1976
DOI: 10.1029/ja081i001p00088
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On a threshold electric field associated with the 398-MHz diffuse radar aurora

Abstract: In this paper we address the question of whether auroral echoes are dependent on the ionospheric electric field. This question naturally arises from the concept of a plasma instability as the source mechanism producing the electron density irregularities responsible for the auroral echoes. Using the data from a backscatter radar located at Homer, Alaska, and the Chatanika incoherent scatter radar in a joint experiment, we show that there is a distinct dependence of the occurrence of diffuse auroral echoes on a… Show more

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Cited by 34 publications
(17 citation statements)
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“…Strong experimental evidence for this relationship has been found recently by ECKLUND et al (1977) andCAHILL et al (1978). The only serious problem in observing auroral zone electric fields with this type of radar is that a threshold electric field apparently is needed to excite the plasma irregularities in the ionosphere (TSUNODA and PRESNELL, 1976;SIREN et al, 1977). CAHILL et al (1978) found threshold values of 15-20mVm-1 for the STARE radars.…”
Section: Instrumentationmentioning
confidence: 87%
“…Strong experimental evidence for this relationship has been found recently by ECKLUND et al (1977) andCAHILL et al (1978). The only serious problem in observing auroral zone electric fields with this type of radar is that a threshold electric field apparently is needed to excite the plasma irregularities in the ionosphere (TSUNODA and PRESNELL, 1976;SIREN et al, 1977). CAHILL et al (1978) found threshold values of 15-20mVm-1 for the STARE radars.…”
Section: Instrumentationmentioning
confidence: 87%
“…Eather [1967] pointed out that emission from the proton aurora rarely exceeds 200 R. For the ionization rate profiles presented by Eather [1970] only 104 el/cm 8. Tsunoda and Presnell [1976] showed that the diffuse auroral echoes can be observed with the 398-MHz Homer radar only when the electron density exceeds few parts times 104 el/cm 8. But on the other hand, the peak electron densities associated with the diffuse radar aurora are typically no more than a few parts times 105 el/cm 3 (R. T. Tsunoda, unpublished data, 1974).…”
Section: Discussionmentioning
confidence: 99%
“…In that event the DB was associated only with the steepest portion of the downward field-aligned current region, that nearest the poleward boundary. The absence of auroral echoes in the region of less intense DFAC can be accounted for if we assume that the ionospheric electric field strength in that region was below the threshold electric field value[Tsunoda and Presnell, 1976]. Therefore the results indicate that the DFAC is collocated with the DB and hence with the eastward electrojet.In the following, we present several of the more interesting examples showing the actual spatial comparison between the radar aurora and field-aligned currents.…”
mentioning
confidence: 90%
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“…Since these were polar cap measurements the ionosphere was well behaved and the possibility of great changes in the acoustic speed due to electron heating less likely. TSUNODA and PRESNELL (1976) have shown a 30mV/m threshold for backscatter at 398MHz by comparing their auroral zone diffuse echoes to simultaneous Chatanika E field measurements. Thus it seems that the Farley-Buneman two-stream instability is the primary mechanism at the high latitudes.…”
Section: Instabilities In the Lower Ionosphere Driven By Perpendiculamentioning
confidence: 99%