1990
DOI: 10.1021/ed067p32
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Grid of expressions related to the Einstein coefficients

Abstract: The following is a collection of all of the relations of Einstein coefficients.

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Cited by 12 publications
(5 citation statements)
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“…In this approximation, which has been found to give a fairly accurate quantitative description of several different molecular systems, the coupling between two CN-stretch modes a and b is given by J a b = 1 4 normalπ normalε 0 [ true normalμ false→ a · true normalμ false→ b r a b 3 3 false( r⃗ a b · true normalμ false→ a false) false( r⃗ a b · true normalμ false→ b false) r a b 5 ] where μ⃗ a , b are the CN-stretch transition dipoles and r ⃗ ab is the distance vector between the two transition dipoles. The magnitude of the CN-stretch transition-dipole moment can be determined from the integrated absorption coefficient, and from the experimental FTIR spectrum (Figure ), we obtain |μ⃗| = 0.089 D. Using the geometrical parameters of the polyisocyanide helix ( r = 2.3 Å, ∠(μ⃗ i , μ⃗ i +1 ) = 90°, ∠(μ⃗ i , r ⃗ i , i +1 ) = 56°), we find J 1 = 7 cm −1 . This implies an ω A − ω E frequency splitting of 14 cm −1 , which agrees reasonably well (both in sign and magnitude) with the experimental value of 8 cm −1 , thus confirming our assigment of the strong absorption band to the E mode and of the shoulder to the A mode.…”
Section: Resultsmentioning
confidence: 85%
“…In this approximation, which has been found to give a fairly accurate quantitative description of several different molecular systems, the coupling between two CN-stretch modes a and b is given by J a b = 1 4 normalπ normalε 0 [ true normalμ false→ a · true normalμ false→ b r a b 3 3 false( r⃗ a b · true normalμ false→ a false) false( r⃗ a b · true normalμ false→ b false) r a b 5 ] where μ⃗ a , b are the CN-stretch transition dipoles and r ⃗ ab is the distance vector between the two transition dipoles. The magnitude of the CN-stretch transition-dipole moment can be determined from the integrated absorption coefficient, and from the experimental FTIR spectrum (Figure ), we obtain |μ⃗| = 0.089 D. Using the geometrical parameters of the polyisocyanide helix ( r = 2.3 Å, ∠(μ⃗ i , μ⃗ i +1 ) = 90°, ∠(μ⃗ i , r ⃗ i , i +1 ) = 56°), we find J 1 = 7 cm −1 . This implies an ω A − ω E frequency splitting of 14 cm −1 , which agrees reasonably well (both in sign and magnitude) with the experimental value of 8 cm −1 , thus confirming our assigment of the strong absorption band to the E mode and of the shoulder to the A mode.…”
Section: Resultsmentioning
confidence: 85%
“…[a] Notation: q m —monolayer capacity (molecule number); K L , K SV —binding constants from the Langmuir isotherm and the Stern–Volmer equation, respectively; Δ G L , Δ G SV —free Gibbs energies calculated based on the value of K L and K SV in accordance with the equation Δ G =− RT Ln( K ); the value of dipole transition moment μ in RhB, taken for the calculation of α , was established from the UV/Vis spectra: it is 15.227 D.…”
Section: Resultsmentioning
confidence: 99%
“…First of all, the integrated absorption coefficient (IAC) can be extracted. 58 This extinction coefficient is defined in terms of the optical density, IAC = R e dn, where n denotes the wave number. The IAC can be computed as the area under optical density (expressed in terms of dm 3 mol À1 cm À1 ) as a function of the wave number.…”
Section: Deconvolution Of the Visible Spectrummentioning
confidence: 99%