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              Optical Fiber Techniques for Medical Applications                                           319

              there were defects in the materials and at the interface.  well only in the spectral range λ> 450 nm, and their laser
              Nowadays, exceptionally pure materials are prepared by  power handling is limited.
              deposition in a vacuum system, and special efforts are
              taken to reduce the number of defects. In the case of  III. LASERS FOR FIBEROPTIC
              optical communications, the fibers are coated with a plas-  MEDICAL SYSTEMS
              ticprimarycoatingastheyarebeingdrawn,inordertopro-
              tect them from moisture or scratches, among other things.
                                                                A. Medical Lasers
              Good-quality optical fibers have transmission losses on
              the order of 1 dB/km. Such quality is normally not needed  There are many regular light sources that are used in
              for medical applications.                         medicine, such as incandescent lamps (e.g., halogen),
                In optics, wavelength λ is normally specified in nano-  high-pressure lamps (e.g., Xe), and light-emitting diodes
                             −9
              meters (1 nm = 10 m), or in micrometers (1 µm =   (i.e., LEDs ). The light emitted from these sources consists
              10 −6  m). The optical spectrum is broadly divided into  of many wavelengths; it is emitted from a relatively broad
              three spectral regions: ultraviolet (UV) for λ< 400 nm,  area, and is spread in many directions. Laser light has
              visible (VIS) λ = 400–700 nm, and infrared (lR) for  characteristics that make it especially useful in medicine.
              λ> 700 nm. The UV region at wavelengths λ< 250    These are:
              nm is sometimes called “deep UV.” The infrared spec-
              trum may be further divided to near infrared (NIR) λ =     Monochromatic—laser light consists of a narrow band
              0.7–3.0 µm and middle infrared (MIR) λ = 3.0–30 µm.  of wavelengths (i.e., “one wavelength”).
              Optical fibers that are based on some mixture of SiO 2 ,     Collimated beam—the laser light is emitted in a
              B 2 O 3 , and Na 2 O, are called silica fibers and they transmit  parallel beam.
              well in the UV, visible, and NIR regions of the optical     High intensity—practically all the laser energy is
              spectra.                                           concentrated in a narrow pencil.
                                                                 Coherent—the laser emission is “ordered” both in

                                                                 space and in time.
                2. Special Optical Fibers
              Standard silica fibers transmit only in the visible and do  The coherence helps to focus the beam to a very small
              not transmit in the deep UV or in the middle infrared. Nor  point (of the order of the wavelength of light). The en-
              could these glass fibers transmit visible or NIR beams  ergy density (energy divided by area) at the focal spot is
              of high intensity. For the transmission of deep UV, one  extremely high. Such energy density cannot be obtained
              could use pure silica as the core material. Doped silica  with standard (noncoherent) light sources.
              (of lower index of refraction) serves as a cladding layer.  All lasers are based on some active medium in which
              These fibers (sometime called “quartz”fibers) also serve  “optical amplification” occurs. This medium can be a solid
              as power fibers for the transmission of laser power. For  crystal (e.g., Nd:YAG or Er:YAG crystals), a liquid (e.g.,
              transmission in the middle infrared, one may use nonox-  dye in a solution), gas (e.g., Ar, CO 2 , or HeNe), or a semi-
              ide glasses such as chalcogenides (e.g., As 2 S 3 )or fluo-  conductor (e.g., GaAs). The medium has to be excited
              rides (e.g., ZrF 4 –BaF 2 –LaF 3 ). Crystals of silver halides  (pumped) in order to start the lasing process, and elec-
              or thallium halide can be extruded through dies. The re-  tric current often provides excitation. Also, in order to get
              sulting fibers were found to be transparent in the middle  laser emission the laser should contain two mirrors, which
              infrared. An alternative is to use hollow plastic or glass  reflect the light back and forth through the lasing medium.
              tubes, coated on the inside with thin metallic coatings.  One of these mirrors is partially transparent, and the laser
              The hollow tubes are transparent in the mid IR and can  beam emerges from this mirror.
              deliver high laser power. These are not actually fibers, but  There are many lasers that emit light in the UV, visi-
              they are thin and fairly flexible and are sometimes referred  ble, and IR. Some lasers emit continuously light of wave-
              to as hollow fibers.                               length λ, and the total power emitted is measured in
                Optical fibers made of plastic materials have been  watts. These are called CW (continuous wave) lasers.
              used in the past for the visible range. For example, poly-  Other lasers emit short bursts of light, in which case the
              methylmethacrylate (PMMA) could be drawn to form  lasers are called pulsed lasers. Some of the lasers used in
              unclad fibers. Alternatively, polystyrene may serve as a  medicine emit long pulses, measured in msec (10 −3  sec),
              core in these fibers, and PMMA as cladding. Such fibers  others emit shorter pulses, measured in µsec (10 −6  sec)
              are flexible and less expensive to fabricate, but their  or nsec(10 −9  sec), and some emit very short pulses, mea-
              properties are still inferior to those of glass. In particular,  sured in psec (10 −12  sec) or fsec (10 −15  sec). The energy
              plastic fibers are relatively thick (1 mm), they transmit  emitted from these lasers can be specified by the pulse
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