TY - JOUR
T1 - High- and low-temperature phases of lithium boron nitride, Li3BN2
T2 - Preparation, phase relation, crystal structure, and ionic conductivity
AU - Yamane, Hisanori
AU - Kikkawa, Shinichi
AU - Koizumi, Mitsue
N1 - Funding Information:
The authors thank Professor F. Kanamaru and his colleaguesa t ISIR of Osaka University and also Pro-fessorH . Horiuchi at the University of Tokyo for their assistancei n structurala nalysis. We also thank Mr. T. Tanaka for operating the intensity collection system on X-ray diffraction of MAC at ISIR. We thank the researchg roup under the directiono f ProfessorS . Ka-wai at ISIR for their technical assistancei n the impedance measurements.T his research was partly supported by a grant from the researchp roject in ISIR on developmento f new materialsf or energya nd also by a grant from the Casio Science Promotion Foundation.
PY - 1987/11
Y1 - 1987/11
N2 - Low- (α) and high- (β) temperature phases of Li3BN2 were prepared from mixtures of Li3N BN = 1.1 - 1.0 in molar ratio at 1070 and 1170 K, respectively. Phase relation between these phases was studied by annealing the products at various temperatures and conducting DTA in a stream of nitrogen. The phase transition temperature is at about 1135 K. The melting point of β-Li3BN2 is around 1189 K. α-Li3BN2 crystallizes directly from the undercooled liquid at 1160 K. The structure of α-Li3BN2, which is analyzed in the present study for the first time, has tetragonal symmetry, P42212, a = b = 4.6435(2), c = 5.2592(5), Å, Z = 2, Dcalc = 1.747 Mg m-3, μ = 0.082 mm-1. The structure was determined by 208 unique X-ray reflections with Fo > 3σ(Fo) and refined up to R = 0.042 by a full-matrix least-squares method. The lattice is composed of Li(1), Li(2), and linear (NBN)3- ions [r(BN) = 1.339(2), Å]. The Li(1) ion is also linearly coordinated by two nitrogen atoms [r(Li(1)N = 1.945(8), Å]. The Li(2) ion is at the center of a tetrahedron of N atoms [r(Li(2)N) = 2.125(18)Å, δ(NLiN) = 103.6(2) and 112.5(9)°]. Lithium ion conductivity of 3 × 10-5 S m-1 was measured at 400 K on a polycrystalline α-Li3BN2 specimen with an activation energy of 78 kJ/mole.
AB - Low- (α) and high- (β) temperature phases of Li3BN2 were prepared from mixtures of Li3N BN = 1.1 - 1.0 in molar ratio at 1070 and 1170 K, respectively. Phase relation between these phases was studied by annealing the products at various temperatures and conducting DTA in a stream of nitrogen. The phase transition temperature is at about 1135 K. The melting point of β-Li3BN2 is around 1189 K. α-Li3BN2 crystallizes directly from the undercooled liquid at 1160 K. The structure of α-Li3BN2, which is analyzed in the present study for the first time, has tetragonal symmetry, P42212, a = b = 4.6435(2), c = 5.2592(5), Å, Z = 2, Dcalc = 1.747 Mg m-3, μ = 0.082 mm-1. The structure was determined by 208 unique X-ray reflections with Fo > 3σ(Fo) and refined up to R = 0.042 by a full-matrix least-squares method. The lattice is composed of Li(1), Li(2), and linear (NBN)3- ions [r(BN) = 1.339(2), Å]. The Li(1) ion is also linearly coordinated by two nitrogen atoms [r(Li(1)N = 1.945(8), Å]. The Li(2) ion is at the center of a tetrahedron of N atoms [r(Li(2)N) = 2.125(18)Å, δ(NLiN) = 103.6(2) and 112.5(9)°]. Lithium ion conductivity of 3 × 10-5 S m-1 was measured at 400 K on a polycrystalline α-Li3BN2 specimen with an activation energy of 78 kJ/mole.
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U2 - 10.1016/0022-4596(87)90135-6
DO - 10.1016/0022-4596(87)90135-6
M3 - Article
AN - SCOPUS:0023455697
SN - 0022-4596
VL - 71
SP - 1
EP - 11
JO - Journal of Solid State Chemistry
JF - Journal of Solid State Chemistry
IS - 1
ER -