磁気圏対流の発達に伴う内部磁気圏プラズマ密度の異常増加
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(2) . ☢ẼᅪᑐὶࡢⓎ㐩క࠺ෆ㒊☢Ẽᅪࣉࣛࢬ࣐ᐦᗘࡢ␗ᖖቑຍ Steep increase in plasma mass density associated with growth of magnetospheric convection ᑿⰼ ⏤⣖*1, ᯇ⥴ ⩧ః*1, *2 Yuki Obana*1 , Shogo Matsuo*1, *2 Abstract Using the cross-phase analysis of geomagnetic data observed in Northern America, we determined the equatorial mass density at L = 2.6 and 2.9 during two geomagnetic storms in April 2001. On 25 April, in the late recovery phase of the first storm, the frequency of the field line resonances increased slightly in response to the reductions in the mass density of the plasma. From 25 to 27 April, the plasma mass density showed a clear diurnal variation associated with a linear increase in the plasma density in the daytime and a decrease in the plasma density at nighttime. The daytime increases in the plasma mass density were related to refilling rates ranging from 181 to 33 amu/cc/h over L = 2.6–2.9. This result is comparable with the results obtained in previous studies. On the other hand, on 28 April, the second storm commenced, and the plasma mass density increased very steeply. The increase rate reached 473 and 118 amu/cc/h at L = 2.6 and 2.9, respectively. These values are remarkably high in comparison with the refilling rate observed previously. Such an increase in the main phase of the storm can be qualitatively explained by the transfer of the plasma and/or the delay of the co-rotation due to the magnetic convection.. 㸬ࡣࡌࡵ ᆅ⌫☢ሙࡢໃຊᅪ࡛࠶ࡿᆅ⌫☢Ẽᅪࡢ୰ࡣࠊࣉࣛࢬ࣐ࡢ ᗘ࣭ᅽຊ➼ࡼࡗ࡚ศ㢮ࡉࢀࡿࡉ ࡲࡊࡲ࡞㡿ᇦࡀ࠶ࡿࠋࡑࡢ୰ࡢ୍ࡘ࡛࠶ࡿࣉࣛࢬ࣐ᅪࡣෆ㒊☢Ẽᅪ⨨ࡋࠊ㟁㞳ᅪ㉳※⪃࠼ ࡽࢀࡿ෭ࡓ࠸ࣉࣛࢬ࣐ࡀ㧗ᐦᗘ⃰㞟ࡋ࡚࠸ࡿ㡿ᇦ࡛࠶ࡿࠋࣉࣛࢬ࣐ᅪࡢእഃࡢቃ⏺ࡣࣉࣛࢬ࣐ ᅪ⏺㠃ࡤࢀࠊࡋࡤࡋࡤᐦᗘࡢᛴ⃭࡞ኚࢆక࠺ࠊ᫂░࡞ቃ⏺ࡋ࡚ほ ࡉࢀࡿ[1,2]ࠋࣉࣛࢬ ࣐ᅪ⏺㠃ࡣ୍⯡ࠊඹᅇ㌿ࡍࡿ㛢ࡌࡓ☢ຊ⥺ᑐὶࡍࡿ㛤࠸ࡓ☢ຊ⥺ࡢ㌶㐨ࡢቃ⏺࡛࠶ࡿㄝ᫂ ࡉࢀ࡚࠾ࡾࠊ☢Ẽᅪᑐὶ㟁ሙࡢᾘ㛗ᛂ⟅ࡋ࡚ࣉࣛࢬ࣐ᅪࡢࡁࡉࡸᙧ≧ࡶࢲࢼ࣑ࢵࢡኚ ࡍࡿ[3]ࠋ☢Ẽᅪᩘ᪥㛫㟼✜࡞≧ែࡀ⥆࠸ࡓᚋࡣࠊࣉࣛࢬ࣐ᅪࡣ㟁㞳ᅪࡽࡢࣉࣛࢬ࣐౪⤥ࡢ⤖ ᯝ㣬ࡋࠊL ~ 8 ⛬ᗘࡲ࡛ᣑࡋ࡚࠸ࡿࠋࡦࡓࡧ☢ẼᅪᨐࡀⓎ⏕ࡋ࡚☢Ẽᅪᑐὶࡀᙉࡲࡿࠊ ࣉࣛࢬ࣐ᅪࡣእഃࡽᾐ㣗ࡉࢀࠊࣉࣛࢬ࣐ᅪ⏺㠃ࡣᆅᚰ㊥㞳 2 ~ 3 [Re]⛬ᗘࡲ࡛⦰ᑠࡋࠊ☢᮰⟶ෆ ࡢࣉࣛࢬ࣐ᐦᗘࡀࡁࡃῶᑡࡍࡿࠋᨐࡀࡲࡾࠊ☢Ẽᅪᑐὶࡀࡲࡿࠊࡧඹᅇ㌿㡿ᇦࡀᣑ ࡋࠊ㛢ࡌࡓ☢ຊ⥺㟁㞳ᅪࡽᚎࠎࣉࣛࢬ࣐ࡀ౪⤥ࡉࢀࠊࣉࣛࢬ࣐ᅪࡣᩘ᪥㛫ࡅ࡚ᅇ ࡍࡿ[4,5]ࠋࡇࡢᅇࣉࣟࢭࢫࢆࣉࣛࢬ࣐ᅪࡢሸ࠸࠺ࠋ "#$%&'()*+',-./$012345" ࣉࣛࢬ࣐ᅪࡢᾐ㣗ሸࡣ☢Ẽᅪࣉࣛࢬ࣐ࡢ㉳※ࡸᆅ⌫Ẽࡽࡢ≀㉁ὶฟࠊᆅ⌫Ẽ⤌ᡂ *1 㜰㟁Ẽ㏻ಙᏛ ᕤᏛ㒊 ᇶ♏⌮ᕤᏛ⛉, *2 ᰴᘧ♫ ᪂〇సᡤ !. .
