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91探花
Juno Jupiter image

Simon Calcutt

Emeritus

Sub department

  • Atmospheric, Oceanic and Planetary Physics

Research groups

  • Planetary atmosphere observation analysis
  • Solar system
  • Space instrumentation
  • Planetary surfaces
simon.calcutt@physics.ox.ac.uk
Telephone: 01865 (2)72916
Atmospheric Physics Clarendon Laboratory, room 308
  • About
  • Publications

Upper limits on hydrogen halides in Jupiter from Cassini/CIRS observations

Icarus 170:1 (2004) 237-241

Authors:

T Fouchet, G Orton, PGJ Irwin, SB Calcutt, CA Nixon

Abstract:

We have determined the following upper limits for the mole fraction of hydrogen halides in Jupiter's atmosphere from Cassini/CIRS observations: [HF] <2.7脳10-11, [HCl] <2.3脳10-9, [HBr]<1.0脳10-9, [HI] <7.6脳10-9. These limits are smaller than solar composition for HF and HCl, and 91探花 the halogens' condensation in ammonium salts predicted by thermochemical models for the upper jovian troposphere. 漏 2004 Published by Elsevier Inc.

An intense stratospheric jet on Jupiter

Nature 427 (2004) 132-135

Authors:

SB Calcutt, Achtergerg, Flasar, Kunde

Retrievals of jovian tropospheric phosphine from Cassini/CIRS

ICARUS 172:1 (2004) 37-49

Authors:

PGJ Irwin, P Parrish, T Fouchet, SB Calcutt, FW Taylor, AA Simon-Miller, CA Nixon

The retrieval of cloud structure maps in the Equatorial region of Jupiter using a principal component analysis of Galileo/NIMS data

Icarus 156 (2002) 52-63

Authors:

PG Irwin, U. Dyudina

Correlation of near-infrared albedo and 5-micron brightness variations in Jupiter's atmosphere

ADV SPACE RES 29:2 (2002) 285-290

Authors:

PGJ Irwin, SB Calcutt, AL Weir, FW Taylor, RW Carlson

Abstract:

The Galileo Near Infrared Mapping Spectrometer (NIMS) has returned many spectra of the Jovian atmosphere in the range 0.7-5.2 mum. Although communications restrictions have limited the data return, several wide-area maps have been recorded at near full NIMS resolution. Using these data it is possible to determine both the average shape of the near-infrared (NIR) spectra with very thick clouds (and zero 5-mum brightness) and how these spectra vary as the 5-mum brightness increases.In most of the cases studied, we find that the variable part of the reflectivity has a very different shape to the mean part and may best be explained by variable reflectivity in the cloud layers at pressures greater than 1 bar. In these cases it would thus appear that a variable opacity in a cloud deck based between 1 and 2 bars is mainly responsible for the NIR albedo variations, and not a higher ammonia cloud based above 1 bar as has often been previously suggested. While the composition of this main variable cloud deck could well be ammonium hydrosulphide, other candidates include ammonia (should the much higher estimate of its deep gaseous fractional abundance resulting from the Galileo probe mission be correct), and perhaps even the upper reaches of a deeper water cloud. (C) 2002 COSPAR. Published by Elsevier Science Ltd. All rights reserved.

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