How to Obtainthe Blocking Energy Barrier of a CoAdatom on a Single MgO Layer: A Theoretical Exploration

Co adatoms deposited on a single MgO layer have been reported to exhibit a record-high zero-field splitting of 58 meV (467.8 cm<sup>–1</sup>). However, their effective blocking energy barrier is almost zero considering the much slower spin relaxation time on the order of 10<sup>–4</sup> s at 0.6 K induced by the significant quantum tunneling of magnetization (QTM) in the ground state (KD<sub>0</sub>). Herein, we propose two viable strategies to obtain the energy barrier by enlarging the Co–O or Mg–O bond lengths, which leads to the decreased QTM in KD<sub>0</sub> arising from the nearest four Mg ions around Co. Thus, it is an effective way to obtain the energy barrier by utilizing substrates that feature longer bond lengths between the transition metal ions of Mg<sup>2+</sup>, Ca<sup>2+</sup>, K<sup>+</sup>, etc. and the O, C, N, etc. in practical applications.

Publication Details

Journal
Figshare
Published
2025-02-22
DOI
https://doi.org/10.1021/acs.inorgchem.5c00058.s001
Primary Topic
Magnetic properties of thin films
Type
article
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article

How to Obtainthe Blocking Energy Barrier of a CoAdatom on a Single MgO Layer: A Theoretical Exploration

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Magnetic properties of thin films
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How to Obtainthe Blocking Energy Barrier of a CoAdatom on a Single MgO Layer: A Theoretical Exploration

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Abstract

Co adatoms deposited on a single MgO layer have been reported to exhibit a record-high zero-field splitting of 58 meV (467.8 cm<sup>–1</sup>). However, their effective blocking energy barrier is almost zero considering the much slower spin relaxation time on the order of 10<sup>–4</sup> s at 0.6 K induced by the significant quantum tunneling of magnetization (QTM) in the ground state (KD<sub>0</sub>). Herein, we propose two viable strategies to obtain the energy barrier by enlarging the Co–O or Mg–O bond lengths, which leads to the decreased QTM in KD<sub>0</sub> arising from the nearest four Mg ions around Co. Thus, it is an effective way to obtain the energy barrier by utilizing substrates that feature longer bond lengths between the transition metal ions of Mg<sup>2+</sup>, Ca<sup>2+</sup>, K<sup>+</sup>, etc. and the O, C, N, etc. in practical applications.

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Magnetic properties of thin films
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