Small Spot Size at long distance

                  
     Large Collimated Output


DBX Expander Laser Modules
  • Compact length ~160mm 
  • Large output beam size 47mm diameter
  • Low beam diveregce < 0.05mrad
  • Wavelengths 532 - 1064nm
  • Standard Powers 1mW - 50mW
  • M4(metric) and 8-32(imperial) mounting holes on base
  • Simply change input lens to change output beam size 
  • Variable focus from 1m to infinity
  • 3 element AR coated lens system
  • Electrically isolated    

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    Contact Us now at expanderlaser@dioptika.com with your requirements     
                                                                    
    Part Number Wavelenth(nm) Power(mW) Output Beam Size(mm) Length(mm) Divergence

    DBXL-20-532-5

    532

    5.0

    47mm

    163mm

    0.05mrad

    DBXL-20-532-15

    532

    15.0

    47mm

    163mm

    0.05mrad

    DBXL-20-635-1

    635

    1.0

    47mm

    163mm

    0.05mrad

    DBXL-20-635-5

    635

    5.0

    47mm

    163mm

    0.05mrad

    DBXL-20-635-25

    635

    25.0

    47mm

    163mm

    0.05mrad

    DBXL-20-658-35

    658

    35.0

    47mm

    163mm

    0.05mrad

    DBXL-20-830-10

    830

    10.0

    47mm

    163mm

    0.05mrad



     

     

     


    Part Number:  DBX - Base
    The mounting base fits securely to the bottom of the beam expander and provides a flat base with a combination of M4 and 8-32 mounting holes.



    Laser Beam Expanders 
                                    
                                                 

                                        















      Laser beam expanders are designed to either decrease the laser's beam spot size at large distances or produce
      a larger diameter collimated laser beam. The main types of beam expanders: Keplerian and Galilean. In its
      simplest form, the Galilean type consists of a positive and a negative focal length lens whereas the Keplerian
      type consists of two positive focal length lenses. Both designs provide a certain angular magnification, called
      the Expander Power. The beam diameter is first increased in size by this power and then the beam divergence is
      reduced by the same power. This combination yields a beam that is not only larger, but one that is also highly
      collimated. The result is a smaller beam at a large distance when compared to the laser alone.  See the below
      equation:

      BL

      =

      ß + ØL (0.3048)

      BL

      =

      Beam Diameter (mm) at distance L

      ß

      =

      Increase in Beam Diameter

      =

      Beam Diameter (mm) x Expander Power

      Ø

      =

      Decrease in Beam Divergence

      =

      Beam Divergence (mrad) Expander Power

      L

      =

      distance (ft.)

      This equation is an approximation for the collimated output beam size at a given distance.

      In addition, an expanded beam can yield smaller spot sizes when used in combination with additional focusing
      optics. This is very useful in focusing optimization. however, many applications simply require a larger continuous
      beam.
      The beam expander power (MP) is equal to the ratio of the effective focal length (EFL) of the objective lens
      to the effective focal length of the entrance optic. The physical separation between the objective lens and entrance
      optic is equal to the sum of their back focal lengths (BFL).

      DiOptika’s  beam expanders are of the Galilean type. The advantages of the Galilean design over the Keplerian is
      that it contains no internal focal point therefore reducing the length.  In addition to improving beam collimation,
      DiOptika’s beam expanders can also be used to focus laser beams.




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