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Crystal structure refinements of stoichiometric Ni 3 Se 2 and NiSe
Author(s) -
Unoki Kohei,
Yoshiasa Akira,
Kitahara Ginga,
Nishiayama Tadao,
Tokuda Makoto,
Sugiyama Kazumasa,
Nakatsuka Akihiko
Publication year - 2021
Publication title -
acta crystallographica section c
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.304
H-Index - 17
ISSN - 2053-2296
DOI - 10.1107/s2053229621002187
Subject(s) - crystallography , stoichiometry , crystal structure , crystal (programming language) , nickel , bond length , materials science , space group , octahedron , single crystal , x ray crystallography , chemistry , analytical chemistry (journal) , diffraction , metallurgy , physics , chromatography , computer science , programming language , optics
Single crystals of Ni 3 Se 2 (trinickel diselenide) and NiSe (nickel selenide) with stoichiometric chemical compositions were grown in evacuated silica‐glass tubes. The chemical compositions of the single crystals of Ni 3 Se 2 and NiSe were determined by scanning electron microscopy and energy‐dispersive X‐ray spectroscopy (SEM/EDS). The crystal structures of Ni 3 Se 2 [rhombohedral, space group R 32, a = 6.02813 (13), c = 7.24883 (16) Å, Z = 3] and NiSe [hexagonal, space group P 6 3 / mmc , a = 3.66147 (10), c = 5.35766 (16) Å, Z = 2] were analyzed by single‐crystal X‐ray diffraction and refined to yield R values of 0.020 and 0.018 for 117 and 85 unique reflections, respectively, with F o > 4σ( F o ). R 32 is a Sohncke type of space group where enantiomeric structures can exist; the single‐domain structure obtained by the refinement was confirmed to be correct by a Flack parameter of −0.05 (2). The existence of Ni—Ni bonds was confirmed in both compounds, in addition to the Ni—Se bonds. The value of the atomic displacement parameter (mean‐square displacement) of each atom in NiSe was larger than that in Ni 3 Se 2 . The larger amplitude of the atoms in NiSe corresponds to longer Ni—Se and Ni—Ni bond lengths in NiSe than in Ni 3 Se 2 . The Debye temperatures, gθ D , estimated from observed mean‐square displacements for Ni and Se in Ni 3 Se 2 , were 322 and 298 K, respectively, while those for Ni and Se in NiSe were 246 and 241 K, respectively. The existence of large cavities in the structure and the weak bonding force are likely responsible for the brittle and soft nature of the NiSe crystal.