New ionic conductors Ln_{2 + x}Ti_{2 − x}O_{7 − x /2} (Ln = Dy−Lu, x = 0.132)

By Shlyakhtina A.   Mosunov A.   Stefanovich S.   Karyagina O.   Shcherbakova L.  

Inorganic Materials, Vol. 40, Iss. 12, 2004-12 ,pp. : 1317-1320

MAIK Nauka/Interperiodica

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Low-frequency and microwave dielectric properties of Ba₂LnTaO₆ (Ln = La, Pr, Sm, Dy, Ce, Gd, Nd, Tm, Tb) ceramics

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Inorganic Materials, Vol. 42, Iss. 1, 2006-01 ,pp. : 64-67

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New Copper Oxychlorides Ca 4 Ln 2 Cu 3 O 8 Cl 4 , First Members of the Intergrowth Series (Ca 2 CuO 2 Cl 2 ) m ( Ln 2 Ca 2 Cu 2 O 6 Cl 2 ) n ( Ln = Gd, Sm)

By Pelloquin D.   Sundaresan A.   Hervieu M.   Michel C.   Raveau B.  

Journal of Solid State Chemistry, Vol. 127, Iss. 2, 1996-12 ,pp. : 315-324

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Gibbs Free Energy of Formation of Ln2CuBaO5 Compounds Determined by the EMF Method (Ln=Yb, Tm, Er, Ho, Dy, and Gd)

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New Bi-Ln-V-O Anionic Conductors with delta-Bi2O3 Fluorite-Type Structure (Ln=Y, Sm, Eu, Gd, Tb, Dy, Er, Yb)

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Journal of Solid State Chemistry, Vol. 134, Iss. 2, 1997-12 ,pp. : 219-226

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