Page 176 - High Power Laser Handbook
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144   Diode Lasers                          High-Power Diode Laser Arrays     145


                      bar metallization, bonding, and heat sink design have cumulatively
                      contributed to long-term reliability.
                         Diode laser bars operating in QCW mode routinely have lifetimes
                      of greater than 1 Gigapulses at peak powers of 200 W or higher. Long-
                      term reliability of a laser diode bar is a function of three primary fac-
                      tors: (1) operating temperature, (2) operating power, and (3) operating
                      current density. For example, a 50-W, 808-nm CW laser bar mounted
                      on a passively cooled heat sink operating at 25°C will last twice as
                      long as the same bar operating at 35°C. If the same bar is operated at
                      60 W instead of 50 W (i.e., the same heat sink operating temperature),
                      then the junction temperature at the laser bar solder interface will rise
                      by approximately 5 to 7°C above the 50 W operation junction tem-
                      perature, which will reduce its lifetime. Furthermore, at 60-W opera-
                      tion, the current density is also higher, which accelerates aging of the
                      bulk semiconductor material.
                         However, advances in the use of aluminum-free active regions
                      and the increase of characteristic temperatures T and T  have allowed
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                      the diode laser bar to operate at higher junction temperatures  with-
                      out  compromising  efficiency. Advancements  in  antireflection  (AR)
                      coatings and facet passivation have increased the catastrophic optical
                      mirror  damage  (COMD)  threshold  of  emitters,  which  has  allowed
                      higher power per emitter in both CW and QCW modes of operation.
                      The use of hard solder, such as AuSn, and of coefficient of thermal
                      expansion (CTE)–matched heat sinks with lower thermal impedance
                      has allowed the diode bar to operate reliably at higher powers.



                 6.6  Product Performance
                      Without first collimating the beam with a cylindrical lens, the large
                      beam divergence (> 40°) perpendicular to the p-n junction (i.e., the
                      fast-axis  direction)  allows  only  a  limited  number  of  applications.
                      Side pumping of solid-state laser crystals, in which the diodes can
                      be placed in very close proximity to the laser crystal, is one of those
                      rare cases where the divergence is of benefit for uniform illumination
                      of the crystal. The divergence in the lateral direction of a diode laser
                      bar typically depends on the drive current or the current density, as
                      the beam is first gain guided and to some extent index guided by the
                      established temperature profile at higher output powers. The lateral
                      divergence takes on values of between 4 and 10 degrees. These values
                      for the divergence in both directions, as well as the dimensions of the
                      emitting  area,  result  in  an  astigmatic  beam.  The  beam  parameter
                                                                    2
                      product (full angle × diameter) is about 2 mm-mrad (M  about 1.3) in
                                                                  2
                      the fast-axis direction and up to 1700 mm-mrad (M  about 1000) in
                      the slow-axis direction, which is too large for most applications. The
                      beam quality in the slow-axis direction can be further improved by
                      using an array of cylindrical lenses to collimate the individual emitters
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