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TPF-I SWG Report - Exoplanet Exploration Program - NASA

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C HAPTER 4<br />

combiner, two beams are extracted, so a total of four beams are sensed at the array. For the second crosscombiner<br />

a second fringe tracker would be needed unless a laser metrology could be used to transfer<br />

measured phase to the second nuller.<br />

4.6.2 Multi-Axial Beam Combiners<br />

In contrast to classical beamsplitter-based beam-combiner designs, it is also possible to combine optical<br />

beams using single-mode fibers. Technology at long wavelengths has not advanced to the point where<br />

each of the various beams to be combined can be injected into separate fibers and then combined using<br />

cross-couplers. However, another approach is feasible. Separate beams can be directly combined into a<br />

single fiber simply by using a common focusing optic, as in Figure 4-14. Each of the individual beams<br />

must couple to the same spatial mode in the single-mode fiber. Thus, if the beams (in the two beam case)<br />

arrive with a relative phase shift of π radians, the two beams entering the fiber mode will cancel each<br />

other. Note that a large number of beams can be combined in one step, as a number of beams around the<br />

periphery of a common focusing optic can all be simultaneously focused onto the common fiber tip<br />

(Figure 4-15; Karlsson et al. 2004; Wallner et al. 2004). This method of “fiber nulling” has now been<br />

verified in the optical regime, where deep narrowband nulls close to one part in a million have already<br />

been obtained (Haguenauer and Serabyn 2006) , and in the near-infrared, where broad-band nulls of a few<br />

10 -4 have been obtained across the H band (Figure 4-16; Mennesson et al. 2006). However, while simple<br />

and easy to use, this nulling approach also has disadvantages, including lower efficiencies in the case of a<br />

small number of beams, and the lack of a complementary, or “bright” output. Thus, more experience with<br />

this type of combiner is required to fully understand the trade-offs relative to classical beamcombiners.<br />

Focal plane<br />

intensity<br />

Single-mode<br />

waveguide<br />

Fiber fundamental mode<br />

Single sub-pupil intensity<br />

Interference intensity<br />

beam 1<br />

Focusing optics<br />

beam 2<br />

Combined field amplitude<br />

Transversal cuts in focal plane<br />

Figure 4-14. Principle of single-mode fiber beam combination. The two beams are combined by the<br />

same focusing element onto the core of a single-mode fiber.<br />

76

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