Colin Wilkins, Vassilis Angelopoulos, Anton Artemyev, Andrei Runov, Xiao-Jia Zhang, Jiang Liu, Ethan Tsai
{"title":"质子各向同性边界的统计特征","authors":"Colin Wilkins, Vassilis Angelopoulos, Anton Artemyev, Andrei Runov, Xiao-Jia Zhang, Jiang Liu, Ethan Tsai","doi":"arxiv-2409.04488","DOIUrl":null,"url":null,"abstract":"Using particle data from the ELFIN satellites, we present a statistical study\nof 284 proton isotropy boundary events on the nightside magnetosphere,\ncharacterizing their occurrence and distribution in local time, latitude\n(L-shell), energy, and precipitating energy flux, as a function of geomagnetic\nactivity. For a given charged particle species and energy, its isotropy\nboundary (IB) is the magnetic latitude poleward of which persistently isotropic\npitch-angle distributions ($J_{prec}/J_{perp}\\sim 1$) are first observed to\noccur. This isotropization is interpreted as resulting from magnetic field-line\ncurvature (FLC) scattering in the equatorial magnetosphere. We find that proton\nIBs are observed under all observed activity levels, spanning 16 to 05 MLT with\n$\\sim$100% occurrence between 19 and 03 MLT, trending toward 60% at dawn/dusk.\nThese results are also compared with electron IB properties observed using\nELFIN, where we find similar trends across local time and activity, with the\nonset in $\\geq$50 keV proton IB occurring on average 2 L-shells lower, and\nproviding between 3 and 10 times as much precipitating power. Proton IBs\ntypically span $64^\\circ$-$66^\\circ$ in magnetic latitude (5-6 in L-shell),\ncorresponding to the outer edge of the ring current, tending toward lower IGRF\nlatitudes as geomagnetic activity increases. The IBs were found to commonly\noccur 0.3-2.1 Re beyond the plasmapause. Proton IBs typically span $<$50 keV to\n$\\sim$1 MeV in energy, maximizing near 22 MLT, and decreasing to a typical\nupper limit of 300-400 keV toward dawn and dusk, with peak observed isotropic\nenergy increasing by $\\sim$500 keV during active intervals. These results\nsuggest that FLC in the vicinity of IBs can provide a substantial depletion\nmechanism for energetic protons, with the total nightside precipitating power\nfrom FLC-scattering found to be on the order of 100 MW, at times $\\geq$10 GW.","PeriodicalId":501423,"journal":{"name":"arXiv - PHYS - Space Physics","volume":"9 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Statistical Characteristics of the Proton Isotropy Boundary\",\"authors\":\"Colin Wilkins, Vassilis Angelopoulos, Anton Artemyev, Andrei Runov, Xiao-Jia Zhang, Jiang Liu, Ethan Tsai\",\"doi\":\"arxiv-2409.04488\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Using particle data from the ELFIN satellites, we present a statistical study\\nof 284 proton isotropy boundary events on the nightside magnetosphere,\\ncharacterizing their occurrence and distribution in local time, latitude\\n(L-shell), energy, and precipitating energy flux, as a function of geomagnetic\\nactivity. For a given charged particle species and energy, its isotropy\\nboundary (IB) is the magnetic latitude poleward of which persistently isotropic\\npitch-angle distributions ($J_{prec}/J_{perp}\\\\sim 1$) are first observed to\\noccur. This isotropization is interpreted as resulting from magnetic field-line\\ncurvature (FLC) scattering in the equatorial magnetosphere. We find that proton\\nIBs are observed under all observed activity levels, spanning 16 to 05 MLT with\\n$\\\\sim$100% occurrence between 19 and 03 MLT, trending toward 60% at dawn/dusk.\\nThese results are also compared with electron IB properties observed using\\nELFIN, where we find similar trends across local time and activity, with the\\nonset in $\\\\geq$50 keV proton IB occurring on average 2 L-shells lower, and\\nproviding between 3 and 10 times as much precipitating power. Proton IBs\\ntypically span $64^\\\\circ$-$66^\\\\circ$ in magnetic latitude (5-6 in L-shell),\\ncorresponding to the outer edge of the ring current, tending toward lower IGRF\\nlatitudes as geomagnetic activity increases. The IBs were found to commonly\\noccur 0.3-2.1 Re beyond the plasmapause. Proton IBs typically span $<$50 keV to\\n$\\\\sim$1 MeV in energy, maximizing near 22 MLT, and decreasing to a typical\\nupper limit of 300-400 keV toward dawn and dusk, with peak observed isotropic\\nenergy increasing by $\\\\sim$500 keV during active intervals. These results\\nsuggest that FLC in the vicinity of IBs can provide a substantial depletion\\nmechanism for energetic protons, with the total nightside precipitating power\\nfrom FLC-scattering found to be on the order of 100 MW, at times $\\\\geq$10 GW.\",\"PeriodicalId\":501423,\"journal\":{\"name\":\"arXiv - PHYS - Space Physics\",\"volume\":\"9 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-09-06\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - PHYS - Space Physics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2409.04488\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Space Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.04488","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Statistical Characteristics of the Proton Isotropy Boundary
Using particle data from the ELFIN satellites, we present a statistical study
of 284 proton isotropy boundary events on the nightside magnetosphere,
characterizing their occurrence and distribution in local time, latitude
(L-shell), energy, and precipitating energy flux, as a function of geomagnetic
activity. For a given charged particle species and energy, its isotropy
boundary (IB) is the magnetic latitude poleward of which persistently isotropic
pitch-angle distributions ($J_{prec}/J_{perp}\sim 1$) are first observed to
occur. This isotropization is interpreted as resulting from magnetic field-line
curvature (FLC) scattering in the equatorial magnetosphere. We find that proton
IBs are observed under all observed activity levels, spanning 16 to 05 MLT with
$\sim$100% occurrence between 19 and 03 MLT, trending toward 60% at dawn/dusk.
These results are also compared with electron IB properties observed using
ELFIN, where we find similar trends across local time and activity, with the
onset in $\geq$50 keV proton IB occurring on average 2 L-shells lower, and
providing between 3 and 10 times as much precipitating power. Proton IBs
typically span $64^\circ$-$66^\circ$ in magnetic latitude (5-6 in L-shell),
corresponding to the outer edge of the ring current, tending toward lower IGRF
latitudes as geomagnetic activity increases. The IBs were found to commonly
occur 0.3-2.1 Re beyond the plasmapause. Proton IBs typically span $<$50 keV to
$\sim$1 MeV in energy, maximizing near 22 MLT, and decreasing to a typical
upper limit of 300-400 keV toward dawn and dusk, with peak observed isotropic
energy increasing by $\sim$500 keV during active intervals. These results
suggest that FLC in the vicinity of IBs can provide a substantial depletion
mechanism for energetic protons, with the total nightside precipitating power
from FLC-scattering found to be on the order of 100 MW, at times $\geq$10 GW.