’˜ŽÒ |
”•\ŽÒ |
µ‘Ò u‰‰ |
u‰‰”Ô† |
ƒVƒ‡[ƒgƒ^ƒCƒgƒ‹ |
—\eW–{•¶ |
‹e’r ’ |
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R003-P008 |
The calculation of geomagnetically induced current by using FDTD method |
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R005-27 |
“ú–{‚É‚¨‚¯‚é“d—£Œ——’‚Ì’·ŠúŠÔ‰ðÍ |
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R006-P012 |
’nã-‰q¯“¯ŽžŠÏ‘ª‚É‚æ‚é‘å‹K–Íï—‚É”º‚¤“dê‚Ì”’BE“`”À‰ß’ö |
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R006-P018 |
Substorm electric fields at mid-latitudes and equatorial electrojets on the nightside |
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R010-08 |
Ž¥‹C—’Žž‚̃Oƒ[ƒoƒ‹‚È“d—£Œ—“d—¬•ª•z |
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# |
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R010-15 |
Ž¥‹CŒ—ˆ³k‚ɑ΂·‚é”ñˆ³k«“d—£Œ—‚̉ž“š|HF DopplerŠÏ‘ª| |
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‹e’r ”ŽŽj |
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R005-33 |
JEM-GLIMS‚É‚æ‚èŠÏ‘ª‚³‚ꂽƒXƒvƒ‰ƒCƒg‚Æ‚»‚ê‚É”º‚¤VHF‘Ñ“d”g‚Ì“Á’¥ |
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‹e’r ‰ës |
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R005-30 |
Imaging Observation of the Earth's Upper Atmosphere by ISS-IMAP |
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–k ˆí˜Y |
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R004-08 |
–k”¼‹…‚É‚¨‚¯‚é‘å‹K–Í‚È‘å—¤•X°”’B‘OŒã‚Ì[‘w…zŠÂ‚Ì•Ï‘J |
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–k Œ³ |
# |
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S001-07 |
“d”gŠ±ÂŒv‹y‚тЂ³‚«‰q¯‚ð—p‚¢‚½–د•úŽËü‘Ñ‹óŠÔ•Ï“®Œ»Û‚ÌlŽ@ |
•\Ž¦ |
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S001-P002 |
Jovian IR aurora observation with Hisaki/EXCEED: Comparison between K- and L-band auroras |
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S001-P003 |
Vertical emissivity profiles of Jovian northern H3+ and H2 infrared auroras |
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–kˆä —çŽO˜Y |
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* |
R010-04 |
‘¾—z‹É’[Ž‡ŠOü‚¨‚æ‚ÑÊ‘w‰æ‘œƒf[ƒ^‚ÉŠî‚ÂA‘¾—zŽ‡ŠOü•úŽË—Ê‚ÌŠˆ“®ŽüŠú•Ï“® |
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–kì •’ |
# |
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R009-P015 |
–دŽ¥‹CŒ—‚ÌŽ¥ê‚Ì“ì–kï—‚ÉŠÖ‚·‚錤‹† |
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–kì —Yˆê˜Y |
# |
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R008-P001 |
FLRŽü”g”Ž©“®ŒŸo‚ÆA‚»‚ê‚É‚æ‚鎥‹CŒ—ƒvƒ‰ƒYƒ}Ž¿—Ê–§“x‚̈ܓxŒo“x\‘¢‚Ì“Œv‰ðÍ |
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–Ø’J ‰À—² |
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R008-15 |
‚’¼ÕŒ‚”g‚É‚¨‚¯‚éÄŒ`¬‚Æ”÷Ž‹“I•sˆÀ’è« |
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–kê ˆçŽq |
# |
* |
R010-05 |
’nŽ¥‹CƒV[ƒ‹ƒh‚Í‹CŒó‚ð•Ï‚¦‚é‚©H@ƒXƒxƒ“ƒXƒ}ƒ‹ƒN‰¼à‚Ì’nŽ¿Šw“IŒŸØ‚ÆV“WŠJ |
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–kŒ´ —O |
# |
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R006-09 |
ƒR[ƒ‰ƒX•úŽË‚É‚æ‚邃Gƒlƒ‹ƒM[“dŽq‚̃sƒbƒ`ŠpŽU—‰ß’ö‚Ì’è—Ê•]‰¿‚ɂ‚¢‚Ä |
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–kŒ´ —D |
# |
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R004-11 |
“©—WŽŽ—¿‚æ‚脒肳‚ê‚é5`9¢‹I‚̼“ú–{‚É‚¨‚¯‚élŒÃ’nŽ¥‹C‹“x |
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–k‘º Œ’‘¾˜Y |
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R006-13 |
IHM–@‚ÆAPGM–@‚ÌCARISMAEMAGDAS“¯ŽžŠÏ‘ªƒf[ƒ^‚Ö‚Ì“K—pFFLRƒpƒ‰ƒƒ^‚̈ܓxˆË‘¶« |
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R008-P001 |
FLRŽü”g”Ž©“®ŒŸo‚ÆA‚»‚ê‚É‚æ‚鎥‹CŒ—ƒvƒ‰ƒYƒ}Ž¿—Ê–§“x‚̈ܓxŒo“x\‘¢‚Ì“Œv‰ðÍ |
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–k‘º ¬Žõ |
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R006-04 |
