) 3 and seems to be a result of stabilizing an unknown triclinic modification of K 4 Zn(MoO 4 ) 3 by substitution of sodium for potassium with the strong differentiation of alkali and zinc cations in the structure. In the structure of K 1.5 Na 0.5 Mn 2 (MoO 4 ) 3 (sp. gr. Pcca, Z = 8, a = 10.6160(7) {\AA} b = 12.2714(8) {\AA} c = 18.0275(11) {\AA} R = 0.0155) of the α-K 2 Mn 2 (MoO 4 ) 3 type, one of three initial potassium positions is jointly occupied by (Na, Mn); a similar phenomenon occurs in isostructural Rb 3 Na 3 Sc 2 (MoO 4 ) 6 . The structure contains zigzag-like ribbons of edge-sharing MnO 6 octahedra linked with separate MnO 6 octahedra and МоО 4 tetrahedra into 3D containing channels along the c-axes filled by K + ions. BVS maps show possible one-dimensional sodium-ion conductivity for the structures of K 1.71 Na 1.71 Mn 1.29 (MoO 4 ) 3 and Rb 3 Na 3 Sc 2 (MoO 4 ) 6 . ",
keywords = "Bond valence sum maps, Complex molybdates, Crystal structure, Ionic conductivity, Solid solutions, Ternary systems, BINARY MOLYBDATES, CRYSTAL-STRUCTURE, IONIC-CONDUCTIVITY, CO, STRUCTURE CRISTALLINE, TUNGSTATES, CHEMISTRY, POTASSIUM, NI, DOUBLE MOLYBDATES",
author = "Gulyaeva, {Oksana A.} and Solodovnikova, {Zoya A.} and Solodovnikov, {Sergey F.} and Yudin, {Vasiliy N.} and Zolotova, {Evgeniya S.} and Komarov, {Vladislav Yu}",
year = "2019",
month = apr,
day = "1",
doi = "10.1016/j.jssc.2019.02.010",
language = "English",
volume = "272",
pages = "148--156",
journal = "Journal of Solid State Chemistry",
issn = "0022-4596",
publisher = "Academic Press Inc.",

}

RIS

TY - JOUR

T1 - Subsolidus phase relations and structures of solid solutions in the systems K 2 MoO 4 –Na 2 MoO 4 –MMoO 4 (M = Mn, Zn)

AU - Gulyaeva, Oksana A.

AU - Solodovnikova, Zoya A.

AU - Solodovnikov, Sergey F.

AU - Yudin, Vasiliy N.

AU - Zolotova, Evgeniya S.

AU - Komarov, Vladislav Yu

PY - 2019/4/1

Y1 - 2019/4/1

N2 - Study of phase formation in the system K 2 MoO 4 –Na 2 MoO 4 at 500 °C showed the existence of the only double molybdate K 2-x Na x MoO 4 (0.4 ≤ x ≤ 1) of the glaserite-related type. Using these data, the subsolidus phase relations in the systems K 2 MoO 4 –Na 2 MoO 4 –MMoO 4 (M = Mn, Zn) were studied at 470–560 °C and the extended solid solutions based on the alluaudite-type Na 4−2x M 1+x (MoO 4 ) 3 were found. In the structure of K 1.71 Na 1.71 Mn 1.29 (MoO 4 ) 3 (sp. gr. C2/c, Z = 4, a = 13.0595(3) Å b = 13.7892(3) Å c = 7.2973(2) Å β = 111.339(1)° R = 0.0134), the potassium ions partially replace Na + in the channels running along c-axis. The structure of K 1.84 Na 2.11 Zn 1.02 (MoO 4 ) 3 (sp. gr. P1̅ Z = 2, a = 7.3258(8) Å b = 9.4128(10) Å c = 9.4302(10) Å α = 93.104(3)° β = 104.573(3)° γ = 104.432(3)° R = 0.0220) is isotypic with alluaudite-related α-K 4 Zn(WO 4 ) 3 and seems to be a result of stabilizing an unknown triclinic modification of K 4 Zn(MoO 4 ) 3 by substitution of sodium for potassium with the strong differentiation of alkali and zinc cations in the structure. In the structure of K 1.5 Na 0.5 Mn 2 (MoO 4 ) 3 (sp. gr. Pcca, Z = 8, a = 10.6160(7) Å b = 12.2714(8) Å c = 18.0275(11) Å R = 0.0155) of the α-K 2 Mn 2 (MoO 4 ) 3 type, one of three initial potassium positions is jointly occupied by (Na, Mn); a similar phenomenon occurs in isostructural Rb 3 Na 3 Sc 2 (MoO 4 ) 6 . The structure contains zigzag-like ribbons of edge-sharing MnO 6 octahedra linked with separate MnO 6 octahedra and МоО 4 tetrahedra into 3D containing channels along the c-axes filled by K + ions. BVS maps show possible one-dimensional sodium-ion conductivity for the structures of K 1.71 Na 1.71 Mn 1.29 (MoO 4 ) 3 and Rb 3 Na 3 Sc 2 (MoO 4 ) 6 .

