Variable Attenuators for Linearly Polarized Laser Beam 990-0070
• Divides laser beam into two parallel beams of manually adjustable intensity ratio • Large dynamic range • Transmitted beam shift ~0.5 mm • High optical damage threshold • S-Pol attenuation range ~ 0.25% - 99.0% •… Read more →
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| SKU | Wavelength · Laser Damage Threshold · Group | |
|---|---|---|
| 990-0070-1030 | 1030 nm·> 10 mJ/cm², 50 fs pulse, 800 nm·For Femtosecond Applications |
2 in stock
Ships in: 2–5 calendar days
$900
|
| 990-0070-1030B | 1010-1050 nm·10 mJ/cm² @ 800 nm, 50 fs·For Femtosecond Applications |
1 in stock
Ships in: 2–5 calendar days
$1,075
|
| 990-0070-1030H | 1030 nm·> 100 mJ/cm², 50 fs pulse, 800 nm·For High Power Femtosecond Laser Applications |
Out of stock
$988
|
| 990-0070-1030HB | 1010-1050 nmn·> 100 mJ/cm², 50 fs pulse, 800 nm·For High Power Femtosecond Laser Applications |
1 in stock
Ships in: 2–5 calendar days
$1,163
|
| 990-0070-1064 | 1064 nm·For Nd:YAG Laser Application |
1 in stock
Ships in: 2–5 calendar days
$795
|
| 990-0070-257 | 257 nm·10 mJ/cm² @ 800 nm, 50 fs·For Femtosecond Applications |
1 in stock
Ships in: 2–5 calendar days
$1,139
|
| 990-0070-257H | 257 nm·100 mJ/cm² @ 800 nm, 50 fs·For High Power Femtosecond Laser Applications |
1 in stock
Ships in: 2–5 calendar days
$1,227
|
| 990-0070-266 | 266 nm·10 mJ/cm² @ 800 nm, 50 fs·For Femtosecond Applications |
1 in stock
Ships in: 2–5 calendar days
$1,139
|
| 990-0070-266H | 266 nm·> 100 mJ/cm², 50 fs pulse, 800 nm·For High Power Femtosecond Laser Applications |
Out of stock
$1,227
|
| 990-0070-343 | 343 nm·> 10 mJ/cm², 50 fs pulse, 800 nm·For Femtosecond Applications |
Out of stock
$1,017
|
| 990-0070-343H | 343 nm·> 100 mJ/cm², 50 fs pulse, 800 nm·For High Power Femtosecond Laser Applications |
Out of stock
$1,104
|
| 990-0070-355 | 355 nm·5 J/cm² @ 1064 nm, 10 ns, 10 Hz·For Nd:YAG Laser Application |
1 in stock
Ships in: 2–5 calendar days
$912
|
| 990-0070-400 | 400 nm·> 10 mJ/cm², 50 fs pulse, 800 nm·For Femtosecond Applications |
Out of stock
$900
|
| 990-0070-400B | 390-410 nm·> 10 mJ/cm², 50 fs pulse, 800 nm·For Femtosecond Applications |
Out of stock
$1,075
|
| 990-0070-400H | 400 nm·> 100 mJ/cm², 50 fs pulse, 800 nm·For High Power Femtosecond Laser Applications |
Out of stock
$999
|
| 990-0070-400HB | 390-410 nm·> 100 mJ/cm², 50 fs pulse, 800 nm·For High Power Femtosecond Laser Applications |
1 in stock
Ships in: 2–5 calendar days
$1,163
|
| 990-0070-515 | 515 nm·> 10 mJ/cm², 50 fs pulse, 800 nm·For Femtosecond Applications |
Out of stock
$900
|
| 990-0070-515B | 505-525 nm·> 10 mJ/cm², 50 fs pulse, 800 nm·For Femtosecond Applications |
Out of stock
$1,075
|
| 990-0070-515H | 515 nm·> 100 mJ/cm², 50 fs pulse, 800 nm·For High Power Femtosecond Laser Applications |
Out of stock
$988
|
| 990-0070-515HB | 505-525·> 100 mJ/cm², 50 fs pulse, 800 nm·For High Power Femtosecond Laser Applications |
Out of stock
$1,163
|
| 990-0070-532 | 532 nm·5 J/cm² @ 1064 nm, 10 ns, 10 Hz·For Nd:YAG Laser Application |
1 in stock
Ships in: 2–5 calendar days
$795
|
| 990-0070-800 | 800 nm·> 10 mJ/cm², 50 fs pulse, 800 nm·For Femtosecond Applications |
Out of stock
$900
|
| 990-0070-800B | 780-820 nm·10 mJ/cm² @ 800 nm, 50 fs·For Femtosecond Applications |
1 in stock
Ships in: 2–5 calendar days
$1,075
|
| 990-0070-800H | 800 nm·> 100 mJ/cm², 50 fs pulse, 800 nm·For High Power Femtosecond Laser Applications |
Out of stock
$988
|
| 990-0070-800HB | 780-820 nm·> 100 mJ/cm², 50 fs pulse, 800 nm·For High Power Femtosecond Laser Applications |
1 in stock
Ships in: 2–5 calendar days
$1,163
|
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Specifications
| Aperture diameter | 17 mm |
| Damage threshold / for high power laser applications | >10 mJ / cm², 50 fs pulse at 800 nm, typical / >100 mJ / cm², 50 fs pulse at 800 nm, typical |
| Time dispersion | t<4 fs for 100 fs Ti:Sapphire laser pulses |
| Polarization Contrast (after 1st polarizer) | >1:200 |
| Polarization Contrast (after 2nd polarizer) | >1:500 |
| Aperture diameter | 17 mm |
| Damage threshold | 5 J / cm² pulsed at 1064 nm, typical |
| Polarization Contrast (after 1st polarizer) | >1:200 |
| Polarization Contrast (after 2nd polarizer) | >1:500 |
| 990-0070 Variable Attenuator - STEP file |
Description
- Divides laser beam into two parallel beams of manually adjustable intensity ratio
- Large dynamic range
- Transmitted beam shift ~0.5 mm
- High optical damage threshold
- S-Pol attenuation range ~ 0.25% - 99.0%
- P-Pol attenuation range ~ 0.5 % - 95.0 %
This Variable Attenuator / Beamsplitter consists of special design Opto-mechanical Adapter and Precision Opto-mechanical Holder 840-0197. Two Thin Film Brewster type polarizers, which reflect s-polarized light while transmitting p-polarized light, are housed into Adapter. Quartz Half Waveplates are housed in rotating holder 840-0197.
The intensity ratio of those two beams may be continuously varied without alteration of other beam parameters by rotating the waveplate. The intensity of either exit beam, or their intensity ratio, can be controlled over a wide dynamic range. P-polarization could be selected for maximum transmission, or high-purity s-polarization could be reflected when maximum attenuation of the transmitted beam takes place. The holder 840-0197 allows to adjust angle of incidence of the Thin Film Brewster type polarizers by ±2° and to get the maximum polarization contrast.
Note: Movable base 820-0090, Rod Holder 820-0050-02 and standard rod should be ordered separately.
