Fluorescence spectra effect

Kalbitz, K., and Geyer, W. (2001). Humiflcation indices of water-soluble fulvic acids derived from synchronous fluorescence spectra - effects of spectrometer type and concentration, J. Plant Nutr. Soil Sci., 164(3), 259-265. 

A number of investigations of the copper-group oxides and dioxygen complexes have been reported. The electronic spectra of CuO, AgO, and AuO were recorded in rare-gas matrices (9), and it was found that the three oxides could be formed effectively by cocondensation of the metal atoms with a dilute, oxygen matrix, followed by near-ultraviolet excitation. The effective wavelengths for CuO or AgO formation were X > 300 nm and for AuO was X > 200 nm. In addition, the laser fluorescence spectrum of CuO in solid Ar has been recorded (97). 

A third possible channel of S state deexcitation is the S) —> Ti transition -nonradiative intersystem crossing isc. In principle, this process is spin forbidden, however, there are different intra- and intermolecular factors (spin-orbital coupling, heavy atom effect, and some others), which favor this process. With the rates kisc = 107-109 s"1, it can compete with other channels of S) state deactivation. At normal conditions in solutions, the nonradiative deexcitation of the triplet state T , kTm, is predominant over phosphorescence, which is the radiative deactivation of the T state. This transition is also spin-forbidden and its rate, kj, is low. Therefore, normally, phosphorescence is observed at low temperatures or in rigid (polymers, crystals) matrices, and the lifetimes of triplet state xT at such conditions may be quite long, up to a few seconds. Obviously, the phosphorescence spectrum is located at wavelengths longer than the fluorescence spectrum (see the bottom of Fig. 1). 

Gorsuch and Hercules 109> stated that certain discrepancies between the fluorescence spectrum of 3-amino-phthalate dianion and the chemiluminescence spectrum of luminol are partly due to reabsorption of the shorter-wavelength chemiluminescence light by the luminol monoanion. These authors confirmed the results of E. H. White and M. M. Bursey 114> concerning the very essential solvent effect on luminol chemiluminescence the relative intensity of the latter in anhydrous DMSO/t-BuOK/ oxygen was found to be about 30,000 times that in DMSO/28 mole % water/potassium hydroxide/oxygen. 

Beattie, I.R., Ozin, G.A., and Perry, R.O., Gas phase Raman spectra of P4, P2, As4 and As2. Resonance fluorescence spectrum of 80Se2. Resonance fluores-cence-Raman effects in the gas-phase spectra of sulfur and iodine. Effect of pressure on the depolarization ratios for iodine,. Chem. Soc., Perkin I, 2071, 1970. 

Such a solvent relaxation explains the increase in the red-shift of the fluorescence spectrum as the polarity of the solvent increases. The effect of polarity on fluorescence emission will be further discussed in Chapter 7, together with polarity probes. Moreover, when a cation receptor is linked to an intramolecular charge transfer fluorophore so that the bound cation can interact with either the donor group or the acceptor group, the ICT is perturbed the consequent changes in photophysical properties of the fluorophore can be used for sensing cations (see Section 10.3.3). 

Radiative transfer results in a decrease of the donor fluorescence intensity in the region of spectral overlap. Such a distortion of the fluorescence spectrum is called the inner filter effect (see Chapter 6). 

In order to minimize the effects of possible inaccuracy of the correction factors for the emission spectrum, the standard is preferably chosen to be excitable at the same wavelength as the compound, and with a fluorescence spectrum covering a similar wavelength range. 

It should again be emphasized that the determination of a true fluorescence spectrum and of a quantum yield requires the use of very dilute solutions or there may be some undesirable effects. 

Polarization effects The transmission efficiency of a monochromator depends on the polarization of light. This can easily be demonstrated by placing a polarizer between the sample and the emission monochromator it is observed that the position and shape of the fluorescence spectrum may significantly depend on the orientation of the polarizer. Consequently, the observed fluorescence intensity depends on the polarization of the emitted fluorescence, i.e. on the relative contribution of the vertically and horizontally polarized components. This problem can be circumvented in the following way. 

It should be recalled that, in polar rigid media, excitation on the red-edge of the absorption spectrum causes a red-shift of the fluorescence spectrum with respect to that observed on excitation in the bulk of the absorption spectrum (see the explanation of the red-edge effect in Section 3.5.1). Such a red-shift is still observable if the solvent relaxation competes with the fluorescence decay, but it disappears in fluid solutions because of dynamic equilibrium among the various solvation sites. 

A very marked effect of specific interactions can also be observed with anthroyl derivatives and in particular with methyl 8-(2-anthroyl)-octanoate. The fluorescence spectrum of this compound in hexane exhibits a clear vibrational structure, whereas in N,N-dimethylformamide and ethanol, the loss of vibrational structure is accompanied by a pronounced red-shift (Figure 7.6) (Perochon et al., 1991). 

The bisanthraceno-crown ether E-l (Figure 10.26) exhibits a fluorescence spectrum composed of the characteristic monomer and excimer bands. Gradual addition of sodium perchlorate to a solution in methanol induces a decrease in the monomer band and an increase in the excimer band. Complexation is indeed expected to bring closer together the two anthracene units, which favors excimer formation. A 2 1 (metabligand) complex is formed with Na+ in methanol and acetonitrile with a positive cooperative effect (see Appendix B). Interestingly, the overall stability constant obtained from absorption data was found to be lower than that... 

Observation of reorientational dynamics of dipolar groups surrounding the fluorophore in response to changes in the dipole moment of the fluorophore occurring upon electronic excitation. Such dynamics result in the appearance of spectral shifts with time,(1 ) in changes of fluorescence lifetime across the fluorescence spectrum,(7,32) and in a decrease in the observable effects of selective red-edge excitation.(1,24 33 34) The studies of these processes yield a very important parameter which characterizes dynamics in proteins— the reorientational dipolar relaxation time, xR. 

A variety of results obtained in studies of dipolar relaxation in the environment of the fluorescence probe 2,6-TNS are illustrated in Figure 2.10. In the model viscous medium (glycerol at 1 °C), the fluorescence spectra exhibit a marked dependence on the excitation wavelength. When 2 varies from 360 to 400 nm, the shift of the fluorescence spectrum maximum is 10 nm with a certain decrease of the half-width. In media with low viscosity, for instance, in ethanol (Figure 2.10a), this effect is never observed. 

Let us consider in greater detail the temperature dependence of the position of the maximum in the fluorescence spectrum of melittin (Figure 2.12). Three characteristic temperature regions may be distinguished. At T< 30 °C the spectrum does not depend on the temperature with excitation at both 280 nm and 305 nm in this case the red-edge effect is maximal. Evidently, the condition xR xF holds in this region. In the range 30 to 50 °C there is a... 

Fig. 7.6 The effect of denaturation on the fluorescence spectrum of fibroblast growth factor. An excitation spectra of native and denatured bFGF B Emission spectra of native and denatured bFGF. Reproduced with permission from J. Pharm. Biomed. Anal. (See Reference 1).

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