Continuously Variable Attenuator / Beamsplitter 990-0060

Continuously Variable Attenuator / Beamsplitter 990-0060

• Divides laser beam into two beams of manually adjustable intensity ratio • Convenient 90° angle between reflected and transmitted beams • Negligible beam deviation • Large dynamic range Continuously Variable… Read more →

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Central wavelength Any
or
Extinction ratio Any
or
Laser Damage Threshold Any
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7 catalog variants — refine the spec to narrow it down.
SKU Central wavelength · Laser Damage Threshold · Extinction ratio
990-0060-11IR 700-1000 nm·2 J/cm² @ 1064 nm, 10 Hz, 10 ns·> 200:1
Out of stock
$1,377
990-0060-11VIS 450-680 nm·1 J/cm² @ 532 nm, 10 Hz, 10 ns·> 200:1
Out of stock
$1,377
990-0061-11 1064 nm·15 J/cm² @ 1064 nm, 10 Hz, 10 ns·> 500:1
1 in stock Ships in: 2–5 calendar days
$863
990-0062-11 1030 nm·15 J/cm² @ 1030 nm, 10 Hz, 10 ns·> 500:1
Out of stock
$863
990-0063-11 800 nm·8 J/cm² @ 800 nm, 10 Hz, 10 ns·> 500:1
1 in stock Ships in: 2–5 calendar days
$863
990-0064-11 532 nm·6 J/cm² @ 532 nm, 10 Hz, 10 ns·> 500:1
Out of stock
$863
990-0065-11 355 nm·3 J/cm² @ 355 nm, 10 Hz, 10 ns·> 500:1
1 in stock Ships in: 2–5 calendar days
$863

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Specifications

Clear aperture 11 mm
Extinction ratio for broadband attenuators for attenuators designed for specific laser wavelength TS / TP < 1:200 TS / TP < 1:500
Weight 0.16 kg

Description

  • Divides laser beam into two beams of manually adjustable intensity ratio
  • Convenient 90° angle between reflected and transmitted beams
  • Negligible beam deviation
  • Large dynamic range


Continuously Variable Attenuators / Beamsplittesr are designed for down to 100 fs laser pulses. They consist of high-performance polarizing optics components placed in precision opto-mechanical holder 840-0197:

  • High power polarizing cubes, which reflect s-polarized light at 90° angle while transmitting p-polarized light
  • Rotating λ/2 waveplates, placed in the incident polarized beam

The intensity ratio of two exiting beams may be continuously varied over a wide dynamic range without alteration of other beam parameters by rotating the waveplate. Pure p-polarization could be selected for maximum transmission, or pure s-polarization for maximum attenuation of the transmitted beam.

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