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piShaper 6_6 Series High efficient laser beam shaping systems
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piShaper 5.6 6 1064 HP
piShaper 7 7 10.6
piShaper 12 12 10.6
Proved achromatic design of piShaper 6_6 systems makes them a versatile solution for applications based on lasers of NIR (near infrared) and Visual spectrum.

Applications:
  • Welding of metals and plastics
  • Flow Cytometry
  • Holography
  • Marking and Engraving
  • Printing
  • Scribing
  • Material micromachining
  • Particle Image Velocimetry
  • Particle Size Analyzing
  • Laser ablation
  • Laser annealing

Technical Specifications:

Common for all piShaper 6_6 models:
Input beam Gaussian, diameter 6 mm (1/e2)
Output beam - Collimated
- Flat-top, uniformity within 5%
- Diameter 6 mm
- High edge steepness
Type Telescope of Galilean type ( without internal focus)
Operating wavelength range* 400 - 1600 nm
Other features

- Achromatic for design wavelengths
- Compact design suitable for scientific and industrial applications
- Long working distance

Overall dimensions - Diameter 39 mm
- Length 130 mm
Weight < 250 g

piShaper 6_6 Features

Model
_1064
_VIS
_TiS
_532/1064
_410/820
_1550
Optimum wavelength range**, nm
1020-1100
420-680
660-1040
520-550, 1020-1100
400-420, 800-840
1500-1600
Design wavelengths
1064 nm (Nd:YAG),
632.8 nm (He-Ne)
442 nm (He-Cd),
632.8 nm (He-Ne)
1064 nm (Nd:YAG),
632.8 nm (He-Ne)
1064 nm (Nd:YAG),
632.8 nm (He-Ne)
442 nm (He-Cd),
632.8 nm (He-Ne)
1064 nm (Nd:YAG),
1550 nm (Laser Diode)
Mounting
M 27x1
M 22x0.5, M 25x1
M 27x1
M 27x1
M 27x1
M 27x1
Applications based on
Nd:YAG, Fiber and other
near IR-lasers
He-Ne, He-Cd and other
lasers of visual range
Ti:Sapphire laser and
other near IR lasers
1st (1064) and 2nd (532)
Harmonics of Nd:YAG laser
1st (820) and 2nd (410)
Harmonics of Ti:Sapphire
near IR Laser
Diode sources
  * - working wavelength range without taking into consideration the coatings
** - according to coatings applied

 -  piShaper_6_6_leaflet


Basic principles of piShaper operation:

  • piShaper is a telescopic optical systems that transforms Gaussian intensity distribution of source laser beam to a flattop one;
  • This transformation is provided for a certain wavelength range, thus piShaper is achromatic system;
  • Galilean design, thus there are no intermediate focusing of a beam;
  • With changing the size of input beam the output beam profile changes as well, see description here;
  • When changing the shape of input beam it is possible to adapt the piShaper to provide flattop output profile, this adaptation is realized through changing the diameter of source beam; description of this adaptation is presented here.

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Drawing:

ENLARGE