1980
DOI: 10.1021/ac50058a024
|View full text |Cite
|
Sign up to set email alerts
|

Determination of the absolute quantum efficiency of luminescence of solid materials employing photoacoustic spectroscopy

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

0
26
0

Year Published

1983
1983
2017
2017

Publication Types

Select...
4
3

Relationship

0
7

Authors

Journals

citations
Cited by 79 publications
(26 citation statements)
references
References 21 publications
(4 reference statements)
0
26
0
Order By: Relevance
“…20p), when the PA amplitude is independent of the sample's absorption coefficient, Adams and co-workers proposed a method to measure the absolute luminescence quantum yield by PA amplitude spectra. [47] The method is based on the fact that the efficiency factor, which converts absorbed power into heat by nonradiative relaxation, varies at different incident wavelengths, resulting in a corresponding variation of PA amplitudes. Overall quantum yields for EuA C H T U N G T R E N N U N G (tta) 3 L 2 at different temperatures are determined from PA amplitude in the 330-400 nm region at a modulation frequency of 33 Hz.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…20p), when the PA amplitude is independent of the sample's absorption coefficient, Adams and co-workers proposed a method to measure the absolute luminescence quantum yield by PA amplitude spectra. [47] The method is based on the fact that the efficiency factor, which converts absorbed power into heat by nonradiative relaxation, varies at different incident wavelengths, resulting in a corresponding variation of PA amplitudes. Overall quantum yields for EuA C H T U N G T R E N N U N G (tta) 3 L 2 at different temperatures are determined from PA amplitude in the 330-400 nm region at a modulation frequency of 33 Hz.…”
Section: Resultsmentioning
confidence: 99%
“…Both the PA phase and amplitude signals were normalized by use of the carbon black reference. Overall quantum yields of EuA C H T U N G T R E N N U N G (tta) 3 L 2 at different temperatures are determined from [47] where A is the PA amplitude at wavelength l 0 , K is a constant representing the thermal properties of the sample and the instrumental arrangement employed, l F is the mean frequency of the luminescence radiation (l F ¼ R I l Á ldl= R I l dl, where I l is the emission intensity at wavelength l) and f tal is the luminescence quantum yield. The subscripts F and NF refer to the luminescence sample and carbon black reference, respectively.…”
Section: Methodsmentioning
confidence: 99%
“…It is also a known fact that the absorption coefficients measured for the same tissue are different in vitro and in vivo [20]. Besides of the concentration, a strong effect on the optical properties of blood arises from the shape, the velocity, aggregation and sedimentation of the erythrocytes [21].…”
Section: Resultsmentioning
confidence: 99%
“…The PA signal is obtained by detecting the heat generated through non-radiative transitions by the sample after absorbing a periodically varying incident light [7][8][9]. The PA spectra of the silica samples are shown in Fig.…”
Section: Pa and Luminescence Spectramentioning
confidence: 99%
“…It is found that A was proportional to ω −1 . It means that PA saturation occurs and A is independent of the sample's absorption coefficient [8]. As the thermal properties of the samples are basically the same, A is proportional to the probability of non-radiative transitions of the samples.…”
Section: Pa and Luminescence Spectramentioning
confidence: 99%