AB - Study of phase formation in the system K 2 MoO 4 –Na 2 MoO 4 at 500 °C showed the existence of the only double molybdate K 2-x Na x MoO 4 (0.4 ≤ x ≤ 1) of the glaserite-related type. Using these data, the subsolidus phase relations in the systems K 2 MoO 4 –Na 2 MoO 4 –MMoO 4 (M = Mn, Zn) were studied at 470–560 °C and the extended solid solutions based on the alluaudite-type Na 4−2x M 1+x (MoO 4 ) 3 were found. In the structure of K 1.71 Na 1.71 Mn 1.29 (MoO 4 ) 3 (sp. gr. C2/c, Z = 4, a = 13.0595(3) Å b = 13.7892(3) Å c = 7.2973(2) Å β = 111.339(1)° R = 0.0134), the potassium ions partially replace Na + in the channels running along c-axis. The structure of K 1.84 Na 2.11 Zn 1.02 (MoO 4 ) 3 (sp. gr. P1̅ Z = 2, a = 7.3258(8) Å b = 9.4128(10) Å c = 9.4302(10) Å α = 93.104(3)° β = 104.573(3)° γ = 104.432(3)° R = 0.0220) is isotypic with alluaudite-related α-K 4 Zn(WO 4 ) 3 and seems to be a result of stabilizing an unknown triclinic modification of K 4 Zn(MoO 4 ) 3 by substitution of sodium for potassium with the strong differentiation of alkali and zinc cations in the structure. In the structure of K 1.5 Na 0.5 Mn 2 (MoO 4 ) 3 (sp. gr. Pcca, Z = 8, a = 10.6160(7) Å b = 12.2714(8) Å c = 18.0275(11) Å R = 0.0155) of the α-K 2 Mn 2 (MoO 4 ) 3 type, one of three initial potassium positions is jointly occupied by (Na, Mn); a similar phenomenon occurs in isostructural Rb 3 Na 3 Sc 2 (MoO 4 ) 6 . The structure contains zigzag-like ribbons of edge-sharing MnO 6 octahedra linked with separate MnO 6 octahedra and МоО 4 tetrahedra into 3D containing channels along the c-axes filled by K + ions. BVS maps show possible one-dimensional sodium-ion conductivity for the structures of K 1.71 Na 1.71 Mn 1.29 (MoO 4 ) 3 and Rb 3 Na 3 Sc 2 (MoO 4 ) 6 .

KW - Bond valence sum maps

KW - Complex molybdates

KW - Crystal structure

KW - Ionic conductivity

KW - Solid solutions

KW - Ternary systems

KW - BINARY MOLYBDATES

KW - CRYSTAL-STRUCTURE

KW - IONIC-CONDUCTIVITY

KW - CO

KW - STRUCTURE CRISTALLINE

KW - TUNGSTATES

KW - CHEMISTRY

KW - POTASSIUM

KW - NI

KW - DOUBLE MOLYBDATES

UR - http://www.scopus.com/inward/record.url?scp=85061430297&partnerID=8YFLogxK

U2 - 10.1016/j.jssc.2019.02.010

DO - 10.1016/j.jssc.2019.02.010

M3 - Article

AN - SCOPUS:85061430297

VL - 272

SP - 148

EP - 156

JO - Journal of Solid State Chemistry

JF - Journal of Solid State Chemistry

SN - 0022-4596

ER -

ID: 18485861