TPF-I SWG Report - Exoplanet Exploration Program - NASA
TPF-I SWG Report - Exoplanet Exploration Program - NASA
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 />
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