Page 18 - Academic Press Encyclopedia of Physical Science and Technology 3rd Analytical Chemistry
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              Analytical Chemistry                                                                        557


















                     FIGURE 10 Schematic representation of an X-ray fluorescence spectrometer employing both wavelength dispersion
                     and energy dispersion.

              topaz) mounted on a goniometer to satisfy Bragg’s  nant effect between an incoming photon and the electrons
              law,                                              of a chromophore, elevating the valence electronic con-
                                                                figuration to a higher energy state. Fluorescence is said to
                               nλ = 2d sin θ,
                                                                occur when the system relaxes to a lower energy state by
              where n is an integer, λ is the wavelength, and θ is the  the release of radiation within 10 −8  sec after absorption
              angle at which constructive interference occurs. Energy-  in a process that ceases in less than 10 −6  sec. Resonance
              dispersive systems (see Section II.B.3.b) employing pulse  fluorescence occurs when the absorbed radiation is reemit-
              height analysis can be used in conjunction with wave-  ted at the same wavelength. Polyatomic molecules often
              length dispersion to distinguish between two or more en-  reemit at wavelengths longer than those absorbed, produc-
              ergies of photons appearing at one angle due to differ-  ing a spectral feature known as a Stokes shift. This is due
              ent values of n, or a multichannel analyzer for discrete  to nonradiative energy losses by molecular vibration in the
              energy measurement can be independently employed. A  electronically excited state. The closely related processes
              schematic representation of a combined wavelength- and  of fluorescence and phosphorescence are summarized in
              energy-dispersive system is shown in Fig. 10.     Fig. 11. Phosphorescence occurs from a forbidden excited
                                                                triplet state after inter-system crossing and may take a pe-
                                                                riod of seconds. This phenomenon is often of very weak
                2. Molecular Emission
                                                                intensity and is not as common as fluorescence, thereby
                Fluorescence spectroscopy. Molecular absorp-    limitingitsanalyticalpotential.Competitionbetweennon-
              tion of ultraviolet or visible radiation results from a reso-  radiative and fluorescent energy loss occurs, reducing the




























                                    FIGURE 11 Energies of fluorescence and phosphorescence processes.
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