(3) ࡢᡂࡾ❧ࡕࢆ⪃࠼ࡿ࠺࠼࡛㔜せ࡛࠶ࡿࡀࠊࡑࡢヲ⣽࡞ᥥീࡸ࣓࢝ࢽࢬ࣒ࡣ࠸ࡲࡔ᫂࡞Ⅼࡀከ ࠸ࠋ࠼ࡤᴟᇦࡢ࢜ࣥὶฟࡣ H+, He+, O+ࡢ⢏Ꮚ✀ࡈὶฟ㏿ᗘࡢ㧗ᗘࣉࣟࣇࣝࡶ᫂ࡽ ࡉࢀ࡚࠸ࡿࡀ[5]ࠊ୰ప⦋ᗘࡢ࢘ࢺࣇ࣮ࣟほ ࡣὶ㔞ࡀᑡ࡞࠸࠺࠼ᨺᑕ⥺ᖏ⢏Ꮚࡢᙳ㡪࡛㞴ࡋ ࡃࠊ㐍ࢇ࡛࠸࡞࠸ࠋKrall et al. [6] ࡢ㟁㞳ᅪࣔࢹࣝᩘ್ィ⟬ࡼࡿࣉࣛࢬ࣐ᅪࡢ H+ He+ࡢ ሸ⋡ࡣኴ㝧άືᗘࡁࡃ౫Ꮡࡋࠊࡑࢀࡒࢀࡃ␗࡞ࡿࡩࡿࡲ࠸ࢆぢࡏࡿணࡉࢀ࡚࠸ࡿࡀࠊ ほ ࡛☜ࡵࡓࡣ࡞࠸ࠋ ࡑࡇ࡛ᮏ◊✲࡛ࡣࠊᆅ☢ẼከⅬほ ࢹ࣮ࢱࢆ⏝࠸ࡓࣉࣛࢬ࣐ᐦᗘࡢ᥎ᐃἲࢆ⏝࠸࡚ࣉࣛࢬ࣐ᅪ ሸࢆヲ⣽ㄪࡓࠋᆅ☢Ẽほ ࡼࡗ࡚㢖⦾ࡽ࠼ࡽࢀࡿ ULF ࿘Ἴᩘᖏࡢᆅ☢Ẽ⬦ືࡀ☢ ຊ⥺ඹ㬆ື (field line resonance: FLR) ⓗ࡞ᛶ㉁ࢆᣢࡘࡇࡣྂࡃࡽ▱ࡽࢀ࡚࠾ࡾ[7]ࠊࡇࡢඹ 㬆ືᩘࢆᆅ☢Ẽࢹ࣮ࢱࡽᢳฟࡋࠊ☢Ẽᅪ㉥㐨㠃࠾ࡅࡿࣉࣛࢬ࣐㉁㔞ᐦᗘࢆ᥎ᐃࡍࡿࠋᆅୖ ☢ሙほ ࡣேཱྀ⾨ᫍࡼࡿᏱᐂࣉࣛࢬ࣐ࡢ┤᥋ほ ẚᏳ౯ከⅬほ ⥙ࡀᒎ㛤࣭⥔ᣢ࡛ࡁࠊ 㛗ᮇほ ࡼࡗ࡚ኴ㝧άືᗘࡢ㛵㐃࡞ࢆㄪࡿ㝿᭷࡛࠶ࡿࠋᡃࠎࡣ 2010 ᖺᗘࡽࢽ࣮ࣗ ࢪ࣮ࣛࣥࢻᆅ☢Ẽほ ⥙ࡢᩚഛࢆጞࡵ࡚࠾ࡾࠊᮏ◊✲ࡣࡑࡢࡓࡵࡢணഛゎᯒⓗ࡞ព⩏ࡶ࠶ࡿࠋ. 㸬ほ ᡭἲ ᆅ☢Ẽほ ࡼࡗ࡚ᚓࡽࢀࡓ ULF ࿘Ἴᩘᖏࡢᆅ☢Ẽ⬦ືࡽࣉࣛࢬ࣐㉁㔞ᐦᗘࢆぢ✚ࡶࡿࡓࡵ ࡣࠊᆅ☢Ẽほ Ⅼ࣌ࢆ㑅ࡧࠊᆅ☢Ẽࢹ࣮ࢱࡽ FLR ඹ㬆࿘ἼᩘࢆྠᐃࡍࡿࠋḟἼື᪉⛬ᘧ ࢆゎࡃࡓࡵ㐺ࡋࡓᆅ☢Ẽࣔࢹࣝࣉࣛࢬ࣐ᐦᗘศᕸࣔࢹࣝࢆ㑅ᢥࡋࡓୖ࡛ࠊἼື᪉⛬ᘧࢆゎ࠸ ࡚ほ ࡽᚓࡓඹ㬆࿘Ἴᩘࢆㄝ᫂ࡍࡿࣉࣛࢬ࣐㉁㔞ᐦᗘࢆồࡵࡿࠋ௨ୗࠊྛᡭ㡰ࡢヲ⣽ࢆㄝ᫂ࡍ ࡿࠋ. ᆅ☢Ẽほ Ⅼ࣌ࡢ㑅ᢥ ᅇゎᯒ⏝࠸ࡓᆅ☢Ẽࢹ࣮ࢱࡣ⡿ᒎ㛤ࡉࢀࡓ the Magnetometers along the Eastern Atlantic Seaboard for Undergraduate Research and Education (MEASURE) ほ ⥙ࡢ Clarkson University (CLK, ⦋ᗘ 44.7°N, ⤒ᗘ 285.0°, L ್ 3.1Re)ࠊMillstone Hill (MSH, 42.6°N, 288.5°, 2.8Re)ࠊThe Johns Hopkins University Applied Physics Laboratory (APL, 39.2°N, 283.1°, 2.4Re)ࡢ 3 ほ Ⅼ࡛ᚓࡽࢀࡓࡶ ࡢ࡛࠶ࡿࠋ࠸ࡎࢀࡢほ Ⅼ࡛ࡶࣇࣛࢵࢡࢫࢤ࣮ࢺᆺ☢ຊィࢆ⏝࠸࡚ᆅ☢Ẽ 3 ᡂศࢆ㸯⛊ẖグ㘓 ࡋ࡚࠾ࡾࠊᮏ◊✲࡛ࡣ H㸦༡㸧ᡂศࢆ⏝ࡋࡓࠋL ್ࡣ☢ຊ⥺ࡀ᭱ࡶ㐲᪉㞳ࢀࡓⅬࡢᆅ⌫ ୰ᚰࡽࡢ㊥㞳࡛ࠊ༢ࡢ Re ࡣᆅ⌫༙ᚄ࡛࠶ࡿࠋࡇࢀࡽࡢほ Ⅼࡽ⾲㸯♧ࡍほ Ⅼ࣌ࢆస ⾲ 1 cross-phase ゎᯒ⏝࠸ࡓᆅ☢Ẽほ Ⅼ࣌ ほ Ⅼྡ. ⦋ᗘ. ⤒ᗘ. L್. CLK-MSH. 43.7±1.1 °N. 286.8±1.8 °. 2.9±0.2 Re. MSH-APL. 40.9±1.7 °N. 285.8±2.7 °. 2.6±0.2 Re. .
