The LaNiIn1-xMx (M = Al, Ge) systems

Zaremba, Nazar; Schepilov, Yu.; Nychyporuk, G.; Muts, Ihor; Pavlyuk, Volodymyr; Zaremba, Vasyl’ I.

doi:10.30970/vch.6101.044

Cited by 4 publications

(1 citation statement)

References 11 publications

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“…Віддалі M2-Ni2 (δ = 0,2695 нм) сумірні з сумою ковалентних радіусів атомів нікелю та статиcтичної суміші In/Sn. [20,21], де під час взаємного заміщення атомів р-елементів формуються тверді розчини різної протяжності.…”

Section: результати досліджень та їх обговоренняunclassified

Crystal structure of the CeNi3In5Sn phase

Dominyuk,

Nychyporuk,

Muts

et al. 2023

Visnyk Lviv Univ. Ser. Chem.

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Section: результати досліджень та їх обговоренняunclassified

Crystal structure of the CeNi3In5Sn phase

Dominyuk,

Nychyporuk,

Muts

et al. 2023

Visnyk Lviv Univ. Ser. Chem.

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The solid solutions TbCuIn_1–x M _x (M = Al, Ga)

Horiacha

Nychyporuk

Pöttgen

et al. 2022

Zeitschrift Für Naturforschung B

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The complete solid solutions TbCuIn1–x M x (M = Al, Ga) were studied by powder X-ray diffraction and scanning electron microscopy for samples equilibrated at T = 873 K. The influence of In substitution by Al or Ga, the solubility ranges and the changes of unit cell parameters have been determined: TbCuIn1.0–0Al0–1.0 (ZrNiAl type, space group P 6 ‾ 2 $\overline{6}2$ m, a = 0.7457(1)–0.7035(1), c = 0.3958(1)–0.4044(1) nm, V = 0.1906–0.1733 nm3); TbCuIn1–0.8Ga0–0.2 (ZrNiAl type, a = 0.74569(5)–0.73882(13), с = 0.39582(3)–0.39663(14) nm, V = 0.1906–0.1875 nm3); TbCuIn0.3–0Ga0.7–1.0 (KHg2 type, Imma, а = 0.43943(9)–0.43750(5), b = 0.70833(12)–0.70537(6), с = 0.74866(12)–0.74525(7) nm, V = 0.2330–0.2300 nm3). The crystal structure of TbCuIn0.42(1)Al0.58(1) was refined from single-crystal X-ray diffractometer data: ZrNiAl type, P 6 ‾ 2 $\overline{6}2$ m, a = 0.71633(6), c = 0.40785(3) nm, wR2 = 0.0379, 291 F 2 values and 16 variables. The basic crystal chemical features are discussed.

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LaNiIn_1–xSn_x and CeNiIn_1–xSn_x solid solutions at T = 870 K

Nychyporuk

Dominyuk

Muts

et al. 2023

Zeitschrift Für Naturforschung B

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The solid solutions LaNiIn1–x Sn x and CeNiIn1–x Sn x were studied by means of X-ray powder diffraction and EDX analyses in the full concentration range for samples annealed at T = 870 K. The limited solubility of the fourth component in the starting compounds with equiatomic composition, and the limits and the unit cell parameters of the solid solutions have been determined. The crystal structure of CeNiIn0.57Sn0.43 was refined from single-crystal X-ray diffraction data: ZrNiAl-type structure; hexagonal space group P 6 ‾ $\bar{6}$ 2m, a = 0.74213(10), c = 0.40825(8) nm, R 1 = 0.0155, wR 2 = 0.0303, 282 independent hkl reflections and 15 refined parameters. The existence ranges within the solid solutions are discussed.

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The LaNiIn1-xMx (M = Al, Ge) systems

Cited by 4 publications

References 11 publications

Crystal structure of the CeNi3In5Sn phase

Crystal structure of the CeNi3In5Sn phase

The solid solutions TbCuIn_1–x M _x (M = Al, Ga)

LaNiIn_1–xSn_x and CeNiIn_1–xSn_x solid solutions at T = 870 K

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The LaNiIn1-xMx (M = Al, Ge) systems

Cited by 4 publications

References 11 publications

Crystal structure of the CeNi3In5Sn phase

Crystal structure of the CeNi3In5Sn phase

The solid solutions TbCuIn1–x M x (M = Al, Ga)

LaNiIn1–x Sn x and CeNiIn1–x Sn x solid solutions at T = 870 K

Contact Info

Product

Resources

About

The solid solutions TbCuIn_1–x M _x (M = Al, Ga)

LaNiIn_1–xSn_x and CeNiIn_1–xSn_x solid solutions at T = 870 K