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Laser beam shaping has never been so easy!

Laser beam shaping has never been so easy!

Laser beam shaping has never been so easy!
 

Laser beam shaping has never been so easy!

 
Laser beam shaping has never been so easy!
Laser beam shaping has never been so easy! Laser beam shaping has never been so easy! Laser beam shaping has never been so easy!
 

Dr. Alexander Laskin provides an overview of AdlOptica 
				and discusses the company's beam shaping optics products.

Focal-piShaper in Photovoltaics


Finalist of 2010 Prism Awards for Photonics Innovation

Laser beam shaping has never been so easy!
Dr. Alexander Laskin provides an overview of AdlOptica at exhibition Munich 2013

Dr. Alexander Laskin provides an overview of AdlOptica GmbH

at exhibition Munich 2013

Laser beam shaping has never been so easy!

With this unique tools it is possible to convert a Gaussian laser beam into a collimated flattop (or top-hat) beam with nearly 100% efficiency.

No more losing of energy!

pi-Shaper Family - Laser beam shaping has never been so easy!
   

πShaper produces a collimated flat-top beam over a large working distance, see the Operational Principle. This enables the beam to be easily manipulated and re-sized with conventional imaging optics.

Almost the same effective sizes of input and output beams make it easy to integrate πShaper to your application.

Being originally designed as achromatic for two laser wavelength πShaper could be easily tuned to work at other laser wavelengths within wider range.

Overview

Model
Type
Input Gaussian beam, 1/e2 level
Output Flattop beam
Wavelength Range*, nm
Application based on
πShaper 6_6_Series
Telescope
6 mm
collimated
6 mm
collimated
1020-1100
Nd:YAG, Fiber and
other near IR lasers
Telescope
6 mm
collimated
6 mm
collimated
420-680
He-Ne, He-Cd and other
lasers of visual range
Telescope
6 mm
collimated
6 mm
collimated
660-1040
Ti:Sapphire laser and
other near IR lasers
Telescope
6 mm
collimated
6 mm
collimated
800-900
Ti:Sapphire laser and
other near IR lasers
Telescope
6 mm
collimated
6 mm
collimated
1200-1400
  near IR Laser Diode sources
Telescope
6 mm
collimated
6 mm
collimated
1500-1600
  near IR Laser Diode sources
Telescope
6 mm
collimated
6 mm
collimated
330-370
  3rd (355 nm) Harmonic of
Nd:YAG and similar lasers
Collimator
75 mrad
divergent
6 mm
collimated
330-370
 3rd (355 nm) Harmonic of
Nd:YAG and similar lasers

πShaper_37_34_1064

Collimator
180 mrad
divergent
34 mm
collimated
1020-1100
High Power Fiber lasers
Fiber-coupled Diode and DPSS lasers
πShaper_12_12_Series

πShaper_12_12_1064

Telescope
12.1 - 12.2 mm
collimated
12 mm
collimated
1020-1100
Nd:YAG, Fiber and
other near IR lasers

πShaper_12_12_1064_C

Collimator
58 mrad
divergent
12 mm
collimated
1020-1100
Nd:YAG, Fiber and
other near IR lasers

πShaper_12_12_TiS

Telescope
11.9 - 12.0 mm
collimated
12 mm
collimated
700-900
Ti:Sapphire laser and
other near IR lasers

πShaper_12_12_TiS_C

Collimator
60 mrad
divergent
12 mm
collimated
700-900
Ti:Sapphire laser and
other near IR lasers

πShaper_12_12_355

Telescope
12.2 mm
collimated
12 mm
collimated
330-380
3rd (355 nm) Harmonic of
Nd:YAG and similar lasers

πShaper_12_12_355C

Collimator
60.5 mrad
divergent
12 mm
collimated
330-380
3rd (355 nm) Harmonic of
Nd:YAG and similar lasers

πShaper_12_12_266

Telescope
12.2 mm
collimated
12 mm
collimated
250-270
4th (266 nm) Harmonic of
Nd:YAG and similar lasers

πShaper_12_12_266C

Collimator
60.5 mrad
divergent
12 mm
collimated
250-270
4th (266 nm) Harmonic of
Nd:YAG and similar lasers
CO2  πShaper Series
πShaper_7_7_10.6
Telescope
7 mm
collimated
7 mm
collimated
9400-11000
CO2 lasers
πShaper_12_12_10.6
Telescope
12 mm
collimated
12 mm
collimated
9400-11000
CO2 lasers
Accessories

πShaper Mount

4-axis Adjustment
       
 *   - according to coatings applied

       Trade mark
Solution for COLLIMATED beams
Basic principles of operation:

  • πShaper's are telescopic or collimator optical systems that transform Gaussian intensity distribution of source laser beam to a flattop one;
  • the development technology lets it possible to realize other output intensity profiles, systems with optical power, i.e. of objective or collimator type;
  • Achromatic design provdes this transformation for a certain wavelength range;
  • 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 an example here;
  • When changing the shape of input beam it is possible to adapt the πShaper to provide flattop output profile, this adaptation is realized through changing the diameter of source beam; an example of this adaptation is presented here.


Laser beam shaping systems.

To increase a picture
Movie picture
  Spectral correspondence:

Laser beam shaping systems.

To increase a picture


       Ideal solution for applications in:

  • Holography
  • Information processing
  • Marking and Engraving
  • Illumination
  • Particle Image Velocimetry
  • Particle Size Analyzing
  • Geochronolgy
  • Flow Cytometry
  • Free Electron Lasers
  • Mass-Spectrometry
  • Laser annealing
  • Welding of metals and plastics
  • Soldering
  • Laser Cleaning

Laser beam shaping has never been so easy! Laser beam shaping has never been so easy! Laser beam shaping has never been so easy!
   

       Copyright © 2004 - 2017

 

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Laser beam shaping has never been so easy!