Max-Planck-Institut für extraterrestrische Physik

High-Energy Astrophysics

Research Topic

X-ray Emission from Comets and Planets

Place the mouse over the image to see this comet in X-rays

Thus, the discovery of X-rays from comet Hyakutake with ROSAT in March 1996 came as a big surprise to many scientists. The surprise increased even more, when additional comets were detected in archival X-ray data obtained during the ROSAT all-sky survey, establishing comets as a new class of X-ray sources. The process which causes the X-ray emission of comets is now understood as the result of charge exchange interactions between heavy, highly ionized atoms in the solar wind with cometary gas. This process reproduces the observed X-ray luminosity and X-ray morphology very well, explains the temporal variability of the X-ray flux, and predicts characteristic signatures in the X-ray spectrum, which can now be tested with the spectroscopic capabilities of Chandra and XMM-Newton. All the observed X-ray properties are consistent with the charge exchange process. Comets can thus be used as natural spacecrafts to probe the heavy ion content of the solar wind at various heliographic latitudes and at different phases in the solar cycle, which is otherwise only accessible by in-situ measurements. Furthermore, X-ray observations of comets provide insights into the physics of the charge exchange process itself, complementing laboratory experiments and theoretical studies. More information is found at the following links:     MPG | ROSAT | NASA | Chandra | LLNL | MPA | XMM-Newton |

Place the mouse over the image to see Venus in X-rays

Orbiting the Sun at heliocentric distances of 0.718 - 0.728 astronomical units, the angular separation of Venus from the Sun, as seen from Earth, never exceeds 47.8 degrees. While the observing window of imaging astronomy satellites is usually restricted to solar elongations of at least 60 degrees, Chandra is the first such satellite which is able to observe as close as 45 degrees from the limb of the Sun. Thus, with Chandra an observation of Venus with an imaging X-ray astronomy satellite became possible for the first time, in January 2001. Venus was clearly detected as a half-lit crescent, with considerable brightening on the sunward limb. This morphology agrees well with that expected from fluorescent scattering of solar X-rays in the planetary atmosphere. The radiation is observed at discrete energies, mainly at 0.53 keV and at 0.28 keV, corresponding to K-alpha fluorescence on oxygen and carbon, the main constituents of the carbon dioxide atmosphere of Venus. In contrast to the optical radiation from Venus, which is sunlight reflected from clouds at 50-70 km height, most of the X-ray fluorescence takes place at heights of 120-140 km. Thus, X-ray observations of Venus can be used to monitor remotely the properties of the upper atmospheric layers of the Venus atmosphere, which are difficult to investigate otherwise, and their response to solar activity. For this observation the Low Energy Transmission Grating (LETG), developed at MPE, played an essential role. It did not only allow us to obtain a high resolution X-ray spectrum, but it provided also an efficient way of diffracting the extremely intense optical light to areas outside the X-ray CCDs, so that optical photons would not interfere with the X-ray observation. With this technique it was possible to detect unambiguously X-rays from Venus, despite the fact that the X-ray intensity did not exceed one ten-billionth of the optical intensity. More information is found at the following links:     MPG | NASA | Chandra | ESA | APOD | Venus image gallery |

Place the mouse over the image to see Mars in X-rays

Also Mars is an X-ray source. In the first Chandra observation, in July 2001, Mars was cleary detected as an almost fully illuminated disk, with an indication of limb brightening at the sunward side, accompanied by some fading at the opposite side. Although the atmosphere of Mars is much more tenuous than that of Venus, it is still opaque to solar X-rays. As the chemical composition of the Martian atmosphere is very similar to that of Venus (predominantly carbon dioxide), the observed X-rays are also here the result of fluorescent scattering of solar X-rays, mainly on carbon and oxygen. Compared to Venus, the region where most of the X-ray scattering happens is more extended and somewhat closer to the surface, at heights of 100-150 km. In addition to the fluorescent radiation, evidence for an additional source of X-ray emission was found, indicated by a faint X-ray halo which could be traced out to about three Mars radii, and by an additional component in the X-ray spectrum of Mars, which has a similar spectral shape as the halo. It is very likely that this halo is caused by the same process which is responsible for the X-ray emission of comets (see above). Scattering of solar X-rays on very small dust particles was one of the early suggestions for explaing the X-ray emission from comets. Such tiny dust grains might be present in the upper Mars atmosphere, in particular during episodes of global dust storms. The Chandra observation happened to take place when a vigorous dust storm was raging on Mars and had covered roughly one hemisphere. This hemisphere was visible at the beginning of the observation and had mainly rotated away from our view by the end of the observation, which lasted for one third of a Mars rotation. The X-ray flux from Mars, however, did not show any modulation, so that it can be excluded that the dust storm had whirled up a sufficient amount of such particles in the upper atmosphere to have a detectable effect on the X-ray radiation. More information is found at the following links:     XMM-Newton(1) | XMM-Newton(2) | Nature | MPG | NASA | Chandra | Mars image gallery |

