Fig. 2

Global performance comparison between multimode and singlemode
interferometry, all sources of noise considered. Top: error of the
phase in multimode (dotted lines) and singlemode (solid lines) as the function of
the number of detected photoevents (per time unit) and K-band
magnitude. For both cases, we can see the three regimes: the detector noise (in
1/N), then (shortly) the photon noise (in
)
and finally the speckle noise (saturation). Bottom: ratio of
multimode vs. singlemode phase error. Plots are shown for several levels of
correction (Strehl ratios). The fixed parameters are
σdet = 4e − / pix,
|Vij | = 1, Npix = 4. Two
turbulence strengths are considered
D/r0 = 8
(left) and
D/r0 = 2
(right) that correspond to the average turbulence conditions of
the VLTI with UTs (D = 8 m) and ATs (D = 1.8 m)
respectively. For the conversion between detected photoevents and magnitude scale,
we have considered a total transmission coefficient of 15%, a detector quantum
efficiency of 50%, an integration time of 30 ms and a spectral resolution of 35 with
2 pixels by spectral channel.
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