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2.4 Output Beam Propagation<br />

26<br />

The lens discussed as a coupler above must also be used to "collimate"<br />

the output of a fiber in the fiber tap. Since the output of the fiber is Gaussian, it<br />

will expand as it propagates away from the lens. If arrays of lenses and fibers<br />

are to be used for interconnects, beam expansion must be minimized to reduce<br />

optical crosstalk between neighboring fibers. Beam expansion is determined<br />

by the microlens focal length ana diameter, which in turn depend upon the<br />

spacing between fiber centers.<br />

The minimum possible fiber spacing in an array will be equal to the<br />

diameter of the fiber cladding, a typical value being 125 nm. Assuming that the<br />

output of the fiber fills the lens, the ratio of lens diameter to beam waist as a<br />

function of distance may be calculated as in Figure 2-3 for several different lens<br />

diameters. It is clear from the figure that the beam divergence, and thus<br />

crosstalk between channels, increases with reduced lens diameter. Hence, a<br />

microlens diameter of 500 |am was chosen to minimize this problem. Table 2-1<br />

summarizes the resulting lens parameters that were calculated based on these<br />

factors.<br />

diameter<br />

500 p.m<br />

NA .16<br />

focal length 1.5625 mm<br />

F# 3.125<br />

Table 2-1 Microlens design parameters.

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