2011
DOI: 10.1016/j.jlumin.2010.10.008
|View full text |Cite
|
Sign up to set email alerts
|

Intermolecular repulsive–dispersive potentials explain properties of impurity spectra in soft solids

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
8
0

Year Published

2011
2011
2020
2020

Publication Types

Select...
7
1

Relationship

3
5

Authors

Journals

citations
Cited by 10 publications
(8 citation statements)
references
References 29 publications
0
8
0
Order By: Relevance
“…The excitonic lineshapes from all states are then summed to produce the pre-burn absorption spectrum. The calculated line shapes depend in both cases on the temperature (T, set to 5 K in these calculations), electronÀphonon coupling strength S (which, although not considered here, has for some systems 21 been suggested to itself vary with site energy), and the phonon spectral density (or equivalently, the one-phonon profile, in HB terminology 11 ). In the more flexible density matrix theory, the line shape also depends on the pigment site energies and an assumed correlation radius for protein phonon modes (see Supporting Information for further comparison of the present method with the formulas used in previous work).…”
Section: Section: Kinetics Spectroscopymentioning
confidence: 99%
“…The excitonic lineshapes from all states are then summed to produce the pre-burn absorption spectrum. The calculated line shapes depend in both cases on the temperature (T, set to 5 K in these calculations), electronÀphonon coupling strength S (which, although not considered here, has for some systems 21 been suggested to itself vary with site energy), and the phonon spectral density (or equivalently, the one-phonon profile, in HB terminology 11 ). In the more flexible density matrix theory, the line shape also depends on the pigment site energies and an assumed correlation radius for protein phonon modes (see Supporting Information for further comparison of the present method with the formulas used in previous work).…”
Section: Section: Kinetics Spectroscopymentioning
confidence: 99%
“…According to Equation (5), the ΔFLN spectrum displays an origin band that comprises the ZPL and PSB components, with intertwined I vib + I mq vibrational sidebands extending toward longer wavelengths. The shape of the origin band I 00 (ν) is known to depend on the excitation wavelength, with significant variations observed even for small changes within the inhomogeneous spread of ZPL frequencies, showing enhancement of the electron-phonon coupling strength with increasing transition wavelength (Rätsep et al, 2009b ; Renge et al, 2011 ). Comparing the low-resolution spectra obtained in different environments, one may conclude that the vibrational sideband is more intense in 1-propanol than in TEA, details of which are revealed by the ΔFLN spectra.…”
Section: Resultsmentioning
confidence: 99%
“…The measurements were performed at 4.5 ± 0.2 K in a He bath cryostat (Utreks), as described previously. Selective excitation of fluorescence was performed using a model 375 dye laser or a Ti:sapphire laser of <0.5 cm –1 line width pumped by a Millennia Prime solid-state laser (all Spectra-Physics). Nonselective fluorescence was excited by a 5 mW diode laser at 407 nm.…”
Section: Experimental and Computational Methodsmentioning
confidence: 99%