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dc.contributor.authorLiu, M.
dc.contributor.authorIssautier, K.
dc.contributor.authorMoncuquet, M.
dc.contributor.authorMeyer-Vernet, N.
dc.contributor.authorMaksimovic, M.
dc.contributor.authorHuang, J.
dc.contributor.authorMartinovic, M.M.
dc.contributor.authorGriton, L.
dc.contributor.authorChrysaphi, N.
dc.contributor.authorJagarlamudi, V.K.
dc.contributor.authorBale, S.D.
dc.contributor.authorPulupa, M.
dc.contributor.authorKasper, J.C.
dc.contributor.authorStevens, M.L.
dc.date.accessioned2024-08-03T06:54:40Z
dc.date.available2024-08-03T06:54:40Z
dc.date.issued2023-05-29
dc.identifier.citationA&A 674, A49 (2023)
dc.identifier.issn0004-6361
dc.identifier.doi10.1051/0004-6361/202245450
dc.identifier.urihttp://hdl.handle.net/10150/673306
dc.description.abstractAims. We applied the quasi-Thermal noise (QTN) method to Parker Solar Probe (PSP) observations to derive the total electron temperature (Te). We combined a set of encounters to make up a 12-day period of observations around each perihelion from encounter one (E01) to ten (E10), with E08 not included. Here, the heliocentric distance varies from about 13 to 60 solar radii (R). Methods. The QTN technique is a reliable tool to yield accurate measurements of the electron parameters in the solar wind. We obtained Te from the linear fit of the high-frequency part of the QTN spectra acquired by the RFS/FIELDS instrument. Then, we provided the mean radial electron temperature profile, and examined the electron temperature gradients for different solar wind populations (i.e. classified by the proton bulk speed, Vp, and the solar wind mass flux). Results. We find that the total electron temperature decreases with the distance as R0.66, which is much slower than adiabatic. The extrapolated Te based on PSP observations is consistent with the exospheric solar wind model prediction at 10 R, Helios observations at &0.3 AU, and Wind observations at 1 AU. Also, Te, extrapolated back to 10 R, is almost the same as the Strahl electron temperature, Ts (measured by SPAN-E), which is considered to be closely related to or even almost equal to the coronal electron temperature. Furthermore, the radial Te profiles in the slower solar wind (or flux tube with larger mass flux) are steeper than those in the faster solar wind (or flux tube with smaller mass flux). The more pronounced anticorrelation of VpA Te is observed when the solar wind is slower and located closer to the Sun. © 2023 EDP Sciences. All rights reserved.
dc.language.isoen
dc.publisherEDP Sciences
dc.rights© The Authors 2023. Open Access article, published by EDP Sciences, under the terms of the Creative Commons Attribution License.
dc.rights.urihttps://creativecommons.org/licenses/by/4.0/
dc.subjectAcceleration of particles
dc.subjectMethods: data analysis
dc.subjectPlasmas
dc.subjectSolar wind
dc.subjectSun: corona
dc.subjectSun: heliosphere
dc.titleTotal electron temperature derived from quasi-Thermal noise spectroscopy in the pristine solar wind from Parker Solar Probe observations
dc.typeArticle
dc.typetext
dc.contributor.departmentLunar and Planetary Laboratory, University of Arizona
dc.identifier.journalAstronomy and Astrophysics
dc.description.noteOpen access journal
dc.description.collectioninformationThis item from the UA Faculty Publications collection is made available by the University of Arizona with support from the University of Arizona Libraries. If you have questions, please contact us at repository@u.library.arizona.edu.
dc.eprint.versionFinal Published Version
dc.source.journaltitleAstronomy and Astrophysics
refterms.dateFOA2024-08-03T06:54:40Z


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© The Authors 2023. Open Access article, published by EDP Sciences, under the terms of the Creative Commons Attribution License.
Except where otherwise noted, this item's license is described as © The Authors 2023. Open Access article, published by EDP Sciences, under the terms of the Creative Commons Attribution License.