(4) ࡗࡓࠋᕥࡽほ Ⅼྡࡢ 3 ᩥᏐࢥ࣮ࢻࠊ࣌ࡢ୰㛫ᆅⅬ࠾ࡅࡿ⦋ᗘࠊ⤒ᗘࠊL ್ࢆ♧ࡋ࡚࠸ࡿࠋ ᮏ◊✲࡛⾜ࡗࡓゎᯒ࡛ࡣ☢Ẽᅪ㉥㐨㠃࠾ࡅࡿࣉࣛࢬ࣐㉁㔞ᐦᗘࡀᚓࡽࢀࡿࡢ࡛ࠊࡇࡢࢹ࣮ࢱ ࢭࢵࢺࡽࡣ☢Ẽᅪࡢ L=2.6, 2.9 Re ࠾ࡅࡿࣉࣛࢬ࣐ᐦᗘࡀồࡵࡽࢀࡿࡇ࡞ࡿࠋ. )/5 ࿘Ἴᩘࡢྠᐃ ULF ⬦ືࡽ FLR ࿘Ἴᩘࢆྠᐃࡍࡿࡣࠊほ Ⅼ࣌㛫࡛ᖜࡲࡓࡣ┦ྠኈࢆẚ㍑ࡍࡿࠋ FLR ᖜࡣඹ㬆Ⅼ࡛ᴟ࡞ࡿᛶ㉁ࡀ࠶ࡿࠋࡲࡓࠊඹ㬆࿘Ἴᩘࡣ☢ຊ⥺ࡢ㛗ࡉ౫Ꮡࡍࡿࡢ࡛ࠊ୍⯡ ⓗ⦋ᗘࡢ␗࡞ࡿほ Ⅼ࡛ࡣ㧗⦋ᗘഃࡢほ Ⅼࡢ࠺ࡀప࠸ඹ㬆࿘Ἴᩘࢆᣢࡘࠋࡑࡢࡓࡵほ Ⅼ ࣌㛫ࡢᖜẚࢫ࣌ࢡࢺࣝࡣᴟᏊᆺࡢ᭤⥺ࢆᥥࡁࠊᴟᏊࡢ୰㛫ࡲࡓࡣ㸯ࢆ㏻ࡿⅬࡀ࣌ࡢ୰ 㛫ᆅⅬ࠾ࡅࡿඹ㬆ືᩘࡋ࡚ᢳฟࡉࢀࡿࠋࡇࢀࡀᖜẚἲࡲࡓࡣ gradient ἲ➼ࡤࢀࡿ᪉ ἲ࡛࠶ࡿ[8]ࠋࡲࡓࠊFLR ࡢ┦ࡣඹ㬆Ⅼࡢ๓ᚋ࡛ࡁࡃኚࡍࡿᛶ㉁ࡀ࠶ࡿࡢ࡛ࠊ㸰Ⅼ㛫ࡢ┦ ᕪࢫ࣌ࢡࢺࣝࡣ୰㛫ᆅⅬࡢඹ㬆ືᩘࢆ୰ᚰᴟࡲࡓࡣᴟᑠࢆ♧ࡍࠋࡇࢀࡀ cross-phase ἲࡢཎ ⌮࡛࠶ࡿ[9]ࠋ ᮏ◊✲࡛ࡣࠊgradient ἲࠊcross-phase ἲ୧᪉ࢆࡗ࡚ FLR ࿘Ἴᩘࢆྠᐃࡋࠊࡑࡢᕪࢆ࿘ἼᩘỴ ᐃୖࡢㄗᕪ⠊ᅖࡋࡓࠋᅗ㸯ࡣ 2001 ᖺ 4 ᭶ 27 ᪥ 17:30-18:30 UT CLK-MSH ࡛ほ ࡉࢀࡓᆅ☢ Ẽ H ᡂศࢹ࣮ࢱࢆࡗࡓゎᯒ࡛࠶ࡿࠋほ Ⅼࡢᆅ᪉ࡣ LT = UT – 5 㛫࡞ࡢ࡛ṇ༗㐣ࡂࡢほ ࢹ࣮ࢱ࡛࠶ࡿࠋୖࡽ CLK ࡢࣃ࣮࣡ࢫ࣌ࢡࢺࣝ(a)ࠊMSH ࡢࣃ࣮࣡ࢫ࣌ࢡࢺࣝ(b)ࠊCLK-MSH 㛫ࡢࢥࣄ࣮ࣞࣥࢫ(c)ࠊ┦ᕪ(d)ࠊࣃ࣮࣡ẚ(e) ࢆ♧ࡋ࡚࠾ࡾࠊᶓ㍈ࡣࡍ࡚࿘Ἴᩘ࡛࠶ࡿࠋ0-23 mHz ࡢ⠊ᅖ࡛ࡣࢥࣄ࣮ࣞࣥࢫࡀ୍㈏ࡋ࡚ 0.9 ௨ୖࢆಖࡗ࡚࠾ࡾࠊCLK MSH ඹ㏻ࡢಙྕࡀධᑕࡋ࡚ ࠸ࡿࡇࡀఛ࠼ࡿࠋࡲࡓ┦ᕪࣃ࣮࣡ẚࡣ~14mHz ࿘㎶≉ᚩⓗ࡞ᵓ㐀ࡀぢࡽࢀࡿࠋ┦ᕪ ࡣᴟᑠࢆ♧ࡋࠊࣃ࣮࣡ẚࡣప࿘Ἴᩘഃ࡛ᴟࠊ㧗࿘Ἴᩘഃ࡛ᴟᑠ࡞ࡿᴟᏊᆺࡢኚࢆぢࡏ࡚ ࠸ࡿࡇࡽ CLK-MSH ୰㛫Ⅼࡢඹ㬆࿘Ἴᩘࢆ 14.5±0.2 mHz ྠᐃࡋࡓࠋ. ᆅ☢Ẽࣔࢹࣝࡢ㑅ᢥ ୖࡢᡭ㡰࡛☢ຊ⥺ඹ㬆࿘Ἴᩘࡀᚓࡽࢀࡓࡢ࡛ࠊḟἼື᪉⛬ᘧࢆゎ࠸࡚ほ ୍⮴ࡍࡿඹ㬆࿘ Ἴᩘࢆ࠼ࡿࣉࣛࢬ࣐ᐦᗘࢆィ⟬ࡍࡿࠋFLR Ἴື᪉⛬ᘧࢆゎࡃࡓࡵࡣ☢ຊ⥺ࡢᙧ≧☢ሙᙉᗘ ࡢሗࡀᚲせ࡛࠶ࡾࠊࡇࢀࡣࣔࢹࣝࡽ࠼ࡿࠋᮏ◊✲࡛ࡣࠊẚ㍑ⓗ L ್ࡢప࠸(<3㸧ほ Ⅼ࣌ ࢆࡗ࡚࠸ࡿࡓࡵࠊᴟᏊ☢ሙࣔࢹࣝࢆ⏝ࡋ࡚࠸ࡿࠋSinger et al. [10] ࡼࡿࠊL<5 ࡛ࡣࠊ ᴟᏊࡣẚ㍑ⓗⰋ࠸㏆ఝ࡛࠶ࡾࠊࢺࣟࢲ࣮ࣝࣔࢻࡢඹ㬆࿘Ἴᩘ࠾ࡅࡿㄗᕪࡣ 10 %௨ୗ࡛࠶ࡿࠋ. ࣉࣛࢬ࣐ᐦᗘศᕸࣔࢹࣝࡢ㑅ᢥ FLR Ἴື᪉⛬ᘧࢆゎࡃࡣ☢ຊ⥺ἢ࠸ࡢࣉࣛࢬ࣐ᐦᗘศᕸࣉࣟࣇࣝࡶᚲせ࡛࠶ࡾࠊࡇࢀࡶ ࣔࢹࣝࡽ࠼ࡿࠋᮏ◊✲࡛ࡣᆅ⌫୰ᚰࡽࡢ㊥㞳㸸r ࡘ࠸࡚ᐦᗘࡀɏ ൌ ɏ ି ݎ ࡛ኚࡍࡿᣦᩘ 㛵ᩘࣔࢹࣝࢆ⏝࠸ࡓࠋɏࡣ௵ពࡢⅬ࠾ࡅࡿࣉࣛࢬ࣐㉁㔞ᐦᗘࠊɏ ࡣ☢Ẽᅪ㉥㐨㠃࠾ࡅࡿࣉࣛ ࢬ࣐㉁㔞ᐦᗘ࡛࠶ࡿࠋᣦᩘ m ࡣ Takahashi et al. [11] ࡢᥦࡍࡿ-1㹼0 ᇶ࡙ࡁࠊm=-1 ࢆ᥇⏝ࡋࡓࠋ. .
