Severity: Warning
Message: file_get_contents(https://...@pubfacts.com&api_key=b8daa3ad693db53b1410957c26c9a51b4908&a=1): Failed to open stream: HTTP request failed! HTTP/1.1 429 Too Many Requests
Filename: helpers/my_audit_helper.php
Line Number: 197
Backtrace:
File: /var/www/html/application/helpers/my_audit_helper.php
Line: 197
Function: file_get_contents
File: /var/www/html/application/helpers/my_audit_helper.php
Line: 271
Function: simplexml_load_file_from_url
File: /var/www/html/application/helpers/my_audit_helper.php
Line: 1057
Function: getPubMedXML
File: /var/www/html/application/helpers/my_audit_helper.php
Line: 3175
Function: GetPubMedArticleOutput_2016
File: /var/www/html/application/controllers/Detail.php
Line: 575
Function: pubMedSearch_Global
File: /var/www/html/application/controllers/Detail.php
Line: 489
Function: pubMedGetRelatedKeyword
File: /var/www/html/index.php
Line: 316
Function: require_once
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). However, their effective blocking energy barrier is almost zero considering the much slower spin relaxation time on the order of 10 s at 0.6 K induced by the significant quantum tunneling of magnetization (QTM) in the ground state (KD). 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 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, Ca, K, etc. and the O, C, N, etc. in practical applications.
Download full-text PDF |
Source |
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http://dx.doi.org/10.1021/acs.inorgchem.5c00058 | DOI Listing |
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