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Thermal behaviour of the rigid boron-oxygen groups in the α-Na2B8O13 crystal structure. / Bubnova, R. S.; Shepelev, Ju F.; Sennovan, N. A.; Filatov, S. K.

In: Zeitschrift fur Kristallographie, Vol. 217, No. 9, 01.01.2002, p. 444-450.

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Bubnova, R. S. ; Shepelev, Ju F. ; Sennovan, N. A. ; Filatov, S. K. / Thermal behaviour of the rigid boron-oxygen groups in the α-Na2B8O13 crystal structure. In: Zeitschrift fur Kristallographie. 2002 ; Vol. 217, No. 9. pp. 444-450.

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@article{fac94d62a01943988aa2dd32a8962d4d,
title = "Thermal behaviour of the rigid boron-oxygen groups in the α-Na2B8O13 crystal structure",
abstract = "The crystal structure of the α-Na2B8O13 stable modification has been refined by single crystal X-ray diffraction at 293, 573 and 773 K. The compound is monoclinic, P21/a space group, unit-cell parameters at 273 K are: a = 6.507(3), b = 17.796(8), c = 8.377(5) {\AA}, β = 96.60(4)°, Z = 4. The structure contains two interlocking boron-oxygen frameworks, each of them consisting of alternating single and double rings composed of two triangles and a tetrahedron so called triborate and pentaborate groups. Two non-equivalent sodium atoms linking two frameworks are coordinated by 8 oxygens. They are connected into finite chains consisting of four NaO8 polyhedra by sharing oxygen edges. The α-Na2B8O13 thermal expansion investigated by high temperature powder X-ray diffraction has sharply anisotropic character including negative thermal expansion: the coefficients of a thermal expansion tensor in temperature region 273-1000 K are α11 = 55-0.042 · (273 + t) α22=11, α33 = 15 + 0.032 · (273 + t), (x 10-6 K-1), μ = (cα33) = 42°. That high anisotropy is caused by anisotropic thermal vibrations of the Na atoms. Under heating a high stability of the B-O rigid groups and a weak contraction of some B-O bond lengths were revealed. In response to anisotropic thermal behaviour of Na atoms rigid B-O groups of the anion framework rotate relative to each other as a three-dimensional hinge.",
author = "Bubnova, {R. S.} and Shepelev, {Ju F.} and Sennovan, {N. A.} and Filatov, {S. K.}",
year = "2002",
month = jan,
day = "1",
doi = "10.1524/zkri.217.9.444.22881",
language = "English",
volume = "217",
pages = "444--450",
journal = "Zeitschfrift fur Kristallographie",
issn = "0044-2968",
publisher = "De Gruyter",
number = "9",

}

RIS

TY - JOUR

T1 - Thermal behaviour of the rigid boron-oxygen groups in the α-Na2B8O13 crystal structure

AU - Bubnova, R. S.

AU - Shepelev, Ju F.

AU - Sennovan, N. A.

AU - Filatov, S. K.

PY - 2002/1/1

Y1 - 2002/1/1

N2 - The crystal structure of the α-Na2B8O13 stable modification has been refined by single crystal X-ray diffraction at 293, 573 and 773 K. The compound is monoclinic, P21/a space group, unit-cell parameters at 273 K are: a = 6.507(3), b = 17.796(8), c = 8.377(5) Å, β = 96.60(4)°, Z = 4. The structure contains two interlocking boron-oxygen frameworks, each of them consisting of alternating single and double rings composed of two triangles and a tetrahedron so called triborate and pentaborate groups. Two non-equivalent sodium atoms linking two frameworks are coordinated by 8 oxygens. They are connected into finite chains consisting of four NaO8 polyhedra by sharing oxygen edges. The α-Na2B8O13 thermal expansion investigated by high temperature powder X-ray diffraction has sharply anisotropic character including negative thermal expansion: the coefficients of a thermal expansion tensor in temperature region 273-1000 K are α11 = 55-0.042 · (273 + t) α22=11, α33 = 15 + 0.032 · (273 + t), (x 10-6 K-1), μ = (cα33) = 42°. That high anisotropy is caused by anisotropic thermal vibrations of the Na atoms. Under heating a high stability of the B-O rigid groups and a weak contraction of some B-O bond lengths were revealed. In response to anisotropic thermal behaviour of Na atoms rigid B-O groups of the anion framework rotate relative to each other as a three-dimensional hinge.

AB - The crystal structure of the α-Na2B8O13 stable modification has been refined by single crystal X-ray diffraction at 293, 573 and 773 K. The compound is monoclinic, P21/a space group, unit-cell parameters at 273 K are: a = 6.507(3), b = 17.796(8), c = 8.377(5) Å, β = 96.60(4)°, Z = 4. The structure contains two interlocking boron-oxygen frameworks, each of them consisting of alternating single and double rings composed of two triangles and a tetrahedron so called triborate and pentaborate groups. Two non-equivalent sodium atoms linking two frameworks are coordinated by 8 oxygens. They are connected into finite chains consisting of four NaO8 polyhedra by sharing oxygen edges. The α-Na2B8O13 thermal expansion investigated by high temperature powder X-ray diffraction has sharply anisotropic character including negative thermal expansion: the coefficients of a thermal expansion tensor in temperature region 273-1000 K are α11 = 55-0.042 · (273 + t) α22=11, α33 = 15 + 0.032 · (273 + t), (x 10-6 K-1), μ = (cα33) = 42°. That high anisotropy is caused by anisotropic thermal vibrations of the Na atoms. Under heating a high stability of the B-O rigid groups and a weak contraction of some B-O bond lengths were revealed. In response to anisotropic thermal behaviour of Na atoms rigid B-O groups of the anion framework rotate relative to each other as a three-dimensional hinge.

UR - http://www.scopus.com/inward/record.url?scp=0036397001&partnerID=8YFLogxK

U2 - 10.1524/zkri.217.9.444.22881

DO - 10.1524/zkri.217.9.444.22881

M3 - Article

AN - SCOPUS:0036397001

VL - 217

SP - 444

EP - 450

JO - Zeitschfrift fur Kristallographie

JF - Zeitschfrift fur Kristallographie

SN - 0044-2968

IS - 9

ER -

ID: 53952388