(5) )/5 Ἴື᪉⛬ᘧࢆゎࡃ ᭱ᚋ FLR Ἴື᪉⛬ᘧࢆゎࡁࠊほ ୍⮴ࡍࡿඹ㬆࿘Ἴᩘࢆ࠼ࡿࣉࣛࢬ࣐ᐦᗘࢆィ⟬ࡍࡿࠋ ᮏ◊✲࡛ࡣἼື᪉⛬ᘧࢆゎࡃ௦ࢃࡾࠊࢺࣟࢲ࣮ࣝࣔࢻᅛ᭷࿘ᮇࡢ㏆ఝᘧࢆ⏝࠸ࡓ[12]ࠋࡇࡢ㏆ ఝᘧࡼࡿㄗᕪࡣࠊL = 2.66 ࡛ 0.9 %ぢ✚ࡶࡽࢀ࡚࠸ࡿ[12]ࠋ2001 ᖺ 4 ᭶ 27 ᪥ 17:30-18:30 UT ࠾ࡅࡿ CLK-MSH ࡢඹ㬆࿘Ἴᩘ 14.5±0.2 mHz ᑐᛂࡍࡿ㉥㐨㠃ࣉࣛࢬ࣐㉁㔞ᐦᗘࡣ 1360±40 amu/cc ࡛࠶ࡗࡓࠋ. 㸬ゎᯒ⤖ᯝ ゎᯒᮇ㛫ࡢᏱᐂኳẼᴫἣ ᮏ◊✲࡛ࡣ 2001 ᖺ 4 ᭶Ⓨ⏕ࡋࡓࡘࡢ☢Ẽᔒక࠺ࣉࣛࢬ࣐ᐦᗘኚࢆㄪࡿࡓࡵࠊ4 ᭶ 20 ᪥ࡽ 5 ᭶ 6 ᪥ࡢ 17 ᪥㛫⡿㝣ࡢ୰⦋ᗘᖏ࡛ほ ࡉࢀࡓᆅ☢Ẽࢹ࣮ࢱࢆゎᯒࡋࡓࠋᅗ 2 ࡣヱᙜᮇ㛫ࡢᏱᐂኳẼᴫἣࢆ♧ࡍࢹ࣮ࢱ࡛࠶ࡿࠋୖࡽኴ㝧㢼ࡢࣉࣟࢺࣥᐦᗘ(a)ࠊኴ㝧㢼㏿ᗘ(b)ࠊ ᝨᫍ㛫✵㛫☢ሙ (Interplanetary Magnetic Field: IMF) ᙉᗘ(c)ࠊᝨᫍ㛫✵㛫☢ሙ༡ᡂศ (IMF_Bzࠊ ྥࡁࡀṇ) (d)ࠊDst ᣦᩘ(e)ࢆ♧ࡍࠋᶓ㍈ࡣ᪥࡛┠┒ࡣ UT ࡢ 0 ࢆ♧ࡍࠋ 4 ᭶ 21 ᪥ᚋ༙ࠊኴ㝧㢼ࣉࣟࢺࣥᐦᗘ IMF ᙉᗘࡀᛴ⃭ୖ᪼ࡋࠊ⥆࠸࡚ IMF_Bz ࡣࡁࡃ㈇᪉ ྥࢀࠊ30 㛫<-10~-5 nT ࢆಖᣢࡋࡓࠋࡇࡢࡼ࠺࡞ኚࡣ㧗㏿ኴ㝧㢼ࡢ๓㠃⏕ࡌࡿᅽ⦰ 㡿ᇦᆺⓗࡔࡀࡇࡢ࣋ࣥࢺ࡛ࡣኴ㝧㢼㏿ᗘࡣ 400~300 km/s ࡛⤊ጞࡋ࡚࠾ࡾࠊ㧗㏿ኴ㝧㢼ࡢ฿ 㐩ࡣ☜ㄆࡉࢀ࡞ࡗࡓࠋኴ㝧㢼ࡣప㏿࡛࠶ࡗࡓࡀࠊIMF_Bz ࡀ༡ྥࡁ࡞ࡗࡓࡇ࡛☢Ẽᅪෆࡢᑐ ὶࢆᘬࡁ㉳ࡇࡋࡓࡢ࡛࠶ࢁ࠺ࠋ☢Ẽᔒࡢᣦᶆ࡛࠶ࡿ Dst ᣦᩘࡀ 21 ᪥ 23 ௨㝆ᛴ⃭ୗࡀࡾጞࡵࠊ. ᅗ 1 2001 ᖺ 4 ᭶ 27 ᪥ 17㸸30 -18㸸30 UT CLK – MSH ࡛ほ ࡉࢀࡓ ᆅ☢Ẽኚື༡ᡂศࡢࢫ࣌ࢡࢺࣝゎᯒ⤖ᯝ. .
(6) 22 ᪥ 16 ࡣ-102 nT 㐩ࡋࡓࠋࡇࡢࡇࡽ 21 ᪥ 23 ࡽ☢ẼᔒࡀⓎ⏕ࡋ࡚࠾ࡾ 22 ᪥ 16 ࡲ࡛ࡀ┦ࠊࡑࢀ௨㝆ࡢᩘ᪥㛫ࡀᅇ┦ㄞࡳྲྀࢀࡿࠋࡇࡢ☢Ẽᔒࢆ౽ᐅୖࠕ☢Ẽᔒ㸯ࠖࡋࡓࠋ 23 ᪥ᚋ༙ࡽ 27 ᪥ࡲ࡛ࡢ㛫ࠊIMF_Bz ࡣᴫࡡ 0~5nT ࡢ㛫࡛᥎⛣ࡋ࡚࠾ࡾࠊ☢Ẽᔒ㸯ࡣ✜ࡸᅇ ࡋ࡚࠸ࡗࡓࠋ 28 ᪥ධࡿࡧኴ㝧㢼ࡢᨐࡀ฿㐩ࡍࡿࠋࡇࡢࡁࡣኴ㝧㢼ࣉࣟࢺࣥᐦᗘࠊIMF ᙉᗘࠊኴ㝧 㢼㏿ᗘࡍ࡚ࡀᛴቑࡋࠊᆺⓗ࡞㧗㏿ኴ㝧㢼ࡼࡿᅽ⦰ᵓ㐀ࡢ≉ᚩࢆ♧ࡋ࡚࠸ࡿࠋ୍᪉ IMF_Bz ࡣࡣࡌࡵྥࡁᡂศࢆ♧ࡋࠊࡢࡕ༡ྥࡁ㌿ࡌࡓࠋࡑࡢࡓࡵ Dst ᣦᩘࡣ 28 ᪥ 2 ௨㝆୍ⓗ ୖ᪼ࡋ࡚ 28 ᪥ 6 41nT 㐩ࡋࠊࡑࡢᚋᛴῶࡋ࡚ 29 ᪥ 4 -47nT 㐩ࡋࡓࠋࡇࡢࡇࡽࡲ ࡎኴ㝧㢼ືᅽࡢ㧗ࡲࡾࡼࡗ࡚☢Ẽᅪ๓㠃ࡀᅽ⦰ࡉࢀࠊ28 ᪥ 6 ࡽ 29 ᪥ 4 ࡀ☢Ẽᔒࡢ┦ࠊ ࡑࡢ࠶ࢆᅇ┦ㄞࡳྲྀࡿࡇࡀ࡛ࡁࡿࠋࡇࡢ☢Ẽᔒࢆࠕ☢Ẽᔒ 2ࠖࡋࡓࠋ. ᅗ 2 4 ᭶ 20 ᪥ࡽ 5 ᭶ 6 ᪥ࡢኴ㝧㢼ࣉࣟࢺࣥᐦᗘ(a), ኴ㝧㢼㏿ᗘ(b), IMF ᙉᗘ(c), IMF ༡ᡂศ(d), Dst ᣦᩘ(e). .
