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 spectra and predissociation dynamics of the Rydberg states 4pσB″∑(υ'=2) and 4pπD'Π(υ'=1) of the D molecule have been studied by a combination of XUV laser pump, UV laser probe, and velocity map imaging methods. The D(2) fragment yield spectrum and the D excitation spectrum have been measured. Although the predissociation rates were found to be small and comparable to the radiative decay rates, the D(2) fragments were observed for all the Rydberg states. The measured D(2) fragment angular distributions are in good agreement with a reported model that has an analytical formula for anisotropy parameters. The results demonstrated that the 4pσB″∑ and 4pπD'Π states dissociate via direct and indirect coupling with an ∑ state, respectively. For predissociation of the 4pσB″∑ state, the experimental data showed that D(1s) + D(2s) is the main channel, supporting previous theoretical predictions that the predissociation occurs by coupling to the vibrational continuum of the 3pσB'∑ state.
Download full-text PDF |
Source |
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http://dx.doi.org/10.1021/acs.jpca.2c04165 | DOI Listing |
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