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: 3122
Function: getPubMedXML
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
Strain engineering can effectively improve the energy band degeneracy of two-dimensional transition metal dichalcogenides so that they exhibit good thermoelectric properties under strain. In this work, we have studied the phonon, electronic, thermal, and thermoelectric properties of 1T-phase monolayer HfS with biaxial strain based on first-principles calculations combined with Boltzmann equations. At 0% strain, the results show that the lattice thermal conductivity of monolayer HfS is 5.01 W m K and the electronic thermal conductivities of n-type and p-type doped monolayer HfS are 2.94 and 0.39 W m K, respectively, when the doping concentration is around 5 × 10 cm. The power factors of the n-type and p-type doped monolayer HfS are different, 29.4 and 1.6 mW mK, respectively. Finally, the maximum value of the n-type monolayer HfS is 1.09, which is higher than 0.09 of the p-type monolayer HfS. Under biaxial strain, for n-type HfS, the lattice thermal conductivity, the electronic thermal conductivity, and the power factor are 1.55 W m K, 1.44 W m K, and 22.9 mW mK at 6% strain, respectively. Based on the above factor, the value reaches its maximum of 2.29 at 6% strain. For p-type HfS, the lattice thermal conductivity and the electronic thermal conductivity are 1.12 and 1.53 W m K at 7% strain, respectively. Moreover, the power factor is greatly improved to 29.5 mW mK. Finally, the maximum value of the p-type monolayer HfS is 3.35 at 7% strain. It is obvious that strain can greatly improve the thermoelectric performance of monolayer HfS, especially for p-type HfS. We hope that the research results can provide data references for future experimental exploration.
Download full-text PDF |
Source |
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http://www.ncbi.nlm.nih.gov/pmc/articles/PMC8582045 | PMC |
http://dx.doi.org/10.1021/acsomega.1c04286 | DOI Listing |
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