1981
DOI: 10.1029/ja086ia06p04686
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Spectral characteristics of magnetic Pi 2 pulsations in the auroral region and lower latitudes

Abstract: The spectral characteristics of magnetic Pi 2 pulsations are studied in detail using data obtained simultaneously over a wide latitudinal range from the auroral region (L=7.5) through low latitudes (L=1.8). Pi 2 is revealed to be observed almost simultaneously with the onset of a substorm expansion over the wide latitudinal range with the common predominant period. The Pi 2 amplitude shows a primary maximum at the auroral oval and an additional secondary maximum near the plasmapause. The Pi 2 period generally … Show more

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Cited by 37 publications
(25 citation statements)
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“…On the other hand, since VA has a sharp gradient just inside the plasmapause where the Pit amplitude appears to show a secondary maximum (e.g., Kuwashima and Saito, 1981), the excitation of 6jljust inside the plasmapause will be primarily due to the effect of inhomogeneity. Further, the excitation will be more intense just inside the plasmapause than in the regions which surround the plasmapause.…”
Section: Discussionmentioning
confidence: 99%
“…On the other hand, since VA has a sharp gradient just inside the plasmapause where the Pit amplitude appears to show a secondary maximum (e.g., Kuwashima and Saito, 1981), the excitation of 6jljust inside the plasmapause will be primarily due to the effect of inhomogeneity. Further, the excitation will be more intense just inside the plasmapause than in the regions which surround the plasmapause.…”
Section: Discussionmentioning
confidence: 99%
“…The amplitude of Pi2 pulsations has the primary maximum around the auroral electrojet latitudes and the secondary maximum near the foot point of the plasmapause (e.g., Kuwashima and Saito, 1981). This secondary maximum is not always observed since it is weak and narrow in latitude.…”
Section: Introductionmentioning
confidence: 99%
“…Pi 2 pulsations at higher latitudes (L >-4) on the nightside have been generally interpreted to be either a transient standing resonance of the auroral field line excited at substorm expansion onset (Maltsev et al, 1974;Saito et al, 1976;Olson and Rostoker, 1977;Kuwashima, 1978) or oscillating localized fieldaligned currents in the substorm current wedge (and/or in the head of the westward traveling surge) (Pashin et al, 1982;Samson and Rostoker, 1983;Sakurai and McPherron, 1983;Glassmeier, 1988;Glassmeier et al, 1988).…”
Section: Introductionmentioning
confidence: 99%