| Substrate Material |
Sapphire Crystal |
| Outer Diameter |
6.5mm, -0.1/0mm |
| Centre Thickness |
3.25mm, +/-0.05mm |
| Lens Design |
Half-ball ; Hemi-spherical surface |
| Radius of Curvature |
3.25mm ,-0.1/0mm |
| Edge Surface |
None; Edge thickness (ET) = 0, specially processed |
| Surface Quality |
Spherical surface:
40/20 scratch and dig; Surface accuracy: <lambda/4 @ 633nm; Clear aperture: >90%
Plano Surface:
20-10S/D; <lambda/4 @633nm over surface; Clear aperture: >90% |
| Coating |
Uncoated on both surfaces |
|
Chamfer/Chip: |
0.2mmx45deg protection chamfer; Chip <0.1mm |
| Orientation |
Random (if special orientation needed, please contact us) |
The effective focal length of a ball lens is very simple to calculate since there are only two variables: the ball lens diameter, D, and the index of refraction, n. The effective focal length is measured from the center of the lens. Therefore, the back focal length can also be easily calculated.
BFL = F - [D/2] EFL = nD/[4(n - 1)]
The Numerical Aperture, NA, of a ball lens is dependent on the focal length of the ball and on the input diameter, d. Since spherical aberration is inherent in ball lenses the following equation begins to fall off as d/D increases.
NA = [2d(n - 1)]/nD
When coupling light from a laser into a fiber, the choice of the ball is dependent on the NA of the fiber and the diameter of the laser beam. The diameter of the laser beam is used to determine the NA of the ball lens. The NA of the ball lens must be less than or equal to the NA of the fiber in order to couple all of the light into the fiber. The ball lens is placed directly onto the fiber.
To couple light from one fiber to another fiber of similar NA, two identical ball lenses are used. Place the two lenses in contact with the fibers.
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Optical Substrates
Optical Lenses
Spherical Plano Convex Lenses
