- πShaper 6_6 Series
- πShaper 12_12 Series
- πShaper NA 0.1/0.2
- πShaper NA 0.1/0.2_12
- πShaper for IR Lasers
- πShaper NA0.055_34_1070
πShaper 6_6 Series
Highly efficient Beam Shapers
transforming Gaussian to Flat-top profile
for all laser wavelengths: UV, visible, near- and mid-IR
Applications:
- Microscopy
- Confocal microscopes
- Holography
- Interferometry
- MOPA lasers
- Free Electron Lasers (FEL)
- Illumination of Spatial Light Modulators (SLM)
- Micromachining
- Particle Image Velocimetry (PIV)
- Laser ablation
- Welding
- Marking
Technical Specifications
| Common for πShaper 6_6 models | ||||
| Type | Field mapping beam shaper as a telescope of Galilean type, without internal focus | |||
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| Output beam |
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| Other features |
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| Overall dimensions |
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| Mounting | M27x1 thread, at entrance and exit | |||
| Weight | <300 g | |||
| πShaper 6_6 features | ||||
| Model | Input 1/e² Diameter, mm | Output FWHM Diameter, mm | Optimum spectrum*, nm | Applications based on lasers |
| _NIR | 5.9 - 6.0 | 6.0 | 1100 - 1700 | near-IR |
| _VIS | 5.9 - 6.0 | 6.0 | 405 - 680 | He-Ne, He-Cd, lasers of visible band |
| _NUV | 5.9 - 6.0 | 6.0 | 335 - 560 |
2nd (532), 3rd (355) Harmonics of Nd:YAG, UV and Violet |
| _1.9-2.8 | 6.1 - 6.2 | 6.4 | 1900 - 2800 | mid-IR |
| _2.05 | 6.4 - 6.5 | 6.4 | 1900 - 2160 | mid-IR |
| _1550 | 6.4 - 6.5 | 6.2 | 1500 - 1600 | near-IR |
| _1064 | 6.4 - 6.5 | 6.1 | 1020 - 1100 | Nd:YAG, Fiber and other near-IR |
| _TiS | 6.4 - 6.5 | 6.0 | 700 - 900 | Ti:sapphire, near-IR |
| _532 | 6.3 - 6.4 | 5.8 | 510 - 550 | 2nd Harmonics of Nd:YAG, similar lasers |
| _350 | 6.3 - 6.4 | 5.6 | 330 - 380 | 3rd (355) Harmonics of Nd:YAG lasers |
| _325 | 6.3 - 6.4 | 5.6 | 305 - 345 | He-Cd, UV |
| _266 | 6.3 - 6.4 | 5.2 | 250 - 275 | 4th (266) Harmonics of Nd:YAG lasers |
| * - according to AR-coatings applied | ||||
| πShaper 6_6_350_C features | |
| Type | Collimator without internal focus |
| Input beam |
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| Output beam |
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| Other features |
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| Overall dimensions |
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| Optimum | 330 - 380 nm |
| Design wavelengths | 350 nm |
| Applications based on | 3rd (355) Harmonics of Nd:YAG laser |
| Mounting | M 27x1 |
| Weight | 250 g |
Basic principles of πShaper operation:
- πShaper transforms Gaussian or similar intensity distribution of source laser beam to a flat-top one;
- TEM00 or multimode with Gaussian or similar intensity profile can be applied;
- Achromatic design provdes this transformation for a certain wavelength range;
- Galilean design, thus there are no intermediate focusing of a beam;
- There are two versions of some πShaper 6_6 systems: Telescope and Collimator, please, look at above descriptions;
- 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 πShaper to provide flat-top output profile, this adaptation is realized through changing the diameter of source beam; description of this adaptation is presented here.
πShaper 12_12 Series
High efficient laser beam shaping systems for UV, Visual and NIR
Most important specific needs of applications based on the UV-lasers as well as Short-pulse Ti:Sapphire
lasers are taken into account while developing the πShaper 12_12 systems.