(7) ࣉࣛࢬ࣐ᐦᗘࡢ᪥᪥ኚ ᅗ 3 ࡣ MSH-ALPࠊCLK-MSH ࡢࢹ࣮ࢱࡽồࡵࡓ 2001 ᖺ 4 ᭶ 20 ᪥ࡽ 5 ᭶ 6 ᪥ࡢࣉࣛࢬ࣐㉁ 㔞ᐦᗘ࡛࠶ࡿࠋࡑࢀࡒࢀ L=2.6 (a) L=2.9 (b) ࡢ☢Ẽᅪ㉥㐨㠃࠾ࡅࡿ್┦ᙜࡍࡿࠋࢹ࣮ࢱࡢ ศᕸ೫ࡾࡀ࠶ࡿࡢࡣᢡࠊ☢ຊ⥺ඹ㬆ືࡢ᳨ฟࡀᅔ㞴࡞ࡿࡓࡵ࡛࠶ࡿࠋࡓ࠼ࡤ㟁㞳ᒙ㟁 ᑟᗘࡀప࠸ኪ㛫ࡣ☢ຊ⥺ඹ㬆ືࡢῶ⾶ࡀᙉࡃࠊ᳨ฟࡀᅔ㞴࡞ࡿࠋࡲࡓࠊᆅ☢Ẽኚື☢Ẽᅪ ᨐᡂศࡀ༟㉺ࡋࡓሙྜࠊ㏫☢Ẽᅪ⎔ቃࡀ㟼✜㐣ࡂ࡚⬦ືࡢ࢚ࢿࣝࢠ࣮※ࡀᙅࡍࡂࡿሙྜࠊ☢ ຊ⥺ඹ㬆㡿ᇦࡢᖜࡀほ Ⅼ࣌㛫ࡢ㊥㞳ᖜ␗࡞ࡿሙྜ࡞ࡣࠊഃ࡛ࡶ᳨ฟࡀᅔ㞴࡞ ࡿࠋ ࡣࡌࡵࡢᩘ᪥㛫ࠊࣉࣛࢬ࣐ᐦᗘࡣ⣙ 2000~2500 amu/cc (L=2.6)ࠊ1000~1300 amu/cc (L=2.9) ࡛ つ๎᥎⛣ࡋ࡚࠸ࡿࠋ25 ᪥ධࡿ☢Ẽᔒ 1 ࡢ㛤ጞక࠸ࣉࣛࢬ࣐ᐦᗘࡀࢃࡎୗࡀࡿࡀࠊ L=2.9 ࡛ࡶ 800amu/cc ࢆୗᅇࡿࡇࡣ࡞ࡃࠊ࡞ᾐ㣗ࡣ㉳ࡇࡽ࡞ࡗࡓࡳࡽࢀࡿࠋ25 ᪥ࡽ 27 ᪥ࡲ࡛ࡣ᪥୰ࡢᐦᗘୖ᪼ࠊኪ㛫ほ ࡀྍ⬟࡞㛫ᖏࡢᐦᗘపୗࢆ⧞ࡾ㏉ࡍࠋࡑࡋ࡚ 28 ᪥ ࡢ᪥୰ࣉࣛࢬ࣐ᐦᗘࡣᛴ⃭ୖ᪼ࡋࠊࡑࢀ௨㝆ᐦᗘࡢ㧗࠸≧ែࡀಖࡓࢀࡿࠋࡍ࡞ࢃࡕ☢Ẽᔒ㸯ࡢ ᅇ┦ᚋᮇࡽ㐃⥆ⓗ࡞ᐦᗘୖ᪼ࡀ⾲ࢀጞࡵࠊ☢Ẽᔒ㸰ࡢ┦ྜࢃࡏ࡚ᛴ⃭࡞ᐦᗘୖ᪼ࡀ㉳ࡇ ࡗ࡚࠸ࡓࠋࡇࡢ࣋ࣥࢺ࡛ࡣ☢Ẽᔒక࠺୍⯡ⓗ࡞ࣉࣛࢬ࣐ᐦᗘࡢኚືࡣࡃ␗࡞ࡿኚࡀほ ࡉࢀࡓゝ࠼ࡿࠋ. ᅗ 3 4 ᭶ 20 ᪥ࡽ 5 ᭶ 6 ᪥ࡢ L=2.6 (a) L=2.9 (b)࠾ࡅࡿࣉࣛࢬ࣐㉁㔞ᐦᗘ. .
(8) (a)MSHͲ APL(L=2.6). plasmamassdensity(amu/cc). 6000 5000 4000 3000 2000. y=473.3xͲ 5276.2 R²=0.954. 1000 0. 10. 14. 18. 22. UT (hour) (b)CLKͲ MSH(L=2.9). plasmamassdensity(amu/cc). 2500 2000 1500 1000. y=118.4xͲ 8.1 R²=0.870. 500 0. 10. 14. 18 UT (hour). 22. ᅗ 4 4 ᭶ 28 ᪥ࡢ L=2.6 (a) L=2.9 (b)࠾ࡅࡿࣉࣛࢬ࣐㉁㔞ᐦᗘࡢ㛫ኚ. .
(9) ࣉࣛࢬ࣐ᐦᗘࡢ༢㛫ᙜࡓࡾኚ㔞 ḟ 4 ᭶ 25㸫28 ᪥ࡢ༢㛫ᙜࡓࡾࡢࣉࣛࢬ࣐ᐦᗘୖ᪼⋡ࢆィ⟬ࡋࡓࠋᅗ 4 ࡣ 4 ᭶ 28 ᪥ࡢ L=2.6 (a) L=2.9 (b) ࠾ࡅࡿࣉࣛࢬ࣐ᐦᗘࡢ㛫ኚࢆ♧ࡋ࡚࠸ࡿࠋᅗ୰ࡢ┤⥺ࡣࢹ࣮ࢱ᭱ࡶࡼࡃ ୍⮴ࡍࡿ┤⥺ࢆ᭱ᑠἲࡼࡾồࡵࡓࡶࡢ࡛ࠊࡑࡢഴࡁࡽ 1 㛫࠶ࡓࡾࡢࣉࣛࢬ࣐ᐦᗘቑຍ 㔞ࡣ L=2.6 ࡛ 473 amu/cc/hourࠊL=2.9 ࡛ 118 amu/cc/hour ⟬ฟࡉࢀࡓࠋྠᵝࡢゎᯒࢆ 4 ᭶ 25 ᪥~27 ᪥ࡢྛࢹ࣮ࢱࡘ࠸࡚ࡶ⾜ࡗࡓ⤖ᯝࢆ⾲ 2 ♧ࡍࠋẚ㍑ࡢࡓࡵࠊ㐣ཤࡢࢹ࣮ࢱゎᯒ◊✲ࡢ⤖ᯝࡶ ྜࢃࡏ࡚ᥖ㍕ࡋ࡚࠸ࡿࠋᮏ◊✲ࡼࡿ 2001 ᖺ 4 ᭶ 28 ᪥ࡢほ ௨እࡣ࠸ࡎࢀࡶ☢Ẽᔒࡀᅇ┦ ධࡗࡓ┤ᚋ 1~3 ᪥ࡢᐦᗘୖ᪼ࢆㄪࡓࡶࡢ࡛࠶ࡿࠋᡃࠎࡢ⤖ᯝࡶྵࡵࠊࢇࡢゎᯒ⤖ᯝ࡛ྠ ୍࣋ࣥࢺෆ࡛ࡣ L ್ࡢᑠࡉ࠸࠺ࡀ༢㛫ᙜࡓࡾࡢᐦᗘୖ᪼⋡ࡀࡁ࠸ࠋࡇࢀࡣ L ್ࡀࡁ ࠸☢᮰⟶㛗ࡃࠊ㟁㞳ᅪ࠾ࡅࡿ༢㠃✚ᙜࡓࡾࡢయ✚ࡶࡁࡃ࡞ࡿࡓࡵ⪃࠼ࡽࢀࡿ[14]ࠋ ࡲࡓࠊᅇゎᯒࡋࡓ⤖ᯝࡢ࠺ࡕ 4 ᭶ 25 ᪥㹼27 ᪥ࡢᐦᗘୖ᪼⋡ࡣ㐣ཤࡢゎᯒ⤖ᯝྠ⛬ᗘࡢ ࡁࡉ࡛࠶ࡗࡓࡢᑐࡋࠊ4 ᭶ 28 ᪥ࡢᐦᗘୖ᪼⋡ࡣ✺ฟࡋ࡚ࡁࡗࡓࠋ2001 ᖺ 6 ᭶ 19 ᪥ࡢᐦᗘ ኚࡶྠ⛬ᗘࡁ࠸ࡀࡇࡢ࣋ࣥࢺ࡛ࡣ L ್ࡢࡁ࠸ほ Ⅼ࡛ࡼࡾ㧗࠸ୖ᪼⋡ࡀぢࡽࢀࠊ㏻ᖖ ࡣ㐪ࡗࡓᐦᗘୖ࣓᪼࢝ࢽࢬ࣒ࡀാ࠸࡚࠸ࡓࡢࡶࡋࢀ࡞࠸ࠋ. ⾲ 2 ࣉࣛࢬ࣐ᐦᗘࡢ༢㛫ᙜࡓࡾኚ㔞 Source and Date. Increasing Rate of Plasma Mass Density. [amu/cc/hour]. L=2.0. L=2.3. L=2.6. L=3.1. L=3.3. L=3.8. 25 Apr 2001. -. -. 181. 40. -. -. -. 26 Apr 2001. -. -. 52. 33. -. -. -. 27 Apr 2001. -. -. 79. 58. -. -. -. 28 Apr 2001. -. -. 473. 118. -. -. -. 200. -. -. -. -. -. -. 11 Mar 2004. -. 248. 110. -. -. 25 Apr 2001. -. -. -. 27. 19. -. -. 26 Apr 2001. -. -. -. 32. 23. -. -. 18 Jun 2001. -. -. -. 46. 70. -. -. 19 Jun 2001. -. -. -. 98. 106. -. -. L=2.9. Our Observation. Chi et al., 2000 25 Sep 1998 Obana et al., 2010. . 39. 13.
