Page 96 - Academic Press Encyclopedia of Physical Science and Technology 3rd BioTechnology
P. 96

P1: GNB Final Pages
 Encyclopedia of Physical Science and Technology  EN005F-954  June 15, 2001  20:48







              Fiber-Optic Chemical Sensors                                                                809

              can be measured using several different optical phenom-
              ena. These phenomena transduce the interactions of light
              with the sensing materials into an (ideally) quantitative
              signal that can be correlated to the analyte identities and
              concentrations.

                1. Absorption

              Absorption is based on the light intensity changes due to
              modulation by a substance in the sample. Light absorp-
              tion is a process in which electromagnetic energy is trans-
              ferred to an atom or a molecule. This energy promotes the
              transition of the molecule from the ground energy state
              to a higher energy excited state. The resulting energy is
              dissipated nonradiatively (i.e., thermally) to the medium
              when the excited state relaxes to the ground state. Each  FIGURE 6 Typical fluorescence spectrum showing the strokes
              molecule (analyte) can be excited at a single wavelength or  shift at longer wavelengths from the excitation spectrum.
              several wavelengths, which furnishes a unique absorption
              spectrum characteristic of the molecule. The absorbance
                                                                  3. Time-Resolved Fluorescence Spectroscopy
              changes are related to the analyte concentration [C] via
              the Beer–Lambert relationship:                    This method is based on the excited-state lifetime. The
                                                                light intensity emitted from molecules excited by a short
                          A = log(I 0 /I) = ε · [C] · l,  (4)
                                                                pulse of light decays exponentially with time. This decay
              where A is the optical absorbance, I 0 and I are the inten-  pattern is unique for each molecule and can be used for
              sities of transmitted light in the absence and presence of  analytical purposes. Alternatively, a phase shift method
              the absorbing species, respectively, l is the effective path  can be employed to measure the fluorescence lifetime. A
              length, and ε is the molar absorption coefficient. In prac-  sinusoidally varying excitation light source is used and the
              tice, optical fibers are connected to a spectrophotometer  phase shift between the excitation waveform and the emis-
              and the measured changes correlate the analyte concen-  sion waveform can be used to detect the analytical signal.
              tration to the absorption at a given wavelength.
                                                                  4. Fluorescence Energy Transfer
                2. Fluorescence
                                                                This phenomenon occurs when two distinct fluorophores
              When fluorescent molecules are excited at a specificwave-  are present. If the emission spectrum of one fluorophore
              length, the molecule reemits radiation at a lower energy,  overlaps with the excitation spectrum of a second fluo-
              i.e., a longer wavelength. The absorption of the excitation  rophore and the two fluorophores are in sufficient prox-
                                                                          ˚
              light shifts the molecule’s energy from the ground state to  imity (<100 A), then the excited fluorophore (donor) can
              a higher energy state. The molecule emits fluorescent light  transfer energy nonradiatively to the second fluorophore
              when it returns to the ground state. The distinct ranges of  (acceptor). This transfer results in an increase in light
              wavelengths over which the molecule is excited and emits  emission by the acceptor and a decrease in light emis-
              are well defined and simple to detect, as shown in a typical  sion from the donor. When an energy transfer pair of flu-
              spectrum of a fluorescent molecule in Fig. 6.      orophores is used to label two molecules that can interact
                Concentrations of the fluorescent analytes are measured  (antibody–antigen, enzyme–substrate), they can be use for
              by transmitting an excitation light through the optical fiber  sensing in fiber-optic chemical sensors.
              and measuring the light emission intensity using a detec-
              tor. A nonfluorescent analyte can be measured indirectly
                                                                  5. Raman Spectroscopy
              if its interaction with an indicator molecule changes the
              indicator emission intensity (see Section III.B).  In Raman spectroscopy, light is scattered from the
                A decrease in fluorescent intensity due to fluorescence  molecule in different directions and is shifted to both
              quenching can also be used for sensing. In this case, the  higher and lower frequencies. The shift in magnitude is
              analyte’s interaction with a fluorescent molecule causes  equal to the characteristic vibration frequencies of the
              a decrease in fluorescence (quenching). The magnitude  molecule, resulting in a unique spectrum for each mole-
              of the fluorescence decrease is related to the analyte  cule. Optical fibers are used as light guides for Raman
              concentration.                                    spectroscopy because the optimum wavelengths for the
   91   92   93   94   95   96   97   98   99   100   101