TY - JOUR
T1 - High-pressure Synthesis of Ba2CoO2Ag2Te2with Extended CoO2Planes
AU - Matsumoto, Yuki
AU - Nambu, Yusuke
AU - Honda, Takashi
AU - Ikeda, Kazutaka
AU - Otomo, Toshiya
AU - Kageyama, Hiroshi
N1 - Funding Information:
This work was supported by CREST (JPMJCR1421), JSPS KAKENHI (JP16H06438, 17H05473, 19H04683), and JSPS Core-to-Core Program (A) Advanced Research Networks. Synchrotron and neutron experiments were performed at SPring-8 BL02B2 of JASRI (No. 2015B1111) and at J-PARC BL21 (No. 2019A0256), respectively. Y.M. was supported by JSPS for Young Scientists.
Publisher Copyright:
© 2020 American Chemical Society.
PY - 2020/6/15
Y1 - 2020/6/15
N2 - Using a high-pressure synthesis method, we prepared the layered oxychalcogenide Ba2CoO2Ag2Te2 (space group: I4/mmm) with alternating stacks of CoO2 and Ag2Te2 layers, separated by Ba atoms. The CoO2 plane is greatly extended (Co-O = 2.19 Å on average) due to tensile strain from adjacent Ag2Te2 layers, causing displacement of oxide anions. Layered cobaltates with trans-CoO4X2 (X = chalcogen, halogen) coordination feature large spin-orbit coupling, which is linearly scaled by the tetrahedral factor of dCo-X/dCo-O. However, applying this relation to Ba2CoO2Ag2Te2 yields a magnetic moment of ∼4 μB, which is nearly twice the experimentally observed value of 1.87(17) μB. This result, along with a reduced Néel temperature (TN = 60 K), originates from the off-centered position of otherwise under-bonded oxide anions, which changes the crystal field splitting of Co d orbitals.
AB - Using a high-pressure synthesis method, we prepared the layered oxychalcogenide Ba2CoO2Ag2Te2 (space group: I4/mmm) with alternating stacks of CoO2 and Ag2Te2 layers, separated by Ba atoms. The CoO2 plane is greatly extended (Co-O = 2.19 Å on average) due to tensile strain from adjacent Ag2Te2 layers, causing displacement of oxide anions. Layered cobaltates with trans-CoO4X2 (X = chalcogen, halogen) coordination feature large spin-orbit coupling, which is linearly scaled by the tetrahedral factor of dCo-X/dCo-O. However, applying this relation to Ba2CoO2Ag2Te2 yields a magnetic moment of ∼4 μB, which is nearly twice the experimentally observed value of 1.87(17) μB. This result, along with a reduced Néel temperature (TN = 60 K), originates from the off-centered position of otherwise under-bonded oxide anions, which changes the crystal field splitting of Co d orbitals.
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U2 - 10.1021/acs.inorgchem.0c00429
DO - 10.1021/acs.inorgchem.0c00429
M3 - Article
C2 - 32437136
AN - SCOPUS:85085771767
SN - 0020-1669
VL - 59
SP - 8121
EP - 8126
JO - Inorganic Chemistry
JF - Inorganic Chemistry
IS - 12
ER -