Product ID Specifications Price Qty In Stock Qty Buy
9000170
Angle tolerance: ±3 arcmin
Apex angle, °: 69.06
Clear aperture: >80
Dimensions A x L, mm: 25.4 x 25.4
Dimensions tolerance, mm: +0/-0.2
S1 Flatness, PV IR S2 Flatness, PV: <λ/10 @ 632.8 nm
Material: UVFS
Protective chamfers: <0.25 mm x 45°
Surface quality, S-D: 20-10
130.00
1
9538253
Apex angle, °: 69.06 (±3 arcmin)
AR coatings: uncoated
Clear Aperture: >80
Dimensions A x L, mm: 30 x 30 (+0/-0.2)
S1 Flatness, PV IR S2 Flatness, PV: <λ/8 @ 633 nm
Material: UVFS
Protective chamfers: 0.1-0.25 mm x 45°
Surface quality, S-D: 20-10
160.00
1
9581228
Angles: 60 deg +/- 2 arcmin
Clear aperture: >80 %
Coatings: Uncoated
Dimensions A x B x C, mm: 12.7 x 12.7 x 12.7 (+0.0/-0.3 mm)
Length: 12.7 mm(+0.0/-0.2 mm)
Material: Sf11
Pyramidal error: ±1 arcmin
Protective chamfers: <0.25 mm x 45 deg
S1 Flatness, PV IR S2 Flatness, PV: <λ/[email protected] 632.8 nm
Surface quality S1/S2: 40/20 S/D
78.00
1
Total: $0.00
Ex Tax: $0.00
0
Dispersing prisms are essential parts in most of ultrashort pulse laser systems. These prisms are used intracavity to compensate for dispersion of fixed cavity optics, such as active gain medium. But in most of cases they are used as extra-cavity elements to manipulate pulse characteristics.

Three materials with different dispersive properties are available. For the highest group velocity dispersion dense SF10 is used. Prisms made of SF10 feature GVD of ~1600 fs²/cm. GVD is equal to ~350 fs²/cm in case of fused silica.

Standard prisms feature high surface quality and flatness and only high purity optical materials are used in production. Prisms are designed in a way to satisfy condition of minimum loss due to entrance and exit at Brewster's angle.
  • High surface quality and flatness
  • Precisely cut at Brewster's angle
  • Minimal Fresnel losses

Brewster Angle Dispersing Prisms For Ultrashort Pulses

  • Product Code: BADP
  • Availability: In Stock




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