The Cassini Campaign observations of the Jupiter aurora by the Ultraviolet Imaging Spectrograph and the Space Telescope Imaging Spectrograph

被引:20
|
作者
Ajello, JM [1 ]
Pryor, W
Esposito, L
Stewart, I
McClintock, W
Gustin, J
Grodent, D
Gérard, JC
Clarke, JT
机构
[1] CALTECH, Jet Prop Lab, Pasadena, CA 91109 USA
[2] Cent Arizona Coll, Casa Grande, AZ 85228 USA
[3] Univ Colorado, Atmospher & Space Phys Lab, Boulder, CO 80303 USA
[4] Univ Liege, Lab Phys Atmospher & Planetaire, B-4000 Liege, Belgium
[5] Boston Univ, Boston, MA 02215 USA
基金
美国国家航空航天局;
关键词
spectroscopy; Jupiter magnetosphere; Jupiter atmosphere; ultraviolet observations;
D O I
10.1016/j.icarus.2005.01.023
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We have analyzed the Cassini Ultraviolet Imaging, Spectrometer (UVIS) observations of the Jupiter aurora with an auroral atmosphere two-stream electron transport code. The observations Of Jupiter by UVIS took place during the Cassini Campaign. The Cassini Campaign included Support spectral and imaging observations by the Hubble Space Telescope (HST) Space Telescope Imaging Spectrograph (STIS). A major result for the UVIS observations was the identification of a large color variation between the far ultraviolet (FUV: 1100-1700 angstrom) and extreme ultraviolet (EUV: 800-1100 angstrom) spectral regions. This change probably occurs because of a large variation in the ratio of the soft electron flux (10-3000 eV) responsible for the EUV aurora to the hard electron flux (similar to 15-22 keV) responsible for the FUV aurora. On the basis of this result a new color ratio for integrated intensities for EUV and FUV was defined (4 pi I1550-1620 angstrom/4 pi I (1030-1150 angstrom)) which varied by approximately a factor of 6. The FUV color ratio (4 pi I (1550-1620) angstrom/4 pi (1230-1300) (angstrom)) was note stable with a variation of less than 50% for the observations studied. The medium resolution (0.9 angstrom FWHM, G140M grating) FUV observations (1295-1345 angstrom and 1495-1540 angstrom) by STIS on 13 January 2001, on the other hand, were analyzed by a spectral modeling technique using a recently developed high-spectral resolution model for the electron-excited H-2 rotational lines. The STIS FUV data were analyzed with a model that considered the Lyman band spectrum (B (1) Sigma(+)(u) -> X-1 Sigma(+)(g)) as composed of an allowed direct excitation component (X-1 Sigma(+)(g) B-1 (+)(Sigma u)) and an optically forbidden component (X-1 Sigma(+)(g) -> EF, GK, H (H) over bar,.... (1)Sigma(+)(u) followed by the cascade transition (1)Sigma -> B-1 Sigma(+)(u)). The medium-resolution spectral regions for the Jupiter aurora were carefully chosen to emphasize the cascade component. The ratio of the two components is a direct measurement of the mean secondary electron energy of the aurora. The mean secondary electron energy of the aurora varies between 50 and 200 eV for the polar cap, limb and auroral oval observations. We examine a long time base of Galileo Ultraviolet Spectrometer color ratios from the standard mission (1996-1998) and compare them to Cassini UVIS, HST, and International Ultraviolet Explorer (IUE) observations. (c) 2005 Elsevier Inc. All rights reserved.
引用
收藏
页码:327 / 345
页数:19
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