2018
DOI: 10.1029/2018ja025514
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Cooperatives Roles of Dynamics and Topology in Generating the Magnetosphere‐Ionosphere Disturbances: Case of the Theta Aurora

Abstract: To understand the magnetosphere‐ionosphere (M‐I) disturbances, it is necessary to know the change in the null‐separator structure along with the development of convection. The present paper explains this proposition by taking the case of the theta aurora that occurs after the switch of interplanetary magnetic field By and reveals auroral development inside the polar cap. The interplanetary magnetic field change is followed by the reformation of the null‐separator structure to cause a convection transient and a… Show more

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Cited by 14 publications
(33 citation statements)
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References 41 publications
(112 reference statements)
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“…Thus, we can estimate how the numerical model is appropriately working by seeing the reproducibility of ionospheric disturbances. As ionospheric disturbances, REPPU code reproduces the quiet arc after the southward turning of the IMF (Tanaka, 2015;, the initial brightening at the substorm onset (Ebihara & Tanaka, 2015a;Tanaka, 2015;, equatorial counter electrojet after the substorm onset (Ebihara et al, 2014), the westward traveling surge (Ebihara & Tanaka, 2015b;Ebihara & Tanaka, 2017b), the Sun-aligned arc under the northward IMF (Tanaka, Obara, et al, 2017), and the theta aurora (Tanaka et al, 2004(Tanaka et al, , 2018 quite similarly to observations. In all cases, the reproducibility of the ionospheric features outperforms other global models.…”
Section: Methods Of the Mhd Simulationsupporting
confidence: 58%
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“…Thus, we can estimate how the numerical model is appropriately working by seeing the reproducibility of ionospheric disturbances. As ionospheric disturbances, REPPU code reproduces the quiet arc after the southward turning of the IMF (Tanaka, 2015;, the initial brightening at the substorm onset (Ebihara & Tanaka, 2015a;Tanaka, 2015;, equatorial counter electrojet after the substorm onset (Ebihara et al, 2014), the westward traveling surge (Ebihara & Tanaka, 2015b;Ebihara & Tanaka, 2017b), the Sun-aligned arc under the northward IMF (Tanaka, Obara, et al, 2017), and the theta aurora (Tanaka et al, 2004(Tanaka et al, , 2018 quite similarly to observations. In all cases, the reproducibility of the ionospheric features outperforms other global models.…”
Section: Methods Of the Mhd Simulationsupporting
confidence: 58%
“…The distribution of the Sun-aligned arc is not radially from the cusp but parallel to the 12-0 LT [Tanaka, Obara, et al, 2017;Tanaka et al, 2018]. The shape of the FAC in this part is similar to the Sun-aligned arc, but the direction is not similar.…”
Section: Features Of Ionospheric Dynamicsmentioning
confidence: 80%
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“…For such comparison in the ionosphere, validity of the global simulation has been confirmed also under the northward interplanetary magnetic field (IMF), in reproducing the Sun‐aligned arc (Tanaka, Obara, et al, ), the theta aurora (Tanaka et al, , ), and the fan‐shaped arc (Tanaka, Obara, et al, ). These phenomena have been known for a long time, but consideration for their causes have been staying at the level of estimation.…”
Section: Introductionmentioning
confidence: 90%
“…On the other hand, Tanaka et al's (2004) detailed examination of the magnetic field line convection after the B y sign change revealed, that a return flow blockage in the convection cells after an IMF B y sign change may be responsible for the pileup of closed flux at the location of the bifurcated plasma sheet. Whether this pile-up of closed flux is created by reconnection or is just a result of redistributing field lines is not addressed by Tanaka et al (2004) and remains to be shown (note that, just recently, a newer version of REPPU code was applied to the theta aurora case and the results are introduced in Tanaka et al 2018).…”
Section: Mhd Simulation For B Y -Switchingmentioning
confidence: 99%