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Supplement to: Electron energy partition across interplanetary shocks: III. Analysis

<p><strong>Quick Summary:</strong></p> <p>The PDF file herein provides additional example superposed epoch analysis (SEA) plots in addition to reference tables of the upstream values used to normalize the SEA data in this file and those in the paper this supplement supports. &nbsp;This is a supplement to Part 3 of a three-part study of the electron&nbsp;velocity distribution functions (VDFs) observed near interplanetary (IP) shocks by the <em>Wind</em> spacecraft. &nbsp;Paper I&nbsp;[<a href="https://iopscience.iop.org/article/10.3847/1538-4365/ab22bd"><em>Wilson et al.</em>, 2019a</a>] introduced the methodology and data products&nbsp;[<a href="https://doi.org/10.5281/zenodo.2875806"><em>Wilson et al.</em>, 2019c</a>] for fitting the electron VDFs to the sum of three model functions. &nbsp;Paper II&nbsp;[<a href="https://iopscience.iop.org/article/10.3847/1538-4365/ab5445"><em>Wilson et al.</em>, 2019b</a>] presents the statistics of the fit parameters produced and provided in the data products from Paper I. &nbsp;Paper III presents and summarizes the analysis of the fit parameters. &nbsp;The papers share the title <strong><em>Electron energy partition across interplanetary shocks</em></strong>.</p> <p><strong><em>Wind</em> Spacecraft:</strong></p> <p>The <em>Wind</em> spacecraft (<a href="http://wind.nasa.gov/">https://wind.nasa.gov</a>) was launched on November 1, 1994 and currently orbits the first Lagrange point between the Earth and sun. &nbsp;It holds a suite of instruments from gamma ray detectors to quasi-static magnetic field instruments,&nbsp;<strong>B</strong><sub>o</sub>. &nbsp;The instruments used in this study and these datasets are the fluxgate magnetometer (<a href="https://doi.org/10.1007/BF00751330">MFI</a>), the radio receivers (<a href="https://doi.org/10.1007/BF00751331">WAVES</a>), ion&nbsp;Faraday cups (<a href="https://doi.org/10.1007/BF00751326">SWE</a>), and the electron and ion electrostatic analyzers (<a href="https://doi.org/10.1007/BF00751328">3DP</a>). &nbsp;The MFI measures 3-vector&nbsp;<strong>B</strong><sub>o</sub>&nbsp;at ~11 samples per second (sps); the SWE measures reduced VDFs of the thermal proton and alpha-particle populations from which velocity moments are derived and used herein; WAVES observes electromagnetic radiation from ~4 kHz to &gt;12 MHz which provides an observation of the upper hybrid line (also called the plasma line) used to define the total electron density; and 3DP observes full 4&pi; steradian VDFs of electrons and ions from a few eV to ~30 keV which provide both ion velocity moments and the electron VDFs modeled herein.</p> <p><strong>PDF Supplement Description:</strong></p> <p>Definitions:</p> <ul> <li>VDF = velocity distribution function</li> <li>Electron Components/Populations&nbsp;[taken from&nbsp;<a href="https://iopscience.iop.org/article/10.3847/1538-4365/ab22bd"><em>Wilson et al.</em>, 2019a</a>,<a href="https://iopscience.iop.org/article/10.3847/1538-4365/ab5445">b</a>] <ul> <li>Core (<em>s</em> = ec): &nbsp;cold, dense population with energies&nbsp;<span class="math-tex">\(E_{ec} \lesssim \text{15 eV}\)</span></li> <li>Halo (<em>s</em> = eh): &nbsp;hot, tenuous population with energies&nbsp;<span class="math-tex">\(E_{eh} \gtrsim \text{20 eV}\)</span></li> <li>Beam/Strahl (<em>s</em> = eb): &nbsp;anti-sunward propagating, magnetic field-aligned beam (or strahl) with&nbsp;<span class="math-tex">\(E_{eb} \sim \text{a few tens of eV}\)</span></li> <li>Effective (<em>s</em> = eff): &nbsp;effective total electron population, i.e., used for approximate moments rather than integrating entire VDF</li> </ul> </li> <li>Ion&nbsp;Components/Populations&nbsp;[taken from&nbsp;<a href="https://iopscience.iop.org/article/10.3847/1538-4365/ab22bd"><em>Wilson et al.