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4.10 Summary of noise levels and transfer functions

To summarize the noise model: The principal noises are frequency and timing noise (FTS), plasma scintillation (solar wind and ionosphere), spacecraft electronics, unmodeled spacecraft motion, unmodeled ground antenna motion, tropospheric scintillation, ground electronics noise, thermal noise in the receiver, and systematic effects. The magnitudes of these noises in Cassini-era (2001 – 2008) observations are given in Table 2. Before any corrections, these noises enter the two-way Doppler as
noise FTS sw y2 (t) = y (t) ∗ [δ(t) − δ(t − T2)] + y (t) ∗ [δ(t) + δ(t − T2 + 2x∕c)] + yion ∗ [δ(t) + δ(t − T2 )] + ys∕c elect(t) ∗ δ(t − T2 ∕2) + ys∕c motion ∗ δ(t − T2 ∕2) + ant tropo ground elect y (t) ∗ [δ(t) + δ (t − T2)] + y (t) ∗ [δ(t) + δ(t − T2)] + y (t) + yrcvr + ysystematic(t), (4 )
where x is the effective distance of the solar wind perturbation from the earth. After multi-link plasma calibration, phase scintillation due to charged particles is effectively removed. Water-vapor-radiometer-based tropospheric calibration removes ≃ 90% of the low-frequency fluctuations due to the neutral atmosphere, so that the calibrated time series y2 is approximately
y (t) ≃ ygw + yFTS (t) ∗ [δ(t) − δ(t − T )] + ys∕c elect(t) ∗ δ(t − T ∕2 ) + 2 2 2 2 ys∕c motion ∗ δ(t − T2∕2 ) + yant(t) ∗ [δ(t) + δ (t − T2)] + ytropo(t)∕10 ∗ [δ(t) + δ(t − T2)] + yground elect(t) + yrcvr + ysystematic(t) gw other = y2 + y2 (t), (5 )
where yother(t) 2 is all the non-GW (noise plus systematics) contributions to the two-way Doppler variability.

Table 2 summarizes the noise model and the associated Allan deviation at τ = 1000 s for the principal noises (models of the spectra of the individual noises are given in [105Jump To The Next Citation Point]). Figure 5View Image shows, highly schematically, the signal flow. This sketch, the GW transfer function (see Equation (1View Equation)), and the noise transfer functions (see, e.g., Figure 7View Image) are used in discussions of sensitivity, signal processing, and for qualifying/disqualifying candidate GW events.


Table 2: Noise sources and contributions (expressed as Allan deviation [23Jump To The Next Citation Point] at 1000 s integration) in Cassini-era precision Doppler tracking GW observations. This table is adapted from [1Jump To The Next Citation Point, 22Jump To The Next Citation Point]. SEP: sun-earth-probe (solar elongation) angle; SNR: signal-to-noise ratio of the downlink. Models of the spectra of the individual noises are given in [105Jump To The Next Citation Point].






Noise source

σ y [1000 s]

Comment




     

Frequency standard

≃ 8 × 10–16

fundamental noise source [1Jump To The Next Citation Point22Jump To The Next Citation Point]

Antenna mechanical

≃ 2 × 10–15

DSS 25 (34-m antenna) under favorable conditions [19Jump To The Next Citation Point]

Ground electronics

≃ 2 × 10–16

measured in controlled test,
DSS 25 [1Jump To The Next Citation Point]

Plasma phase scintillation

< 10–15, for Ka-band and SEP ∘ > 150

σy depends on SEP; dispersive; scales as square of radio wavelength; see Figure 10View Image

Stochastic spacecraft motion

≃ 2 × 10–16

Cassini in quiet cruise [122123]; see Figure 13View ImageUpdateJump To The Next Update Information

Receiver thermal noise

few × 10–16

depends on link SNR and detector bandwidth [23]

Spacecraft transponder noise

≃ 10–16

preflight tests of Cassini Ka-band translator [122Jump To The Next Citation Point]

Tropospheric scintillation
(raw)

< 3 × 10–15 to ≃ 30 × 10–15

variable; nondispersive [20,  71]

Tropospheric scintillation
(corrected)

< 1.5 × 10–15 to ≃ 3 × 10–15

under favorable conditions [19Jump To The Next Citation Point]; median conditions in connected-element interferometry tests [90Jump To The Next Citation Point]







     


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