Physics of auroral phenomena : proceedings of the 34th Annual seminar, Apatity, 01 - 04 March, 2011 / [ed.: A. G. Yahnin, A. A. Mochalov]. - Апатиты : Издательство Кольского научного центра РАН, 2011. - 231 с. : ил.

Trans-polar propagation ofPil wave burst as observed by an Antarctic array during the Themis 2007 /03 /23 substorm the distant region, r » r 0, the electromagnetic field of the fast wave trapped in the ionospheric waveguide is dominant. In this region the direct signal falls off —2 rapidly as oc r , but the waveguide field weakly depends on radial distance В oc r~xn e x p ( - r / A ) , where attenuation length Л is very large, especially for nighttime conditions. The ducted wave has a lower cutoff frequency. The fundamental cutoff frequency is a ~VA12 D , where VA is the characteristic Alfven velocity inside the waveguide, and D is its width. The excitation factor of a waveguide mode decreases rapidly with increasing frequency, therefore the ground signal is expected to have a larger amplitude near cut­ off frequencies. Attenuation of the ducted wave (mostly caused by the ionospheric Joule loss) is an increasing function of frequency, larger for out-of-geomagnetic meridian plane propagation, and is minimized at со*. Observations of Pci propagation at mid-latitudes have shown that the damping rate is ~10dB/100km as a maximum in the injection region and ~2.5dB/100km in the region beyond 500 km [Hayashi et al., 1981]. Spatial attenuation is larger in the daytime than in the nighttime. Thus, the band-limited enhancement of Pil bursts can arise owing to the combination of two factors: cutoff at lower frequency, and weaker excitation and more severe attenuation of higher frequencies. The observed tendency of diminishing frequency of the high-frequency enhancement agrees with the modeling predictions of the damping increase for higher frequency. On the other hand, the band-limited enhancement may be caused by the resonant response/transmission of the auroral ionosphere [ Lysak, 1988; Pilipenko et a l, 2002]. The IAR excitation may occur only in the region of the Pil source. Because the IAR fundamental frequency COA ~ VA sin I / 2D (/ is the declination) is commonly less than the ionospheric waveguide cutoff frequency, (0A < CO. , the waveguide mode cannot excite the IAR upon its propagation. We suppose that at auroral latitudes the enhancements at -0.42 Hz (MCQ) and -0.35 Hz (POK) are caused by IAR effects. The difference in the highlighted frequencies is quite natural, because the conjugate ionospheres are not identical. This study demonstrates that Antarctica has a unique dense array of search-coil magnetometers corresponding to all magnetospheric domains: the sub-auroral and auroral regions, cusp, and polar cap, which may be used by the space community as an effective tool for substorm-related research. This study is an additional demonstration of the ever growing potentialities of the Antarctic array for space physics. Acknowledgements. We acknowledge B. Fraser for the provision of Australian station data, A. Rodger for data from HBA, M. Vellante for data from TNB and DMC, and V. Bedenko for the help in data analysis. This research was supported by U.S. NSF grants ANT- 0840133 and ATM-0827903. References Amoldy R.L., et al., Pil magnetic pulsations in space and at high latitudes on the ground, J. Geophys. Res., 103, 23581, 1998. Arthur C.W., R.L. McPherron, Simultaneous ground-satellite observations o f Pi2 magnetic pulsations and their high frequency enhancement. Planet. Space Sci., 28, 875, 1980. Bosinger T. A.G. Yahnin, PilB type magnetic pulsations as a high time resolution monitor o f substorm developement, Ann. Geophysicae, 5A, 231,1987. Fujita S., T. Tamao, Duct propagation o f MHD waves in the upper ionosphere. 1. 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