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4-6                                                              MEMS: Design and Fabrication


                TABLE 4.2 SOR Applications

                Application area                                   Instruments/technologies needed
                Structural analysis
                Atoms                               Photoelectron spectrometers
                Molecules                           Absorption spectrometers
                Very large molecules                Fluorescent spectrometers
                Proteins                            Diffraction cameras
                Cells                               Scanning electron microscope (to view topographical radiographs)
                Crystals                            Time resolved X-ray diffractometers
                Polycrystals
                Chemical analysis
                Trace                               Photoelectron spectrometers
                Surface                             (Secondary ion) mass spectrometer
                Bulk                                Absorption/fluorescence spectrometers
                                                    Vacuum systems
                Microscopy
                Photoelectron                       Photoemission microscopes
                X-ray                               X-ray microscopes SEM (for viewing)
                                                    Vacuum systems
                Micro/nanofabrication
                X-ray lithography                   Steppers, mask making
                Photochemical deposition of thin films  Vacuum systems
                Etching                             LIGA process
                Medical diagnostics
                Radiography                         X-ray cameras and equipment
                Angiography and tomography          Computer aided display
                Photochemical reactions
                Preparation of novel materials      Vacuum systems
                                                    Gas-handling equipment
                Source: Adapted with permission from Nippon Telegraph and Telephone Corporation (NNT), 1991.


             walls further differentiates LIGA exposure stations. All these factors make exploring LIGA a challenge.
             However, given sufficient research and development money, large markets are likely to emerge over the
             next five to ten years. These markets could be in the manufacture of devices with stringent requirements
             imposed on resolution, aspect ratio, structural height, and parallelism of structural walls. Optical appli-
             cations for the information technology (IT) field seem particularly attractive early product targets.
               So far, it is the research community that has primarily benefited from the availability of SOR photon
             sources. With its continuously tunable radiation across a very wide photon range, highly polarized and
             directed into a narrow beam, SOR provides a powerful probe of atomic and molecular resonances. Other
             types of photon sources prove unsatisfactory for these applications in terms of intensity or energy spread.
             As can be concluded from Table 4.2, applications of SOR beyond lithography range from structural and
             chemical analysis to microscopy, angiography, and even to the preparation of new materials.

             4.2.2.2 Technical Aspects
             Some important concepts associated with synchrotron radiation (such as the bending radius of the syn-
             chrotron magnet, magnetic field strength, beam current, critical wavelength, and total radiated power)
             require introduction. Figure 4.4 presents a schematic of an X-ray exposure station. Electrons are injected
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             into the ring, where they are maintained at energies anywhere from 10 to 10 eV. The cone of radiation
             shown in this figure is the electromagnetic radiation emitted by the circling electrons due to the radial
             acceleration that keeps them in the orbit of the electron synchrotron or storage ring. For high-energy par-
             ticle studies, this radiation, emitted tangential to the circular electron path (Bremsstrahlung), limits the
             maximum energy the electrons can attain. Bremsstrahlung is a nuisance for studies of the composition of
             the  atomic  nucleus  in  which  high-energy  particles  are  smashed  into  the  nucleus. To  minimize  the



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