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 excited state dynamics of periodic mesoporous organosilica (powder) bearing biphenylylene moieties densely in the silica framework (Bp-PMO) is investigated for the first time using femtosecond time-resolved diffuse reflectance (TDR) and picosecond time-resolved fluorescence spectroscopies. The TDR spectra revealed the excitation-relaxation process of the biphenylylene moieties, including the relaxation of the twisted Frank-Condon (FC) state to the lowest singlet excited state (S(1)) with a time constant of 730 ± 95 fs, and efficient quenching of the S(1) state by excimer (E) formations with two time constants of 7.0 ± 0.2 ps (E(1): ca. 64%) and 170 ± 47 ps (E(2) and E(3): ca. 36%). The individual absorption spectra of the FC, S(1), and E states were reconstructed by the TDR spectral analysis. The time-resolved fluorescence spectra showed that the excimers decayed with three time constants of 1.3 ± 0.2 ns (E(1)), 8.2 ± 0.7 ns (E(2)) and 27 ± 2 ns (E(3)). The fluorescence quantum yields of the excimers are suggested to be almost zero for E(1), and unity for E(2) and E(3), which implies that the fluorescence quantum yield of Bp-PMO (Φ(F) = 0.38) can be explained by the fraction of the highly emissive excimers (E(2) and E(3)). The excited state dynamics of Bp-PMO is quite different from those of a solution of 4,4'-bis-(triethoxysilyl)biphenyl precursor and a biphenyl molecular crystal (powder).
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Source |
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http://dx.doi.org/10.1039/c004255b | DOI Listing |
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