AdlOptica社はマルチフォーカスおよびレーザービーム成形光学の分野で活躍しているメーカーです。UVからIRまでのスペクトル、mWからkWまでの出力、CWまたはパルスレーザー、アクロマティックデザインなど、様々なアプリケーションに対応しております。
AdlOptica πシェイパー12_12
πシェイパー12_12 高効率レーザービームシェイパー UV,可視,NIRレーザー用
π Shaper 12_12 高効率レーザービーム ビームシェイピング UV, 可視, NIR レーザー用 紫外、可視、近赤外
・自由電子レーザー
・蛍光技術
・フライング プレート法
・ディスプレイを作る技術
・質量分析
・超短パルス レーザー励起
・MOPAテクニック
・材料加工
| Technical Specifications: | ||||||||||||||||||||||||||||||||||||||||||||||
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Features
|
Model*
|
Input beam
all values at 1/e2 |
Output beam
Diameter, mm (FWHM) |
Spectral
range, nm |
Overall dimensions, mm
|
Weight, g
|
Applications
based on |
|
|
Diameter
|
Length
|
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|
_1064
|
– collimated – Dia 12.8 – 13.0 mm |
12.4
|
1020 – 1100
|
49
|
270
|
530
|
Nd:YAG, Fiber lasers, Other NIR Lasers |
|
_1064_HP
|
– collimated – Dia 12.0 – 12.1 mm |
12.0
|
42
|
328
|
530
|
||
|
_1064_C
|
– divergent – Divergence 58 mrad |
12.0
|
42
|
285
|
480
|
||
|
_TiS_HP
|
– collimated – Dia 12.0 – 12.1 mm |
12.0
|
700 – 900
|
42
|
328
|
530
|
Ti:Sapphire lasers, Other NIR Lasers |
|
_532
|
– collimated – Dia 12.8 – 13.0 mm |
12.0
|
515 – 550
|
49
|
270
|
530
|
2nd Harmonic Nd:YAG, Lasers of Visual range |
|
_532_HP
|
– collimated – Dia 12.0 – 12.1 mm |
11.8
|
42
|
328
|
530
|
||
|
_355_HP
|
– collimated – Dia 12.0 – 12.1 mm |
11.3
|
330 – 380
|
42
|
328
|
530
|
3rd Harmonic Nd:YAG, Lasers of UV-range |
|
_266
|
– collimated – Dia 12.6 – 12.8 mm |
10.6
|
250 – 270
|
49
|
270
|
530
|
4th Harmonic Nd:YAG, Lasers of UV-range |
|
_266_HP
|
– collimated – Dia 12.0 – 12.1 mm |
10.6
|
42
|
328
|
530
|
||
|
_266_C
|
– divergent – Divergence 60 mrad |
12.0
|
42
|
285
|
480
|
||
|
* – Basic models are Telescopes of Galilean type (without internal focus),
Models with index _HP are versions for high peak power lasers, Models with index _C are Collimators without internal focus. |
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Basic principles of πShaper 12 12 operation:
πShaper transforms Gaussian or similar intensity distribution of source laser beam to a flattop 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 the πShaper 12_12 systems: Telescope and Collimator, please, look at the descriptions below;
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 flattop output profile, this adaptation is realized through changing the diameter of source beam;
Versions of the πShaper 12_12 for other wavelengths ranges are, also, available.
πShaper 12_12_266_C コリメーター バージョン
拡散ビーム入力 平行ビーム出力
