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| | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | Optics | | | | | | | | | | | | | | optical Systems | | | | | PPLN Devices | | | | Sp | herical Singlets | | | | | | | | | | | | | | | | | Equilateral Dispersive Prism Dispersive Equilateral Prisms have lower stray light and none of the higher order problems associated with diffraction gratings. Two high refractive index, low Abbe Vd number glasses have been chosen to provide the maximum dispersive power. The Abbe Vd number is calculated by: | | | | | | | | | | Multi-element Lenses | | | | | | | | | | | | | | 1 | | | | | | | | | | | | | Cylindrical Lenses | | | | A | spheric Lenses | | | | | | | | | | | | | Yd: | | | | | | | | | | | | | | nF - nc | | | | | | | | | | where np and nc are the indices of refraction for the helium d-line (587.6nm), the hydrogen p-line (486.1nm) and the hydrogen C-line (656.3nm). prom the formula, An = np - nc is a measure of dispersion. A higher value of An yields a lower Vd, and a greater dispersion. Such prisms are typically used at the minimum angle of deviation. This is the angle where the wavelength of interest travels parallel to the base of the prism and the angle of incidence is equal to the angle of refraction when measured to the normal of the face of the prism at the respective interface. At the minimum angle of deviation, a maximum clear aperture is achieved and reflective loss in the P-polarization is reduced due to the close proximity to Brewster's angle of the incident light. For S-polarization, an anti-reflective coating will enhance transmission. | | | | | | | | | | Windows | | & Diffusers | | | | | | | | | | Prisms | | | | | | | | | | Gratings | | | | | | | | | | iffractive Optics | | | | | | | | | | olarization Optics | | | | | | | | | | | | | | Beamsplitters | | | | | | | | | | Filters & Attenuators | | | | | | | | | | Swivel Mount: 60mm Cage System See Page 212 | | | | | | | | | | Specifications ■ Materials: P2 or SF11 (See Price Table) ■ Dimensional Tolerances: ±0.15mm ■ Angular Tolerances: ±5 arcmin ■ Surface Quality: 40-20 ■ Surface Flatness: A./10 (70% of Clear Aperture) | | | | | | Prism, PM2 and Base not included -4 | | | | | | | | | | | | | | SF11 stains easily. Clean off fingerprints quickly and this optic will last. | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | AX | Vd (see note 2) | INDEX n @ 633nm | | | | ITEM# | $ | | € | „ | A=B=C=H | GLASS | A9 (see note 1) | | | | PS850 | $ 76.00 | £ 57.00 | € 79,80 | „ 12,920 | 10mm | F2 | 150nm/degree | 36.37 | 1.617 | | | | PS851 | $ 86.00 | £ 64.50 | € 90,30 | „ 14,620 | 10mm | SF11 | 67nm/degree | 25.76 | 1.779 | | | | PS856 | $ 82.00 | £ 61.50 | € 86,10 | „ 13,940 | 15mm | F2 | 150nm/degree | 36.37 | 1.617 | | | | PS857 | $ 90.00 | £ 67.50 | € 94,50 | „ 15,300 | 15mm | SF11 | 67nm/degree | 25.76 | 1.779 | | | | PS858 | $ 88.00 | £ 66.00 | € 92,40 | „ 14,960 | 20mm | F2 | 150nm/degree | 36.37 | 1.617 | | | | PS859 | $ 90.00 | £ 67.50 | € 94,50 | „ 15,300 | 20mm | SF11 | 67nm/degree | 25.76 | 1.779 | | | | PS852 | $ 98.00 | £ 73.50 | € 102,90 | „ 16,660 | 25mm | F2 | 150nm/degree | 36.37 | 1.617 | | | | PS853 | $ 98.00 | £ 73.50 | € 102,90 | „ 16,660 | 25mm | SF11 | 67nm/degree | 25.76 | 1.779 | | | | PS855 | $ 216.00 | £ 162.00 | € 226,80 | „ 36,720 | 40mm | SF11 | 67nm/degree | 25.76 | 1.779 | | | | PS854 | $ 198.00 | £ 148.50 | € 207,90 | „ 33,660 | 50mm | F2 | 150nm/degree | 36.37 | 1.617 | | | | | | | | | | | | | | | | | | | | | | | | | 1 AX/A8 is calculated for a 633nm HeNe Laser with the prism angle set such that the light rays pass through the prism parallel to its base (i.e. minimum deviation angle). V = nd - 1 2 The Abbe number is calculated by d = np - nc where nd, np and nc are the indices of refraction for the helium D-line (587.6nm), the hydrogen p-line (486.1nm) and the hydrogen C-line (656.3nm). | | | | | | | | | | "IHOTOiSilSl Sales: 973-579-7227 | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | |
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