(10) 㸬⪃ᐹ. ᮏ◊✲ࡢゎᯒ⤖ᯝࡽࠊ☢Ẽᔒ㸰ࡢ┦ᮇ㛫࠶ࡓࡿ 4 ᭶ 28 ᪥✺ฟࡋ࡚ࡁ࡞ࣉࣛࢬ࣐ᐦᗘ ୖ᪼⋡ࡀほ ࡉࢀࡓࠋࡋࡋࡣࡌࡵ㏙ࡓࡼ࠺ࠊ☢Ẽᅪᑐὶࡢᾘ㛗㐃ືࡋ࡚㉳ࡇࡿࣉࣛࢬ ࣐ᅪࡢᐦᗘኚືࡣ㏻ᖖࠊᑐὶࡢⓎ㐩ࡶᐦᗘపୗࢆ㉳ࡇࡍࠋᮏ◊✲ࡢゎᯒᮇ㛫ᖖࡣ㏫ࡢ ᐦᗘኚࡀ㉳ࡇࡗ࡚࠸ࡓ⌮⏤ࢆ⪃ᐹࡍࡿࠋ. ኴ㝧㢼ືᅽࡢᛴቑࡼࡿ☢Ẽᅪ๓㠃ࡢᅽ⦰ ᅗ 2 ࡛♧ࡋࡓࡼ࠺ 28 ᪥ࡢࡣࡌࡵࠊኴ㝧㢼ࡢᐦᗘ࣭㏿ᗘࡀᛴ⃭ୖ᪼ࡋ࡚࠸ࡿࠋࡇࢀࡼࡾື ᅽࡀᛴቑࡋ☢Ẽᅪ๓㠃ࡀᅽ⦰ࡉࢀࡓ⪃࠼ࡽࢀࡿࠋᐇ㝿 Dst ᣦᩘࡶ 40 nT ࡢᛴ⃭࡞ୖ᪼ࡀほ ࡉࢀ࡚࠾ࡾࠊࡇࡢᅽ⦰ࡢᙳ㡪࡛ഃࣉࣛࢬ࣐ᅪࡶᅽ⦰ࡉࢀᐦᗘࡢᛴୖ᪼ࡀ㉳ࡇࡗࡓࡢࡶࡋࢀ࡞ ࠸ࠋࡋࡋኴ㝧㢼ືᅽኚࡀ L=2~3 ࡢ῝ෆ㒊☢Ẽᅪࡲ࡛ᅽ⦰ࡋࡓ⪃࠼ࡿࡢࡣ㞴ࡋ࠸ࠋࡲࡓ ᅽ⦰㐣⛬ࡢ⤊ᚋࡣࣉࣛࢬ࣐ᐦᗘࡣ㧗Ṇࡲࡾࡍࡿ⪃࠼ࡽࢀࡿࡀࠊᐇ㝿ࡣ Dst ᣦᩘࡢ❧ࡕୖࡀ ࡾᚋ 20 㛫௨ୖࢃࡓࡗ࡚⥅⥆ⓗᐦᗘୖ᪼ࡀほ ࡉࢀ࡚࠾ࡾࠊࡇࢀࢆㄝ᫂ࡍࡿࡢࡣ㞴ࡋ࠸ࡶ ࡋࢀ࡞࠸ࠋ. ᑐὶࡼࡿኪഃࡽࡢࣉࣛࢬ࣐ὶධ ☢Ẽᅪᑐὶࡣ☢Ẽᅪᑿ㒊ࡽഃྥࡅ࡚つᶍ࡞ࣉࣛࢬ࣐☢᮰⟶ࡢ㐠ືࢆᘬࡁ㉳ࡇࡍࡢ࡛ࠊ ࣉࣛࢬ࣐ᅪᾐ㣗ࡢึᮇẁ㝵࡛ኪഃࡢࣉࣛࢬ࣐ᅪ⏺㠃ࡀෆഃධࡾ㎸ࡴࠋࡇࡢࡇࡣほ ࡽࡶ☜ ࡵࡽࢀ࡚࠸ࡿࡀ[15]ࠊഃ᪉ྥ⛣㏦ࡉࢀࡓࣉࣛࢬ࣐ࡀࡑࡢᚋࡇࡽࡢࡼ࠺ᾘ㈝ࡉࢀࡿࡢ ࠊ࠸ࡲࡔ᫂ࡽࡣ࡞ࡗ࡚࠸࡞࠸ࠋᮏ◊✲࡛ほ ࡉࢀࡓ 4 ᭶ 28 ᪥ࡢࣉࣛࢬ࣐ᐦᗘୖ᪼ࡣࠊኪഃ ࡽࡢࣉࣛࢬ࣐ࡢ㍺㏦ࡼࡿࡶࡢࡶࡋࢀ࡞࠸ࠋIMF ࡢ༡ྥࡁᡂศ Dst ᣦᩘࠊࡕࡽࡢᣦᶆࡶ ☢Ẽᅪᑐὶࡀᑡ࡞ࡃࡶ 29 ᪥ࡢึࡵࡈࢁࡲ࡛ࡣ⥅⥆ࡋ࡚࠸ࡓࡇࢆ♧ࡋ࡚࠾ࡾࠊ⥅⥆ⓗ࡞ࣉࣛࢬ ࣐౪⤥ࡀྍ⬟࡛࠶ࡗࡓࡇࢆ♧၀ࡋ࡚࠸ࡿࠋࡋࡋ࡞ࡀࡽࠊࡇࡢࣔࢹ࡛ࣝࡣᮅ᪉ࡸኤ᪉㡿ᇦࡢ ࣉࣛࢬ࣐౪⤥ࡣᐜ࡛᫆࠶ࡿࡀࠊṇ༗㏆ࡢ㡿ᇦ౪⤥ࡍࡿࡢࡣ㞴ࡋ࠸ࡶࡋࢀ࡞࠸ࠋᚋࣔࢹࣝ ィ⟬➼ࢆ⾜ࡗ࡚☜ㄆࡍࡿᚲせࡀ࠶ࡿࡔࢁ࠺ࠋ. ᑐὶࡼࡿඹᅇ㌿㏿ᗘࡢ㐜ᘏ ☢Ẽᅪᑐὶࡢቑࡼࡿࡶ࠺ࡦࡘࡢᙳ㡪ࡋ࡚ࠊ༗ᚋഃ࠾ࡅࡿ☢᮰⟶ࡢඹᅇ㌿ࡢ㐜ᘏࢆ⪃ ࠼ࡿࠋ☢Ẽᅪෆࡢ☢᮰⟶ࡢ㐠ືࡣ☢Ẽᅪᑐὶ㟁ሙඹᅇ㌿㟁ሙࡢ㔜ࡡྜࢃࡏ࡛⏕ࡲࢀࡿ㟁ሙᨭ 㓄ࡉࢀࠊඹᅇ㌿ࡀᨭ㓄ⓗ࡞ࣉࣛࢬ࣐ᅪෆ࠾࠸࡚ࡶ☢᮰⟶ࡢᅇ㌿㏿ᗘࡣ 10㸣⛬ᗘඹᅇ㌿ࡽ㐜ࢀ ࡚࠸ࡿ[16]ࠋ☢Ẽᅪᑐὶࡣ༗ᚋഃࡢඹᅇ㌿ࢆጉࡆࡿ᪉ྥാࡃࡢ࡛ࠊᑐὶࡀᙉࡲࢀࡤࡇࡢ㐜ᘏࡣࡉ. .
