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File: /var/www/html/index.php
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Function: require_once
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Filename: Session/Session.php
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File: /var/www/html/index.php
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Function: require_once
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Filename: helpers/my_audit_helper.php
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File: /var/www/html/application/helpers/my_audit_helper.php
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Function: file_get_contents
File: /var/www/html/application/helpers/my_audit_helper.php
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Function: simplexml_load_file_from_url
File: /var/www/html/application/helpers/my_audit_helper.php
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Function: getPubMedXML
File: /var/www/html/application/controllers/Detail.php
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Function: pubMedSearch_Global
File: /var/www/html/application/controllers/Detail.php
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Function: pubMedGetRelatedKeyword
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Function: require_once
Spin reorientation is a magnetic phase transition in which rotation of the magnetization vector with respect to the crystallographic axes occurs upon a change in the temperature or magnetic field. For example, SmFeO shows a magnetization rotation from the axis above 480 K to the axis below 450 K, known as the Γ → Γ transition. This work reports the successful synthesis of the new single-crystal perovskite SmFeMnO and finds interesting spin reorientations above and below room temperature. In addition to the spin reorientation of the Γ → Γ magnetic phase transition observed at around = 382 K, a new spin reorientation, Γ → Γ, was seen at around = 212 K due to Mn doping, which could not be observed in the parent rare earth perovskite compound. This unexpected spin configuration has complete antiferromagnetic order without any canting-induced weak ferromagnetic moment, resulting in zero magnetization in the low-temperature regime. - and - measurements have been made to study the temperature and magnetic-field dependence of the observed spin reorientation transitions.
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Source |
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http://www.ncbi.nlm.nih.gov/pmc/articles/PMC5619851 | PMC |
http://dx.doi.org/10.1107/S205225251700793X | DOI Listing |
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