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: 176
Backtrace:
File: /var/www/html/application/helpers/my_audit_helper.php
Line: 176
Function: file_get_contents
File: /var/www/html/application/helpers/my_audit_helper.php
Line: 250
Function: simplexml_load_file_from_url
File: /var/www/html/application/helpers/my_audit_helper.php
Line: 1034
Function: getPubMedXML
File: /var/www/html/application/helpers/my_audit_helper.php
Line: 3152
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
In the present study, the effect of heterovalent Fe ions on the dielectric, pyroelectric, and ferroelectric properties of the (1 - )AgNbO-FeNbO ( = 0.005, 0.01, 0.025, 0.05, and 0.1) system was investigated. The substitution of smaller ionic radius Fe in B-sites and the formation of FeNbO as a secondary phase contributed to improved dielectric performance, especially the pyroelectric effect, of (1 - )AgNbO-FeNbO ceramics by generating electron-rich ceramics. The (1 - )AgNbO-FeNbO ceramics were prepared by conventional solid-state sintering. Pure AgNbO had a perovskite crystal structure with an orthorhombic crystal system, but the FeNbO in (1 - )AgNbO-FeNbO ceramics was formed as a secondary phase with a monoclinic structure. In addition, the XRD and Raman spectroscopy data showed that some Fe was substituted into B-sites of AgNbO. The introduction of FeNbO effectively reduced the average grain size from 1.85 ± 0.09 μm to 1.22 ± 0.03 μm for pure AgNbO and 0.9AgNbO-0.1FeNbO, respectively. In addition, the relative density of the (1 - )AgNbO-FeNbO ceramics decreased from 97.96% ± 0.01 for = 0 to 96.75% ± 0.03 for = 0.1. The real part of the permittivity ', at room temperature, increased from 186.6 for = 0 to a value of 738.7 for = 0.1. Additionally, the maximum pyroelectric coefficient increased fivefold, reaching values of 2270 nC cm K for = 0.1. Furthermore, a harvested pyroelectric energy density () of 1140 μJ cm for = 0.025 was achieved, which is appreciably higher than the 840 μJ cm value for = 0.
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Source |
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http://dx.doi.org/10.1039/d3dt02864j | DOI Listing |
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