Place the mouse over the image to see Saturn in X-rays

Saturn was unambiguously detected in X-rays only recently: in September 2002 with XMM-Newton and in April 2003 with Chandra. In the Chandra image, Saturn is clearly resolved. Although the spatial information is limited by the small number of photons (about 100), it is evident that the X-ray photons came almost exclusively from the southern hemisphere, which was tilted towards us. No X-ray photons were detected from the regions which were covered by the rings. This is an indication that the rings of Saturn are optically thick to X-rays and have a low X-ray albedo. Despite the low number of photons, it is not an easy task to find a simple spectral model which reproduces the measured energy distribution. The only acceptable single component model, a 0.18 keV blackbody, is physically not plausible. A 0.39 keV thermal spectrum, with an oxygen fluorescence emission line superimposed, however, provides an acceptable and physically motivated fit. The oxygen line accounts for one quarter of the energy emitted in the 0.3-2.0 keV band. This suggests that the observed X-rays from Saturn are maily solar X-rays, scattered in its upper atmosphere by a superposition of elastic scattering, mainly on hydrogen, and fluorescent scattering, mainly on oxygen. The intensity of the oxygen fluorescence line is comparable to that observed from Mars, if the different size of both planets and their different distance from the Sun and Earth is taken into account. The X-ray intensity of Saturn, however, exceeds that expected for scattering of solar X-rays, suggesting the presence of an additional mechanism. There are similarities in the X-ray emission of Saturn and the equatorial X-ray emission of Jupiter. However, while the X-ray intensity of Jupiter increases towards the magnetic poles, it was observed to decrease towards Saturn's south pole. More information is found at the following links:     NASA | Chandra | Saturn image gallery |

• Discovery of X-rays from Venus with Chandra,
  K. Dennerl, V. Burwitz, J. Englhauser, C. Lisse, S. Wolk, 2002,
  A&A 386, 319-330
  
  
• Discovery of X-rays from Mars with Chandra,
  K. Dennerl, 2002,
  A&A 394, 1119-1128
  
  
• X-rays from solar wind charge exchange at Mars: A comparison of simulations and observations,
  H. Gunell, M. Holmström, E. Kallio, P. Janhunen, K. Dennerl, 2004,
  GRL 31, L22801
  
  
• X-ray emission from Saturn,
  J.-U. Ness, J.H.M.M. Schmitt, S.J. Wolk, K. Dennerl, and V. Burwitz, 2004,
  A&A 418, 337-345
  
  
• A major step in understanding the X-ray generation in comets: recent progress obtained with XMM-Newton,
  K. Dennerl, B. Aschenbach, V. Burwitz, J. Englhauser, C. M. Lisse, P. M. Rodriguez-Pascal, 2003,
  in: X-Ray and Gamma-Ray Telescopes and Instruments for Astronomy, Proc. SPIE 4851, 277-288
  
  
• The morphology of cometary X-ray emission,
  R. Wegmann, K. Dennerl, C. Lisse, 2004,
  A&A 428, 647-661
  
  
• First observation of Mars with XMM-Newton: High resolution X-ray spectroscopy with RGS,
  K. Dennerl et al. 2006,
  A&A 451, 709-722
  
  
• X-Rays from Mars,
  K. Dennerl 2006,
  Space Science Reviews, Volume 126, Issue 1-4, pp. 403-433
  
  
• X-rays from Venus observed with Chandra,
  K. Dennerl 2008,
  Planetary and Space Science, Volume 56, Issue 10, p. 1414-1423
  
  
• X-Rays from Nonmagnetic Planets,
  K. Dennerl 2008,
  in: Advances in Geosciences, Volume 15, Planetary Science.

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H. Steinle

K. Dennerl