Single-spacecraft measurements of solar-wind turbulence are interpreted as spatial spectra through Taylor's hypothesis (TH), which maps measured frequencies to wavenumbers via the advective Doppler shift and fails when the spacecraft speed relative to the plasma does not dominate fluctuation and Alfvénic speeds. Bourouaine & Perez (2019) proposed a sweeping-based spacetime-correlation model (BP19) that reconstructs the plasma-frame field-perpendicular spectrum from spacecraft frequency spectra under oblique sampling, with a single control parameter ; Perez, Bourouaine, Chen & Raouafi (2021) validated its use on four intervals from Parker Solar Probe's first four perihelia, but only for sampling angles above 30 degrees, , and inertial-range scales below roughly one quarter of the outer scale. The complementary regime — which contains most of what PSP actually measures — remains open and is the object of this task.
Background
A spacecraft immersed in the solar wind measures a time series of velocity and magnetic-field fluctuations, and nearly all knowledge of solar-wind turbulence spectra comes from converting such series into spatial information via Taylor's hypothesis (TH): if the plasma flow — or, for a fast spacecraft, the spacecraft velocity relative to the plasma frame — sweeps turbulent structures past the detector much faster than they evolve, the measured angular frequency maps to the wavenumber component along the sampling direction through , so a frequency power spectrum directly yields a one-dimensional spatial spectrum. The hypothesis requires the advective speed to dominate both the rms speed of the energy-containing (outer-scale) eddies and the relevant wave phase speeds. The Parker Solar Probe (PSP) mission, which approaches the Sun to within tens of solar radii, breaks these conditions: near perihelion the spacecraft speed in the plasma frame is only a few times the Alfvén speed , the sampling angle between the spacecraft velocity in the plasma frame and the local magnetic field varies strongly in time and is frequently small, and outer-scale velocity fluctuations are no longer negligible. Solar-wind turbulence is also anisotropic: in the critically balanced picture of strong magnetohydrodynamic (MHD) turbulence, Alfvénic propagation along the field balances the nonlinear cascade time, so the parallel-to-perpendicular wavenumber ratio is small in the inertial range (the range between the energy-containing scale and the dissipation scale) and the quantity of theoretical interest is the field-perpendicular reduced spectrum , the energy per unit after integrating over .
Bourouaine & Perez (2019) — "BP19" — proposed a way to interpret PSP turbulent signals beyond TH: extending the classical hydrodynamic random-sweeping picture to MHD, they modeled the Eulerian spacetime correlation of small-scale Alfvénic fluctuations as decorrelated by random advection through the outer-scale velocity, obtaining a kernel that relates the measured frequency spectrum to ,
for sufficiently oblique sampling, where compares the outer-scale rms velocity with the perpendicular spacecraft speed in the plasma frame and is a computable broadening factor depending on the spectral index . TH is recovered as and is expected to remain a good approximation for (a criterion established by Bourouaine & Perez 2020) irrespective of the Alfvén Mach number, provided the turbulence is strongly anisotropic and the sampling is sufficiently oblique ( much larger than a critical angle set by the anisotropy, ). The underlying spacetime-correlation model was validated against high-resolution simulations of strong reduced MHD (RMHD, the anisotropic limit of MHD for Alfvénic fluctuations) for inertial-range scales below roughly one quarter of the outer scale (Perez & Bourouaine 2020), and the reconstruction was demonstrated on Helios data at 0.6 au (Bourouaine & Perez 2020).
Perez, Bourouaine, Chen & Raouafi (2021) applied this methodology to four 24-hour intervals from PSP's first four close encounters (heliocentric distances 0.13–0.19 au). For sampling angles they found , so TH and the limit of BP19 hold there, spectral indices are faithfully recovered, and the reconstructed is independent of sampling angle — the method's internal consistency check. However, the validated regime excludes most of PSP's data: the distribution of peaks at small angles (a substantial portion of the signal lies at 10–20 degrees, nearly parallel to the field), the analysis neglects the parallel terms in the Doppler relation, the critical angle is estimated only from a critically balanced closure (, an acknowledged overestimate), the model's validity near the spectral break separating the and inertial ranges — where fluctuations are expected to be more isotropic — is unestablished, closer perihelia are expected to push toward and beyond the threshold at which TH and its BP19 limit fail, and the sensitivity of reconstructed amplitudes and indices to plasma-moment uncertainties (between PSP's Solar Probe Cup, SPC, and SPAN-ion plasma instruments) is unquantified.
Problem Statement
Complete and delimit the program, initiated by Bourouaine & Perez (2019) and applied by Perez et al. (2021), of converting single-point Parker Solar Probe frequency spectra into plasma-frame field-perpendicular turbulence spectra : determine for which sampling angles , sweeping parameters , and scale ranges (relative to the outer scale and the -to-inertial spectral break) the reconstruction is valid, and provide a reconstruction method covering PSP's actual measurement conditions near the Sun. The requested results are: (1) a generalized frequency–wavenumber reduction that retains the field-parallel contributions — the full and dependence of the Doppler relation and decorrelation kernel — so that near-parallel sampling (, below the critical angle ) can be interpreted, reducing to the published oblique, kernel in the appropriate limits; (2) a theoretical and observational characterization of the large-sweeping regime expected at PSP's closest perihelia, where both plain Taylor's hypothesis and its BP19 limit fail — in particular whether the sweeping kernel or any successor within the sweeping spacetime-correlation family (including the generalized kernel of result (1)) still reconstructs and its spectral index there; (3) a quantitative validity boundary in scale — how close to the outer scale and the spectral break the sweeping phenomenology can be trusted as fluctuations become more isotropic; (4) empirical single-point diagnostics of the turbulence anisotropy and of the critical sampling angle that do not rely on the critically balanced estimate , which is known to overestimate ; and (5) a quantified propagation of measurement uncertainties — plasma-moment discrepancies between the SPC and SPAN-ion instruments — into the reconstructed spectral amplitudes and indices. All five results are required and each is judged independently: establishing either outcome for a given result resolves that result, but a partial answer covering only a subset of the five does not complete the task. In particular, result (2) is a yes/no question, resolved by either a reconstruction that remains valid at or a quantified demonstration that no kernel in the sweeping spacetime-correlation family reconstructs there; for the latter outcome, the demand for a reconstruction method covering PSP's actual measurement conditions is met by the reconstruction method together with its explicitly delimited range of validity.
References
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