</em>, 2019a</a>,<a href="https://iopscience.iop.org/article/10.3847/1538-4365/ab5445">b</a>] <ul> <li>Proton (<em>s</em> = p): &nbsp;core solar wind proton beam, i.e., main proton population streaming away from sun</li> <li>Alpha-particles (<em>s</em> = <span class="math-tex">\(\alpha\)</span>): &nbsp;alpha-particle magnetic field-aligned beam</li> </ul> </li> <li><span class="math-tex">\(k_{B}\)</span>&nbsp;=&nbsp;the Boltzmann constant [J K<sup>-1</sup>]</li> <li><span class="math-tex">\(\mu_{o}\)</span>&nbsp;=&nbsp;permeability of free space [T m A<sup>-1</sup>]</li> <li><span class="math-tex">\(n_{s}\)</span>= number density of species&nbsp;<em>s</em>&nbsp;[cm<sup>-3</sup>] (s = ec for core, eh for halo, eb for beam/strahl, p for proton, etc.)</li> <li><span class="math-tex">\(B_{o, j}\)</span>= j<sup>th</sup>&nbsp;component (GSE coordinate basis) of&nbsp;quasi-static magnetic field vector [nT]</li> <li><span class="math-tex">\(V_{Ts, j}\)</span>&nbsp;= j<sup>th</sup>&nbsp;component (relative to&nbsp;<strong>B</strong><sub>o</sub>) of thermal speed of species&nbsp;<em>s</em>&nbsp;[km/s] <ul> <li><span class="math-tex">\(V_{Ts, j} = \sqrt{ \tfrac{ 2 \ k_{B} \ T_{s, j} }{ m_{s} }}\)</span>, where&nbsp;<span class="math-tex">\(T_{s, j}\)</span>&nbsp;is the&nbsp;j<sup>th</sup>&nbsp;component (relative to&nbsp;<strong>B</strong><sub>o</sub>) of the temperature of species&nbsp;<em>s</em>&nbsp;[eV]</li> </ul> </li> <li><span class="math-tex">\(V_{os, j}\)</span>&nbsp;=&nbsp;j<sup>th</sup>&nbsp;component (relative to&nbsp;<strong>B</strong><sub>o</sub>) of drift speed of species&nbsp;<em>s</em>&nbsp;[km/s] in ion rest frame</li> <li><span class="math-tex">\(V_{s, j}\)</span>&nbsp;= j<sup>th</sup>&nbsp;component (GSE coordinate basis) bulk velocity of&nbsp;species&nbsp;<em>s</em>&nbsp;[km/s] in spacecraft frame</li> <li><span class="math-tex">\(T_{s, tot} = {1 \over 3} (T_{s, \parallel} + 2 \ T_{s, \perp})\)</span>, where&nbsp;<span class="math-tex">\(\parallel(\perp)\)</span>&nbsp;is the parallel(perpendicular) component&nbsp;relative to&nbsp;<strong>B</strong><sub>o</sub></li> <li><span class="math-tex">\(P_{s, j} = n_{s} \ k_{B} \ T_{s, j}\)</span>&nbsp;=&nbsp;partial thermal pressure [eV cm<sup>-3</sup>] of the <em>j</em><sup>th</sup> component of species <em>s</em></li> <li><span class="math-tex">\(P_{t, j} = \sum_{s} \ P_{s, j}\)</span>&nbsp;= total&nbsp;thermal pressure [eV cm<sup>-3</sup>] of the <em>j</em><sup>th</sup> component summed over all species including ions</li> <li><span class="math-tex">\(\mathcal{A}_{s} = \left(\tfrac{ T_{\perp} }{ T_{\parallel} } \right)_{s}\)</span>&nbsp;=&nbsp;temperature anisotropy [N/A] of species <em>s</em></li> <li><span class="math-tex">\(\xi_{s, j} = \tfrac{1}{2} m_{s} \ n_{s} \ V_{os, j}^{2}\)</span>&nbsp;= ram energy density [eV cm<sup>-3</sup>] <em>j</em><sup>th</sup> component of species <em>s</em></li> <li><span class="math-tex">\(\epsilon_{j} = \tfrac{ B_{o}^{2} }{ 2 \ \mu_{o} } + \sum_{s} \left[ P_{s, j} + \xi_{s, j} \right]\)</span>&nbsp;= total energy density [eV cm<sup>-3</sup>] of the&nbsp;<em>j</em><sup>th</sup> component&nbsp;of the system in the plasma bulk flow rest frame</li> <li><span class="math-tex">\(\zeta_{s, j} = \tfrac{ \xi_{s, j} }{ \epsilon_{j} }\)</span>&nbsp;=&nbsp;ratio of the ram energy density of the <em>j</em><sup>th</sup> component of species <em>s</em> to the total energy density [N/A]</li> <li><span class="math-tex">\(\psi_{s, j} = \tfrac{ P_{s, j} }{ \epsilon_{j} }\)</span>&nbsp;=&nbsp;ratio of the thermal energy density of the <em>j</em><sup>th</sup> component of species <em>s</em> to the total energy density [N/A]</li> <li><span class="math-tex">\(\Pi_{s, j} = \tfrac{ P_{s, j} }{ P_{t, j} }\)</span>&nbsp;=&nbsp;ratio of the partial thermal pressure of the <em>j</em><sup>th</sup> component of species <em>s</em> to the total thermal pressure [N/A]</li> <li><span