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Emission band

Description of Method. Quinine is an alkaloid used in treating malaria (it also is found in tonic water). It is a strongly fluorescent compound in dilute solutions of H2SO4 (f = 0.55). The excitation spectrum of quinine shows two absorption bands at 250 nm and 350 nm, and the emission spectrum shows a single emission band at 450 nm. Quinine is rapidly excreted from the body in urine and is easily determined by fluorescence following its extraction from the urine sample. [Pg.431]

Minimizing Spectral Interferences The most important spectral interference is a continuous source of background emission from the flame or plasma and emission bands from molecular species. This background emission is particularly severe for flames in which the temperature is insufficient to break down refractory compounds, such as oxides and hydroxides. Background corrections for flame emission are made by scanning over the emission line and drawing a baseline (Figure 10.51). Because the temperature of a plasma is... [Pg.437]

Fig. 5. The emission spectmm of a typical cool white halophosphate phosphor showing the emission band around 480 nm and the emission... Fig. 5. The emission spectmm of a typical cool white halophosphate phosphor showing the emission band around 480 nm and the emission...
Combined Soot W2O, and CO2 Radiation The spectral overlap of H9O and CO9 radiation has been taken into account by the constants for obtaining Ec- Additional overlap occurs when soot emissivity , is added. If the emission bands of water vapor and CO9 were randomly placed in the spectrum and soot radiation were gray, the combined emissivity would be Eg phis , minus an overlap correction g s- But monochromatic soot emissivity is higher the shorter the wavelength, and in a highly sooted flame at 1500 K half the soot emission hes below 2.5 [Lm where H9O and CO9 emission is negligible. Then the correction g s must be reduced, and the following is recommended ... [Pg.582]

In the case of substances whose structures are pH-dependent (e.g. phenols, carboxylic and sulfonic acids, amines etc.) it is possible to produce fluorescences or make them disappear by the deliberate manipulation of the pH [213] (Table 20). Shifts of the positions of the absorption and emission bands have also been reported. This is particularly to be observed in the case of modified silica gels, some of which are markedly acidic or basic in reaction (Table 25). [Pg.91]

Absorption and emission spectra of six 2-substituted imidazo[4,5-/]quinolines (R = H, Me, CH2Ph, Ph, 2-Py, R = H CH2Ph, R = Ph) were studied in various solvents. These studies revealed a solvent-independent, substituent-dependent character of the title compounds. They also exhibited bathochromic shifts in acidic and basic solutions. The phenyl group in the 2-position is in complete conjugation with the imidazoquinoline moiety. The fluorescence spectra of the compounds exhibited a solvent dependency, and, on changing to polar solvents, bathochromic shifts occur. Anomalous bathochromic shifts in water, acidic solution, and a new emission band in methanol are attributed to the protonated imidazoquinoline in the excited state. Basic solutions quench fluorescence (87IJC187). [Pg.239]

The nature of the light emissions is influenced by the way in which the absorbed energy is transferred through the polymer matrix. In crystalline polymers, exciton migration is possible as all molecules lose their energetic individuality and all electronic and oscillation levels are coupled [20]. Thus, new exciton absorption and emission bands are formed and the excitation energy can move along the chain ... [Pg.401]

For copolymers of structure I, for both types of side-chains, there is a striking similarity with the optical properties of the corresponding models the absorption and photoluminescence maxima of the polymers arc only 0.08-0.09 eV red-shifted relative to those of the models, as shown in Figure 16-9 (left) for the octyloxy-substituted compounds. The small shift can be readily explained by the fact that in the copolymers the chromophorcs are actually substituted by silylene units, which have a weakly electron-donating character. The shifts between absorption and luminescence maxima are exactly the same for polymers and models and the width of the emission bands is almost identical. The quantum yields are only slightly reduced in the polymers. These results confirm that the active chro-mophores are the PPV-type blocks and that the silylene unit is an efficient re-conjugation interrupter. [Pg.298]

Apart from the interferences which may arise from other elements present in the substance to be analysed, some interference may arise from the emission band spectra produced by molecules or molecular fragments present in the flame gases in particular, band spectra due to hydroxyl and cyanogen radicals arise in many flames. Although in AAS these flame signals are modulated (Section 21.9), in practice care should be taken to select an absorption line which does not correspond with the wavelengths due to any molecular bands because of the excessive noise produced by the latter this leads to decreased sensitivity and to poor precision of analysis. [Pg.792]

A typical procedure is shown in Figure 2. Other dyes besides ethidium can be used, although ethidium has an advantage in that its excitation emission bands are well removed from any protein absorbances. A standard curve can be constructed for the nucleic acid of concern and the limits of detection established. In Step 3, proteolytic enzymes may be substituted for heparin, or the step may be bypassed in the case of proteins which do not interfere. After measurement of the unknown sample the nucleic acid concentration may be simply calculated or read from the standard curve. [Pg.49]

Luminescence studies revealed that compounds (119)-(121) displayed broad emission bands at 298 K, with ranging from 387 nm to 371 nm for the P to Bi derivatives, respectively [92]. On cooling to 77 K, compound (119) displays both a fluorescent band nm) and a phosphorescent... [Pg.158]

Figures 21.16, 21.17 and 21.18 show the X-ray-excited luminescence properties of Ce -activated Ba3BP30i2, BaBPOs and Ba3BP07 respectively. They all show a broad emission band with peak center at about 351 nm for Ba3BP30i2 Ce, ... Figures 21.16, 21.17 and 21.18 show the X-ray-excited luminescence properties of Ce -activated Ba3BP30i2, BaBPOs and Ba3BP07 respectively. They all show a broad emission band with peak center at about 351 nm for Ba3BP30i2 Ce, ...
Figure 21.22 shows the comparison between the XEL spectra of Ba3BP3 Oi2 Eu and that of Bi4Ge30i2 powders with the same measurement conditions. It is worthwhile to note that both spectra have a similar broad emission band. The integral area of the emission bands for Ba3BP30i2 Eu powders is... [Pg.319]

Fig. 6 shows PL spectra of CdS nanoparticles and CdS-ZnS core-shell nanoparticles. In PL spectrum of CdS nanoparticles, the emission band is seen at around 400nm. The emission band of CdS-ZnS core-shell nanoparticles is higher dian that of CdS ones at around 400nm. The PL enhancement of CdS-ZnS core-shell nanoparticl is due to passivation which means that surface atoms are bonded to the shell material of similar lattice constant and much larger band gap [9], Althou the sur ce treatment conditions are different, the ranission band of CdS-ZnS core-shell nanoparticles is same in PL spectra of Fig. 6(b). This indicates that interfacial state between CdS core and shell material was unchan d by different surfaKs treatment. [Pg.760]


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Band emission spectra

Band-edge emission

Combustion gases emission band

Composites valence band emission

Emission spectrum banding series

Inhomogeneous bands emission

Near-band-edge emission

Polycyclic aromatic hydrocarbons infrared emission bands

Rare Earth Ions (Band Emission)

Singlet emission band

Spectral emission bands

Unidentified infrared emission bands

Valence-band emission

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