Applications:
Applications:
- Free Electron Lasers
- Fluorescence Technologies
- Flying Plate Technique
- Display Making Technologies
- Mass-Spectrometry
- Ultrashort Pulse Laser Pumping
- MOPA Techniques
- Material processing
Technical Specifications
| Common for all πShaper 12_12 models | |||||
| Input beam | TEM00 or multimode with Gaussian or similar intensity profile | ||||
| Output beam |
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| Other features |
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| Mounting |
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| πShaper 12_12 features | |||||
| Model* | Input 1/e² Ø, mm | Output FWHM Ø, mm | Optimum spectrum, nm | Dimensions D / L, mm |
Applications based on |
| _2.05_HP | collimated Ø 12.0 - 12.1 |
12.1 | 1900 - 2160 | 42 / 358 | mid‐IR Lasers |
| _1550_HP | collimated Ø 12.0 - 12.1 |
12.2 | 1500 - 1600 | 42 / 358 | near‐IR Lasers |
| _1064_HP | collimated Ø 12.0 - 12.1 |
12.0 | 1020 - 1100 | 42 / 358 | Nd:YAG, Fiber lasers, Other NIR Lasers |
| _1064_HP_W | collimated Ø 12.0 - 12.1 |
12.0 | 49 / 360 | High-Power USP lasers Water cooled system |
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| _TiS_HP | collimated Ø 12.0 - 12.1 |
12.0 | 700 - 900 | 42 / 358 | Ti:Sapphire lasers, Other NIR Lasers |
| _532 | collimated Ø 12.8 - 13.0 |
11.8 | 515 - 550 | 49 / 270 | 2nd Harmonic Nd:YAG, Visible Lasers |
| _532_HP | collimated Ø 12.0 - 12.1 |
11.8 | 42 / 358 | ||
| _355_HP | collimated Ø 12.0 - 12.1 |
11.3 | 330 - 380 | 42 / 358 | 3rd Harmonic Nd:YAG, UV Lasers |
| _325 | collimated Ø 12.7 - 12.9 |
11.4 | 305 - 345 | 49 / 270 | UV Lasers |
| _266 | collimated Ø 12.6 - 12.8 |
10.6 | 250 - 270 | 42 / 285 | 4th Harmonic Nd:YAG, UV Lasers |
| _266_HP | collimated Ø 12.0 - 12.1 |
10.6 | 42 / 358 | ||
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* - Basic models are Telescopes of Galilean type (without internal focus), Models with index _HP are versions for high peak power lasers. |
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Basic principles of πShaper_12_12 operation:
- πShaper transforms Gaussian or similar intensity distribution of source laser beam to a flat-top one;
- TEM00 or multimode with Gaussian or similar intensity profile can be applied;
- 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;
- When changing the shape of input beam it is possible to adapt the πShaper to provide flat-top output profile, this adaptation is realized through changing the diameter of the input beam;
- Versions of the πShaper 12_12 for other wavelengths ranges are, also, available.
πShaper NA 0.1 / 0.2
Refractive beam shaping optics for multimode fiber-coupled high-power solid-state and diode lasers
πShaper NA 0.1 / 0.2
- combines collimating and focusing optics,
- is optimized to operate with multimode high power fiber-coupled diode lasers in 910-980 nm and solid state-lasers in 1050-1080 nm spectral bands,
- to be connected directly to fiber,
- converts with near 100% efficiency a divergent Gaussian-like beam into a beam with Donut or Flat-top intensity profile,
- provides round or linear spots depending on optical design.