(11) ࡽቑࡍࡿࠋࡑࡢ⤖ᯝࠊ༗ᚋഃ࡛ࡣᆅୖࡢࠕᐃⅬほ ࡛ࠖᮾഃࡽࡎࢀ࡚ࡁࡓ☢᮰⟶ࢆほ ࡋ ࡚࠸ࡿࡇ࡞ࡾࠊ㟁㞳ᅪࡽࡢࣉࣛࢬ࣐౪⤥㔞ࡀ୍ᐃ࡛ࡶࣉࣛࢬ࣐ᐦᗘୖ᪼⋡ࡀぢࡅୖࠊୖ ᪼ࡍࡿ⪃࠼ࡽࢀࡿࠋ. ᚋࡢㄢ㢟 4 ᭶ 28 ᪥ࡢࣉࣛࢬ࣐ᐦᗘ␗ᖖୖ᪼ࢆᐃᛶⓗㄝ᫂ࡍࡿ࠸ࡃࡘࡢࣔࢹࣝࢆ⪃ᐹࡋࡓࠋࡍ࡛㏙ ࡓࡼ࠺ࠊ࠸ࡎࢀ୍ࡘࡢࣔࢹ࡛ࣝ༑ᩘ㛫ࢃࡓࡗ࡚⥅⥆ࡉࢀࡓᐦᗘୖ᪼ࢆㄝ᫂ࡍࡿࡢࡣ㞴 ࡋࡃࠊ࠸ࡃࡘࡢ࣓࢝ࢽࢬ࣒ࡢ」ྜ⪃࠼ࡓ࠺ࡀࡼ࠸ࡶࡋࢀ࡞࠸ࠋᚋࡢ⤒ᗘ⥺ࡢほ ࢹ࣮ࢱࡸ㟁Ꮚᐦᗘኚ➼ẚ㍑ࡋ࡚⌫ⓗ࡞ᐦᗘኚࢆㄪࡿᚲせࡀ࠶ࢁ࠺ࠋ ࡲࡓࠊኪഃࣉࣛࢬ࣐ᅪ⏺㠃ࡢ⛣ືࡸ༗ᚋഃ࡛ࡢඹᅇ㌿㐜ᘏࡣࠊࣉࣛࢬ࣐ᅪᾐ㣗ᮇ࠾ࡅࡿࣉࣛ ࢬ࣐ὶኻ㐣⛬ࢆ⪃࠼ࡿୖ࡛㔜せ࡛ࠊኪഃࡢࣉࣛࢬ࣐ࡀࡇࡲ࡛㐩ࡋࠊࡑࡢᚋࡇࡽࡢࡼ࠺ ὶฟࡍࡿࡢ࠸ࡲࡔ᫂ࡽ࡞ࡗ࡚࠸࡞࠸ࠋᡃࠎࡢゎᯒ⤖ᯝࡣኪഃࡢࣉࣛࢬ࣐ࡀഃ୍᪦྿ࡁ ᐤࡏࡽࢀ࡚࠸ࡿࡇࢆ♧၀ࡋ࡚࠸ࡿࠋࡉࡽ 29 ᪥௨㝆ࣉࣛࢬ࣐ᐦᗘࡀ㧗Ṇࡲࡾࡋ࡚࠸ࡿࡇࡽࠊ ὶฟ࣓࢝ࢽࢬ࣒ࡀసືࡍࡿࡓࡵࡣఱࡽࡢ᮲௳ࡸ㜈್ࡀ࠶ࡾࠊࡇࡢ࣋ࣥࢺ࡛ࡣసືࡋ࡞ࡗ ࡓྍ⬟ᛶࡶ♧၀ࡋ࡚࠸ࡿࠋ☢Ẽᔒ㸰ࡣ Dst ᣦᩘࡢ᭱ᑠ್ࡀ ̺47nT ‶ࡓ࡞࠸ᑠつᶍ࡞☢Ẽᔒ࡛ ࠶ࡿࡇࡀ㛵ಀࡋ࡚࠸ࡓࡢࡶࡋࢀ࡞࠸ࠋᚋࡉࡽゎᯒࢆቑࡸࡋࠊ᫂ࡽࡍࡿࡁㄢ㢟࡛ ࠶ࡿࠋ. 㸬ࡲࡵ 2001 ᖺ 4 ᭶ 20 ᪥ࡽ 5 ᭶ 6 ᪥⡿㝣ࡢ୰⦋ᗘᖏ࡛ほ ࡉࢀࡓᆅ☢Ẽࢹ࣮ࢱࢆゎᯒࡋ L=2.6, 2.9 ࡢ☢᮰⟶࠾ࡅࡿ 17 ᪥㛫ࡢࣉࣛࢬ࣐ᐦᗘኚࢆㄪࡓࠋࡇࡢᮇ㛫ࡣ 4 ᭶ 21 ᪥ 28 ᪥ ࡘࡢ☢ẼᔒࡀⓎ⏕ࡋ࡚࠸ࡿࠋ୍ࡘ┠ࡢ☢Ẽᔒ࡛ࡣࣉࣛࢬ࣐ᐦᗘࡣࢃࡎῶᑡࡋࠊᅇ┦㛤ጞ 4 ᪥┠ࡽሸࡳࡽࢀࡿ㐃⥆ⓗ࡞ᐦᗘୖ᪼ࡀぢࡽࢀࡓࠋᖹᆒⓗ࡞ᐦᗘୖ᪼⋡ࡣ L=2.6 ࡛ 50~180 amu/cc/hࠊL=2.9 ࡛ 30~60 amu/cc/h ࡛࠶ࡗࡓࠋࡇࢀࡣ㐣ཤほ ࡉࢀࡓ☢Ẽᅪᅇ┦࠾ࡅࡿࣉࣛ ࢬ࣐ᅪሸ⋡ࡰ୍⮴ࡍࡿࠋ୍᪉ 4 ᭶ 28 ᪥ጞࡲࡗࡓ☢Ẽᔒ࡛ࡣࣉࣛࢬ࣐ᐦᗘࡢῶᑡࡣぢࡽ ࢀࡎࠊ㏫ 28 ᪥ᛴ⃭࡞ࣉࣛࢬ࣐ᐦᗘࡢୖ᪼ࡀほ ࡉࢀࡓࠋࣉࣛࢬ࣐ᐦᗘୖ᪼⋡ࡣ L=2.6 ࡛ 473 amu/cc/hࠊL=2.9 ࡛ 118 amu/cc/h 㐩ࡋ࡚࠾ࡾࠊ㐣ཤࡢ◊✲ẚ㍑ࡋ࡚ࡶ✺ฟࡋ࡚㧗࠸ୖ᪼⋡࡛࠶ ࡗࡓࠋ ☢Ẽᔒ㛤ጞᚋ␗ᖖ㧗࠸ࣉࣛࢬ࣐ᐦᗘୖ᪼ࡀ⏕ࡌࡓ⌮⏤ࢆ⪃࠼ࡿࡓࡵࠊኴ㝧㢼ືᅽࡢᛴቑ ࡼࡿ☢Ẽᅪ๓㠃ࡢᅽ⦰ࠊᑐὶࡼࡿኪഃࡽࡢࣉࣛࢬ࣐ὶධࠊᑐὶࡼࡿඹᅇ㌿㏿ᗘࡢ㐜ᘏࡢ 3 ࡘࡢࣔࢹࣝࢆ⪃ᐹࡋࡓࠋኪഃࡽࡢࣉࣛࢬ࣐ὶධඹᅇ㌿㏿ᗘࡢ㐜ᘏࡣࠊᐦᗘୖ᪼ࡀ༑ᩘ㛫 ⥅⥆ⓗ⥆࠸ࡓࡇࢆᐃᛶⓗࡼࡃㄝ࡛᫂ࡁࡿࠋᅇᚓࡽࢀࡓ⤖ᯝࡣ☢Ẽᔒ㛤ጞᚋࠊኪഃࡽ ഃࣉࣛࢬ࣐ࡀ⛣㏦ࡉࢀࠊ༗ᚋഃ࡛ࡼࡳࢆᙧᡂࡋࡓࡇࢆ♧ࡋ࡚࠸ࡿࡢࡶࡋࢀ࡞࠸ࠋࡉࡽ. .
