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: 3165
Function: getPubMedXML
File: /var/www/html/application/controllers/Detail.php
Line: 597
Function: pubMedSearch_Global
File: /var/www/html/application/controllers/Detail.php
Line: 511
Function: pubMedGetRelatedKeyword
File: /var/www/html/index.php
Line: 317
Function: require_once
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Under the excitation of a 980 nm laser, the visible upconversion (UC) luminescence of Er ions doped Yb ions self-activated NaYb(MoO) phosphor and crystal, as well as the Yb/Er ions codoped NaBi(MoO) crystal were investigated comprehensively. The results indicate that all three samples exhibit two significant green emission bands and a weak red emission band in the visible band corresponding to the transitions of H/S → I and F → I of Er ions, respectively. Through the variable power density spectra of three different samples, the relationship between the energy back transfer (EBT) process of Yb-Er ions and the power density point and Yb ion concentration was investigated. The EBT process was observed in both the Er ions doped Yb ions self-activated NaYb(MoO) phosphor and crystal, as confirmed by the luminescence image of the sample. At high power density, the Yb ions self-activated sample exhibited yellow luminescence, with the crystal appearing later than the phosphor. In contrast, the NaBi(MoO) crystal displayed bright green emission within the measured power density range. In addition, by monitoring the relative intensity change of Yb emission in 5 at% Er:NaYb(MoO) crystal, the generation of EBT process in self-activated samples at high power density is more directly explained. These experimental results provide a reliable basis for our comprehensive understanding of the EBT mechanism, and also provide a reliable direction for the final determination of the optimal excitation power density for optical temperature measurement.
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Source |
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http://www.ncbi.nlm.nih.gov/pmc/articles/PMC12081802 | PMC |
http://dx.doi.org/10.1007/s12200-025-00155-5 | DOI Listing |