- Welding
- Cladding
- Brazing
- Hardening
- Technologies where Flat-top or Donut spot required
Technical Specifications
| Type | Combined Collimator+Focusing Lens, without internal focus, to be connected to multimode fiber | |
| Input beam |
- multimode with Gaussian-like intensity profile - Divergent |
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| Output beam |
- convergent - divergence 2Θ = 0.04 - 0.07 rad |
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| Working distance | 200 - 350 mm depending on spot size and intensity profile | |
| Resulting spot |
- donut or flat-top intensity distribution depending on working plane - round spot - diameter in range 4 - 12 mm depending on working plane - linear spot - length in range 6 - 12 mm depending on working plane |
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| Laser power | Up to 6 kW (CW) | |
| Other features |
- Water cooling - Other wavelengths on request - Extended depth of field |
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| Overall dimensions |
- Diameter 100 mm - Length 250 - 300 mm, depending on configuration for round or linear spot |
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| Weight | < 3 kg | |
| πShaper NA 0.1 / 0.2 features | ||
| Model | πShaper NA0.2_910-980 | πShaper NA0.1_1064 |
| Multimode fiber |
- NA0.22 - fiber core diameter 100 - 1000 μm - beam divergence 2Θ = 0.38 - 0.4 rad (1/e²) |
- NA0.13 - fiber core diameter 50 - 400 μm - beam divergence 2Θ = 0.15 - 0.18 rad (1/e²) |
| Operating spectral band, nm | 910 - 980 | 1050 - 1080 |
| Applications based on | fiber-coupled diode lasers | fiber and fiber-coupled solid-state lasers |
πShaper NA 0.1_12 and πShaper NA 0.2_12
Series of high efficient collimating Beam Shapers for fiber coupled DPSS and diode lasers, fiber lasers divergent Gaussian to collimated Flat-top beam
These unique tools convert divergent Gaussian laser beams,
TEM00 and multimode,
into collimated Flat-top, super-Gauss or inverse-Gauss beams with nearly 100% efficiency.
Combining of functions in one device: collimating and
beam shaping.
πShaper produces low divergent collimated Flat-top beam
(like Greek letter pi), therefore the resulting profile is kept stable over large working distance,
and it is easy to manipulate and re-size the beam with conventional imaging optics,
and create Round and Linear spots of necessary size.
Optimized to operate with powerful (> 0,5 kW) fiber lasers, fiber coupled DPSS or Diode lasers.
Compatibility with standard industrial fiber connectors is provided.
Applications:
- Welding
- Hardening
- Cladding
- Laser pumping
- Display Making Technologies
- other techniques of Material Processing
Technical Specifications
| Common for πShaper NA 0.1_12 / NA 0.2_12 models | |||||
| Input beam |
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| Features | |||||
| Model | Input 1/e² Ø, mm | Output FWHM Ø, mm | Optimum spectrum, nm | Dimensions D / L, mm |
Comments |
| NA 0.1_12_780 | 0.1 - 0.11 | 12.0 | 750 - 820 | 49 or 63* / 295* | Fiber coupled Diode lasers, TEM00 and multimode |
| NA 0.1_12_1064 | 12.2 | 1020 - 1100 | Fiber lasers, fiber coupled DPSS lasers |
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| NA 0.1_12_1550 | 12.4 | 1500 - 1600 | Fiber and Diode lasers |
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| NA 0.1_12_325 | 0.122 | 10.8 | 300 - 355 | 49 / 270 | UV lasers |
| NA 0.2_12_808 | 0.18 - 0.2 | 12.3 | 780 - 840 | 49 / 315** |
Fiber coupled Diode lasers, TEM00 and multimode |
| NA 0.2_12_970 | 930 - 1020 | ||||
| NA 0.2_12_1064 | 1020 - 1100 | Fiber lasers, fiber coupled DPSS lasers |
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* - with collimator compatible with QBH ** - with collimator compatible with FC/PC |
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πShaper NA 0.1_12_1064 connected to fiber laser with QBH connector
IR πShaper Series
πShaper Series of high efficient laser beam shaping systems for IR lasers
Developed for applications based on carbon dioxide (CO2) lasers this beam shaping system opens new opprtunities to improve the technologies of material processing.
