Severity: Warning
Message: file_get_contents(https://...@gmail.com&api_key=61f08fa0b96a73de8c900d749fcb997acc09&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: 3145
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
J Phys Chem Lett
†School of Photovoltaic and Renewable Energy Engineering, ‡School of Physics, and ¶School of Chemistry, University of New South Wales, Sydney, New South Wales 2052, Australia.
Published: June 2015
Molecular materials afford abundant flexibility in the tunability of physical and electronic properties. As such, they are ideally suited to engineering low-cost, flexible, light-harvesting materials that break away from the single-threshold paradigm. Single-threshold solar cells are capable of harvesting a maximum of 33.7% of incident sunlight, whereas two-threshold cells are capable of energy harvesting efficiencies exceeding 45%. In this Perspective, we provide the theoretical background with which upper efficiency limits for various multiple-threshold solar cell architectures may be calculated and review and discuss various reports that employ processes such as triplet-triplet annihilation and singlet fission in multiple-threshold devices comprised of molecular materials.
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http://dx.doi.org/10.1021/acs.jpclett.5b00716 | DOI Listing |
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