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
The electronic structure and thermoelectric properties of FeAsS are studied by the first-principles and the Boltzmann transport theory. The results show that FeAsS is a semiconductor with an indirect band gap of 0.73 eV. The dimensionless figure of merit () has obvious anisotropy, value along the - and -directions is significantly larger than that along the -direction, and p-type doping has better thermoelectric performance than n-type doping. The largest value can reach 0.84, which is for p-type doping along the -direction. The lattice thermal conductivity is extremely low, which is smaller than 1 W m K. The results show that FeAsS is a promising candidate for thermoelectric applications.
Download full-text PDF |
Source |
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http://www.ncbi.nlm.nih.gov/pmc/articles/PMC6644735 | PMC |
http://dx.doi.org/10.1021/acsomega.8b02042 | DOI Listing |
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