class="math-tex">\(s_{es}\)</span>&nbsp;= exponent for the symmetric self-similar model VDF of&nbsp;species&nbsp;<em>s</em></li> <li><span class="math-tex">\(\kappa_{es}\)</span>&nbsp;= kappa value for the bi-kappa VDF of&nbsp;species&nbsp;<em>s</em></li> <li><span class="math-tex">\(p_{es}(q_{es})\)</span>&nbsp;= parallel(perpendicular)&nbsp;exponent for the asymmetric self-similar model VDF of&nbsp;species&nbsp;<em>s</em></li> <li><span class="math-tex">\(n_{eff} = \sum_{s} \ n_{s}\)</span>&nbsp;= effective number density of all electron populations</li> <li><span class="math-tex">\(T_{eff, j} = \tfrac{ \sum_{s} \ n_{s} \ T_{s, j} }{ n_{eff} }\)</span>&nbsp;= effective temperature of the&nbsp;<em>j</em><sup>th</sup> component of all electrons&nbsp;populations</li> <li><span class="math-tex">\(\beta_{s, j} = \tfrac{ 2 \ \mu_{o} \ n_{s} \ k_{B} \ T_{s, j} }{ B_{o}^{2} }\)</span>&nbsp;= plasma beta [N/A]&nbsp;of the <em>j</em><sup>th</sup> component of species <em>s</em></li> </ul> <p>&nbsp;</p> <p>This PDF supplement contains the following SEA plots:</p> <ul> <li><span class="math-tex">\(T_{s, j}\)</span>&nbsp;vs&nbsp;<span class="math-tex">\(\Delta\)</span>t (for <em>s</em> = ec, eh, and eb and <em>j</em> = <span class="math-tex">\(\parallel \text{ or } \perp \text{ or tot}\)</span>)</li> <li><span class="math-tex">\(\mathcal{A}_{s}\)</span>&nbsp;vs&nbsp;&nbsp;<span class="math-tex">\(\Delta\)</span>t (for <em>s</em> = ec, eh, and eb)</li> <li><span class="math-tex">\(\left( \tfrac{ T_{s} }{ T_{eff} } \right)_{j}\)</span>&nbsp;vs&nbsp;&nbsp;<span class="math-tex">\(\Delta\)</span>t (for <em>s</em> = ec, eh, and eb&nbsp;and j = <span class="math-tex">\(\parallel \text{ or } \perp \text{ or tot}\)</span>)</li> <li> <p><span class="math-tex">\(\psi_{s, j}\)</span>&nbsp;vs&nbsp;&nbsp;<span class="math-tex">\(\Delta\)</span>t (for <em>s</em> = ec, eh, eb, p, and <span class="math-tex">\(\alpha\)</span> and j = <span class="math-tex">\(\parallel \text{ or } \perp \text{ or tot}\)</span>)</p> </li> <li> <p><span class="math-tex">\(\Pi_{s, j}\)</span>&nbsp;vs&nbsp;&nbsp;<span class="math-tex">\(\Delta\)</span>t (for <em>s</em> = ec, eh, eb, p, and <span class="math-tex">\(\alpha\)</span> and j = <span class="math-tex">\(\parallel \text{ or } \perp \text{ or tot}\)</span>)</p> </li> </ul> <p>The PDF supplement contains tables of upstream median values for each shock used for normalizing the SEA plots, where the parameters listed include:</p> <ul> <li><span class="math-tex">\(T_{s, j}\)</span>&nbsp;(for <em>s</em> = ec, eh, and eb and&nbsp;j = <span class="math-tex">\(\parallel \text{ or } \perp \text{ or tot}\)</span>)</li> <li><span class="math-tex">\(n_{s}\)</span>&nbsp;(for <em>s</em> = ec, eh, eb, and eff and&nbsp;j = <span class="math-tex">\(\parallel \text{ or } \perp \text{ or tot}\)</span>)</li> <li><span class="math-tex">\(\tfrac{ n_{s} }{ n_{eff} }\)</span>&nbsp;(for <em>s</em> = ec, eh, and eb and&nbsp;j = <span class="math-tex">\(\parallel \text{ or } \perp \text{ or tot}\)</span>)</li> <li><span class="math-tex">\(\beta_{s, j}\)</span>&nbsp;(for <em>s</em> = ec, eh, and eb and&nbsp;j = <span class="math-tex">\(\parallel \text{ or } \perp \text{ or tot}\)</span>)</li> <li><span class="math-tex">\(s_{ec}\text{, }\kappa_{eh}\text{, and }\kappa_{eb}\)</span></li> <li><span class="math-tex">\(\mathcal{A}_{s}\)</span>&nbsp;(for <em>s</em> = ec, eh, eb, and eff)</li> <li><span class="math-tex">\(\left( \tfrac{ T_{s} }{ T_{eff} } \right)_{j}\)</span>&nbsp;(for <em>s</em> = ec, eh, and eb&nbsp;and j = <span class="math-tex">\(\parallel \text{ or } \perp \text{ or tot}\)</span>)</li> </ul>

ShareScore

36/100

Overall dataset sharing score

Score breakdown

These five areas show where the dataset supports — or may limit — practical reuse.

Stewardship
8
Harmonization
8
Access
16
Reuse readiness
0
Engagement
4

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