(12) ࡢ⤒ᗘ⥺ୖ࡛ࡶゎᯒࢆ㐍ࡵࠊ⌫ⓗ࡞ᐦᗘኚືࢆ᫂ࡽࡍࡿࡶࠊࣔࢹࣝィ⟬ࢆ⾜࠸ᩘ 㔞ⓗẚ㍑◊✲ࢆ⾜ࡗ࡚ࣉࣛࢬ࣐ᅪࡢᾐ㣗㐣⛬࠾ࡅࡿࣉࣛࢬ࣐ὶฟ⤒㊰ࢆゎ᫂ࡍࡿࡇࡀᚋࡢ ㄢ㢟࡛࠶ࡿࠋ. ㅰ㎡ ᮏ◊✲䛷⏝䛧䛯ᆅ☢Ẽ䝕䞊䝍䛿 㻹㻱㻭㻿㼁㻾㻱 ᆅ☢Ẽほ ⥙䛷ほ 䛥䜜䚸㼁㻯㻸㻭 ᆅ☢Ẽ䝕䞊䝍䝉䞁䝍䞊 䜢㏻䛨䛶౪⤥䛥䜜䜎䛧䛯䚹䝕䞊䝍䜢ᥦ౪䛔䛯䛰䛝䜎䛧䛯 㻹㼍㼞㼗㻌 㻹㼛㼘㼐㼣㼕㼚 ༤ኈ䛸䜹䝸䝣䜷䝹䝙䜰Ꮫ䝻䝃䞁䝊
(13) 䝹䝇ᰯᆅ⌫ᝨᫍ≀⌮Ꮫ◊✲ᡤ䛚䜘䜃ᆅ⌫Ᏹᐂ⛉Ꮫ⛉䛻ឤㅰ䛔䛯䛧䜎䛩䚹. ཧ⪃ᩥ⊩ [1] Park, C.G., “Whistler observation of the interchange of ionization between the ionosphere and the protonosphere”, J. of Geophys. Res., 75 (22), 4249-4260 (1970). [2] Chappell, C. R., K. K. Harris, and G. W. Sharp, “A Study of the Influence of Magnetic Activity on the Location of the Plasmapause as Measured by OGO 5”, J. of Geophys. Res., 75 (1), 50-56 (1970). [3] Nishida, A., “Formation of plasmapause, or magnetospheric plasma knee, by the combined action of magnetospheric convection and plasma escape from the tail”, J. Geophys. Res., 71, 5,669 (1966). [4] Park, C.G., “Some Features of Plasma Distribution in Plasmasphere Deduced from Antarctic Whistlers”, J. of Geophys. Res., 79 (1), 169-173 (1974). [5] Abe, T., B. A. Whalen, A. W. Yau, S. Watanabe, E. Sagawa, and K. I. Oyama, “Altitude profile of the polar wind velocity and its relationship to ionospheric conditions”, Geophysical Research Letters, 20(24), 2825-2828 (1993). [6] Krall, J., J. D. Huba, and J. A. Fedder, “Simulation of field-aligned H(+) and He(+) dynamics during late-stage plasmasphere refilling”, Annales Geophysicae, 26(6), 1507-1516 (2008). [7] Sugiura, M., and C. R. Wilson, “Oscillation of the Geomagnetic Field Lines and Associated Magnetic Perturbations at Conjugate Points”, J. of Geophys. Res., Vol. 69, pp.1211 (1964). [8] Baransky, L.N., Y.E. Borovkov, M.B. Gokhberg, and S.M. Krylov, “The Gradient-Method of Measuring the Resonance Frequencies of Magnetic-Field Lines”, Izvestiya Akademii Nauk Sssr Fizika Zemli (8), 74-91 (1985). [9] Waters, C.L., F.W. Menk, B.J. Fraser, and P.M. Ostwald, “Phase-Structure of Low-Latitude Pc3-4 Pulsations”, Planetary and Space Science, 39 (4), 569 (1991). [10] Singer, H.J., D.J. Southwood, R.J. Walker, and M.G. Kivelson, “Alfven wave resonances in a realistic magnetospheric magnetic field geometry”, J. of Geophys. Res., 86, 4589-4596 (1981). [11] Takahashi, K., R.E. Denton, R.R. Anderson, and W.J. Hughes, “Frequencies of standing Alfven wave harmonics and their implication for plasma mass distribution along geomagnetic field lines: Statistical analysis of CRRES data”, J. of Geophys. Res.-Space Physics, 109 (A8) (2004). [12] Vellante, M., and M. Forster, “Inference of the magnetospheric plasma mass density from field line. .
(14) resonances: A test using a plasmasphere model”, J. of Geophys. Res.-Space Physics, 111 (A11) (2006). [13] Chi, P.J., C.T. Russell, S. Musman, W.K. Peterson, G. Le, V. Angelopoulos, G.D. Reeves, M.B. Moldwin, and F.K. Chun, “Plasmaspheric depletion and refilling associated with the September 25, 1998 magnetic storm observed by ground magnetometers at L=2”, Geophysical Research Letters, 27 (5), 633-636 (2000). [14] Obana, Y., F. W. Menk, and I. Yoshikawa, “Plasma refilling rates for L=2.3-3.8 flux tubes”, J. of Geophys. Res.-Space Physics, 115, A03204, doi:10.1029/2009JAA014191 (2010). [15] Murakami, G., M. Hirai, and I. Yoshikawa, “The plasmapause response to the southward turning of the IMF derived from sequential EUV images”, J. of Geophys. Res.-Space Physics, 112(A6), 7 (2007). [16] Sandel, B. R., J. Goldstein, D. L. Gallagher, and M. Spasojevic, “Extreme Ultraviolet Imager observations of the structure and dynamics of the plasmasphere”, Space Science Reviews, 109(1-4), 25-46 (2003).. .
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