Applications:- Welding of metals and plastics
- Marking and Engraving
- Printing
- Material micromachining
- Material processing
- Cutting
- Cladding
Technical Specifications
| Type | Telescope of Galilean type ( without internal focus) | |||||
| Input beam | - Collimated - TEM00 or multimode with Gaussian or similar intensity profile |
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| Output beam | - Collimated - Flat-top, uniformity within 5% - High edge steepness |
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| Other features | - Compact design suitable for scientific and industrial applications - Materials of lenses ZnSe - Extended working distance - Option of water cooling |
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| Applications based on | CO2, CO, Quantum Cascade lasers, other MWIR or LWIR lasers | |||||
| Features | ||||||
| Model | Input 1/e² Ø, mm | Output FWHM Ø, mm | Mounting | Dimensions D / L, mm |
Optimum spectrum, nm | |
| πShaper 7_7 | ||||||
| _10.6 | 7.0 | 7.0 | M27x1 | 39 / 135 | 10000 - 11000 | |
| _9.4 | 9000 - 10000 | |||||
| πShaper 12_12 | ||||||
| _10.6 | 12.0 | 12.0 | Input: M27x1 Output: M33x1 Adaptor M33x1 -> M27x1 |
49 / 360 | 10000 - 11000 | |
| _9.4 | 49 / 271 | 9000 - 10000 | ||||
| _5.1 | 5000 - 5500 | |||||
Basic principles of πShaper operation:
- πShaper transforms Gaussian or similar intensity distribution of source laser beam to a flat-top one;
- TEM00 or multimode with Gaussian or similar intensity profile can be applied;
- 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 πShaper to provide flat-top output profile, this adaptation is realized through changing the diameter of source beam; description of this adaptation is presented here.
Operation principle on example of πShaper 7_7_10.6
πShaper NA0.055_34_1070
Highly efficient Beam Shapers transforming divergent Gaussian to collimated Flat-top beam
With these unique devices it is possible to convert a divergent TEM00 or multimode laser beam from a fiber laser
into a collimated Flat-top beam with nearly 100% efficiency and conserving flatness of the wavefront.
πShaper produces a collimated Flat-top beam over large working distance.
This enables manipulating and re-sizing the Flat-top output beam using conventional imaging optics.
High transmission and reduced thermally induced optical effects such as focus shift.
Applications:
- Hardening
- Welding
- Cladding
- Applications based on high-power fiber lasers and getting benefits from flat-top, super-Gauss and inverse-Gauss beams
Specifications
| Description | Collimating refractive beam shaper without internal focusing, transforming a divergent Gaussian-like beam from a single mode or multimode fiber coupled laser or fiber laser into a flat-top collimated beam. |
| Input beam |
- Divergent - TEM00 or multimode - With Gaussian-like intensity profile - Divergence: - maximum full beam angle 0.14 rad - optimum 1/e² full angle 0.11 rad (half angle 0.055 rad) - minimum 1/e² full angle 0.08 rad |
| Output beam |
- Collimated - Flat-top, uniformity within 5% when optimum input divergence - FWHM diameter 34 mm - Variable divergence full angle ±2mrad, for correction purpose |
| Output clear aperture | 37 mm |
| Spectral bands | 1020 - 1100 nm, 640 - 700 nm |
| AR-coatings | W-type, minimums @ 1070 nm, 670 nm |
| Transmission @ 1070 nm | >98% @ 1070 nm |
| Features of mechanical design |
- Fiber connection: rotatable QB Fiber connector mount - 4-axis Fiber End alignment - Variable FEP along the optical axis ±20 mm, for correction of output divergence - Variable distance between components, for correction of output profile - Compatibility with previous designs |
| Water cooling |
- Coating of water cooling channel: Al oxide - Maximum water pressure 5 bar - Water cooling fittings 6-1/8 - Hose Ø: inner 4 mm, outer 6 mm - Deionised / distilled water |
| Mounting | By cylinder surface Ø73.5 and 4 mounting holes Ø5.4, 62x62 |
| Overall dimensions |
- Diameter 90 mm (without fittings) - Length 627.2 ±20 mm (with QB fiber connector mount) |
| Operating and storage environment |
- Humidity less than 80% - Temperature 15°C - 27°C - Proper alignment of a laser source by operation |
| Weight | < 5 kg |