ƒvƒ‰ƒYƒ}Œ—EMIC”g“®‚Ì“Œv‰ðÍ |
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# |
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R006-22 |
“d—£Œ—‚ւ̃Gƒlƒ‹ƒM[—¬“ü‚ÆŽ_‘fE…‘fƒCƒIƒ“—¬o‚Æ‚ÌŒoŒ±“IŠÖŒWŽ®‚Ì‘¾—z“V’¸ŠpˆË‘¶« |
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R006-24 |
‚ ‚¯‚ڂ̉q¯‚ÌPWSŠÏ‘ªƒf[ƒ^‚É‚æ‚éƒvƒ‰ƒYƒ}Œ—\‘¢‚Ì•Ï“®‚Ì“Œv‰ðÍ |
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–؉º •–ç |
# |
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R005-07 |
ƒ|[ƒJ[ƒtƒ‰ƒbƒg‹y‚уgƒƒ€ƒ\MFƒŒ[ƒ_[‚ÅŠÏ‘ª‚³‚ꂽ’†ŠÔŒ—d—Í”g“Á«‚ÉŠÖ‚·‚錤‹† |
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R005-P002 |
“~‹G–k‹Éˆæ’†ŠÔŒ—‚Ìï—ó‘Ô‚ðŽ¦‚·Žw•W‚ÌŒŸ“¢ |
•\Ž¦ |
–ØŒ´ ‘åé |
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R005-16 |
Recent Lithium release and future Barium release experiments from sounding rocket in cusp region |
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# |
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R005-P005 |
q‹ó‹@‚æ‚èŠÏ‘ª‚µ‚½’‹ŠÔ‰º•””MŒ—ƒŠƒ`ƒEƒ€‹¤–ÂŽU—Œõ‚©‚ç‚Ì•—‘¬ŽZo–@‚ÌŠJ” |
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–Ø‘º ˆ¨ |
# |
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R003-P008 |
The calculation of geomagnetically induced current by using FDTD method |
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–Ø‘º ’qŽ÷ |
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R009-P015 |
–دŽ¥‹CŒ—‚ÌŽ¥ê‚Ì“ì–kï—‚ÉŠÖ‚·‚錤‹† |
•\Ž¦ |
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R009-P017 |
The Radio & Plasma Wave Investigation (RPWI) for JUICE |
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* |
S001-01 |
The inward transportation of hot electron in the Jovian inner magnetosphere |
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S001-02 |
EXCEED‚É‚æ‚é–دŠÏ‘ª- ƒI[ƒƒ‰‚ÆIPT‚Ì‘Œõ‚Æ“®Œa•ûŒü‚̃Gƒlƒ‹ƒM[—A‘—- |
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S001-03 |
Local electron heating in the Io plasma torus associated with Io observed by HISAKI |
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# |
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S001-04 |
Multi-wavelength observations of Jovian aurora coordinated with Hisaki and other telescopes |
•\Ž¦ |
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S001-06 |
Solar wind influence on the dawn-dusk asymmetry of the Io plasma torus observed by HISAKI/EXCEED |
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* |
S001-09 |
–د–鑤Ž¥‹CŒ—‚É‚¨‚¯‚郊ƒRƒlƒNƒVƒ‡ƒ“‚Ì‚»‚ÌêŠÏ‘ª |
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S001-10 |
Oxygen torus in the inner magnetosphere of Saturn observed by Hisaki |
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S001-11 |
HISAKI/EXCEED‚ÅŠÏ‘ª‚³‚ꂽŽ¥‹C—’’†EƒWƒIƒRƒƒi‚ÌLyman-ƒ¿‚Ì‘Œõ |
•\Ž¦ |
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* |
S001-12 |
Hisaki/EXCEED observation of solar-wind-driven atmospheric escape from Venus |
•\Ž¦ |
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S001-13 |
Variations of the total oxygen ion content in the Venusian ionosphere controlled by the solar wind |
•\Ž¦ |
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S001-P001 |
‹à¯E‰Î¯ŠÏ‘ªŽž‚É‚¨‚¯‚éEXCEED‚ÌŒŸoŠí«”\‚̕ω»‚𓥂܂¦‚½ŽUˆí‘å‹C‚ÉŠÖ‚·‚é‰ðÍ |
•\Ž¦ |
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S001-P005 |
Variation characteristics of Jupiter's hectometric radiation during the HISAKI observation campaign |
•\Ž¦ |
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S001-P006 |
Hisaki‚É‚æ‚éEUV‹“x‹y‚Ñ’nãŠÏ‘ª‚É‚æ‚é–دƒfƒJƒ[ƒ^“d”g‚Ì”äŠr‰ðÍ |
•\Ž¦ |
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S001-P007 |
‚Ђ³‚«iSPRINT-Aj‰q¯‚̉^—p󋵂ɂ‚¢‚Ä |
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