Our 3 mm thick Ultrafast Laser Beam Sampler is designed to minimize pulse dispersion while splitting off, or sampling, a beam by Fresnel Reflection for beam monitoring applications. The N-BK7 substrate is uncoated on the front surface to achieve beam division by Fresnel Reflection. The back surface is antireflection coated to prevent ghosting. A slight wedge in the substrate virtually eliminates internal fringes.
- Thin 3 mm substrate minimizes pulse dispersion
- Fresnel Reflectance from 1-10% at 45°
- Uncoated front surface for beam sampling
- AR coated back surface
- Grade A N-BK7 substrate See All Features
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![]() | 10B20-01NC.2Laser Beam Sampler, Ultrafast, 25.4 mm Diameter, 3.0 mm Thick | In Stock FREE 2-day shipping on thousands of products on Newport.com Learn More |
Specifications
- Wavelength Range660-1000 nm
- OrientationBeam should enter surface marked with an arrow
- Diameter25.4 mm
- Antireflection CoatingNC.2
- MaterialGrade A N-BK7
- Surface Quality15-5 scratch-dig
- Angle of Incidence45 °
- Substrate Number10B20
- Surface Flatness≤λ/10 at 632.8 nm over the clear aperture
- DurabilityMIL-C-675C, moderate abrasion million cycles
- Chamfers0.25-0.76 mm face width
- Chamfers Angle Tolerance45° ±15°
- Damage Threshold500 W/cm2 CW, 0.5 J/cm2 with 10 nsec pulses, typical
- Diameter Tolerance+0/-0.13 mm
- Wedge30 ±15 arc min
- Thickness3.0 mm
- Thickness Tolerance±0.38 mm
Features
Sample Ultrashort Pulses
In a beam sampler, percentage of reflected light is determined by the Fresnel reflection from a single surface. At the nominal 45° AOI the beam sampler reflects approximately 10% and 1% for s- and p- polarizations, respectively. For measuring beam power, the beam sampler should be oriented such that the laser is p-polarized. This choice will maximize transmitted power and attenuate power incident on the detector. Depending on the polarization of the incident beam, front surface reflectance from 1-10% can be attained at 45° incidence.
N-BK7 Substrates for VIS and NIR Applications
Slight Wedge Suppresses Unwanted Fringes
Optics with perfectly parallel faces are unsuited for use as reference elements in laser setups as reflections from both surfaces would be collinear resulting in undesired large period fringes. The introduction of a slight wedge causes unwanted reflections from the second surface to be deflected from the optical path. The back surface (S2) of this beam sampler is slightly wedged. The laser beam should enter the non-wedged surface (S1) where an arrow on the side points to.
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