A laboratory database of solid CO and CO2 for ISO

P.Ehrenfreund 1, A.C.A. Boogert 2, P.A. Gerakines 1,3, D.J. Jansen 1, A.G.G.M. Tielens 4, and E.F. van Dishoeck 1

Introduction

CO and, according to recent ISO observations, also CO2 are important ices in dense clouds. Peak position and band width of the strong bands of CO and CO2 indicate not only the polar and apolar character of the ice, but can also give an indication on temperature and radiation history of grains. The study of CO and CO2 bands provides a powerful tool to determine the icy grain mantle composition, in particular the presence of solid O2 and N2, and the grain evolution in the cycle of interstellar clouds. We present laboratory measured infrared spectra of mixtures containing CO and CO2 at temperatures between 10 and 80 K. Comparison of these laboratory data to astronomical spectra, taken by the ISO satellite and ground based facilities, is an essential tool to determine the composition and evolution of interstellar grain mantles.

This database contains 75 experiments on apolar ices and standard polar mixtures. The datafiles also contain the optical constants n and k. The changes in the profiles are simulated for different particle shapes such as spheres, ellipsoids and core/mantle particles. Using this database, observers can fit their observed profiles themselves, and assess the influence of any particle shape using the optical constants. Please refer to the present paper in the A & A special issue, when using datafiles from the database. We wish you fun and success! You can retrieve a ps file by clicking here. A complete paper with the physical interpretation "Infrared spectroscopy of apolar ice analogs" is submitted to A & A Main Journal and will be accessible here after the referee process. (Ehrenfreund et al. 1997).

Experimental

Ices were condensed as pure gas or gas mixture in a high vacuum chamber on the surface of a CsI window, cooled by a closed cycle He refrigerator to 10 K. Infrared transmission spectra were obtained with a BioRad FTS 40A spectrometer at a resolution of 1 cm-1. Gases and gas mixtures have been prepared in a glass vacuum manifold. The purity of the used gases CO, CO2, N2 and O2 was 99.9997 % (Messer Griesheim). The deposition rate and sample thickness growth rate were about 1015 molec cm-2 s-1 and 1 um hr-1, respectively. Sample thickness of 0.05 to approximately 0.5 um have been estimated. A detailed description of the experimental setup has been given by Gerakines et al. 1995, A & A 296, 810.

Particle size and shape effects can affect the strong absorption features of solid CO and CO2. Interactions of an electromagnetic radiation field with the molecules in small grains can change the absorption profile and peak position. It induces an electric charge near the surface of the grain, and therefore the oscillators in the grain are subjected to applied and induced electric field components. The strength of the induced component depends on the polarizability of the grain, which in turn depends on the grainshape and the dielectric or optical constants of the ice.

The optical constants of all our spectra were calculated using the standard Kramers-Kronig analysis (e.g. Hudgins et al. 1993, ApJS 86, 713). For our optical constants we find that particle shape effects influence the profile of the CO2 stretch mode when the ice contains at least 10% CO2. For CO this limit is 30% (Tielens et al. 1991, ApJ 381, 181). However, we stress that at present the optical constants obtained by different laboratory groups do not agree. Thus, the calculated cross sections for the different particle shapes are somewhat uncertain. We refer to the detailed discussion given in Ehrenfreund et al. 1997.

The grain shape calculations were done in the Rayleigh limit, which is an approximation of Mie theory for particles small compared to the wavelength. For the grain core we used the optical constants of astronomical silicate (Laor & Draine 1993, ApJ 402, 441). We have performed calculations for different particle shapes such as:

The table below lists all available datafiles

Data-file order

Data files are ordered as such: Two files are available for each mixture:

  1. Code E1.NK - E75.NK contains the laboratory data and the optical constants.
    E1.NK - E75.NK files have 5 columns: The spectra are given between approximately 5000 and 500 cm-1, according to the mixture and the presence of important overtone bands. All spectra are baseline corrected. Spikes between 1000 - 500 cm-1 are intrinsic to the spectrometer-setup. Particularly strong spikes are present between 690--720 cm-1, close to the CO2 bending mode, and we removed these by linear interpolation. The remaining spikes have no influence on the optical constant or particle shape calculations of the CO and CO2 profiles.
  2. Code E1.PSC - E75.PSC contains the wavelength dependend absorption cross sections, normalized to grain (core + mantle) volume (`Cabs/V').
    E1.PSC - E75.PSC files have 5 columns:

Dynamical database

We want to state that this database is a dynamical system. Currently there are strong controversies concerning the measurements of optical constants of ices between various leading groups in the field. New laboratory measurements can always improve the accuracy to derive optical constants, therefore experiments might be added to this database or new measurements affecting optical constants and particle shape calculations may be implemented. We ask you therefore to check the "update" date.

P. Ehrenfreund, A. Boogert, P. Gerakines, D. Jansen

The database

    APOLAR ICES
E1.NK E1.PSC CO pure 10K
E2.NK E2.PSC CO pure 30K
E3.NK E3.PSC H2O:CO = 1:100 10K
E4.NK E4.PSC H2O:CO = 1:100 30K
E5.NK E5.PSC H2O:CO:O2 = 1:80:20 10K
E6.NK E6.PSC H2O:CO:O2 = 1:80:20 30K
E7.NK E7.PSC CO:O2 = 100:50 10K
E8.NK E8.PSC CO:O2 = 100:50 35K
E9.NK E9.PSC CO:O2 = 100:70 10K
E10.NK E10.PSC H2O:CO:O2 = 1:50:50 10K
E11.NK E11.PSC H2O:CO:O2 = 1:50:50 30K
E12.NK E12.PSC H2O:CO:O2 = 1:20:60 10K
E13.NK E13.PSC H2O:CO:O2 = 1:20:60 30K
E14.NK E14.PSC CO2 pure 10K
E15.NK E15.PSC CO2 pure 50K
E16.NK E16.PSC CO2 pure 80K
E17.NK E17.PSC H2O:CO2 = 1:100 10K
E18.NK E18.PSC H2O:CO2 = 1:100 30K
E19.NK E19.PSC H2O:CO2 = 1:10 10K
E20.NK E20.PSC H2O:CO2 = 1:10 80K
E21.NK E21.PSC H2O:CO2 = 1:6 10K
E22.NK E22.PSC H2O:CO2 = 1:6 42K
E23.NK E23.PSC H2O:CO2 = 1:6 45K
E24.NK E24.PSC H2O:CO2 = 1:6 50K
E25.NK E25.PSC H2O:CO2 = 1:6 55K
E26.NK E26.PSC H2O:CO2 = 1:6 75K
E27.NK E27.PSC CO:CO2 = 100:4 10K
E28.NK E28.PSC CO:CO2 = 100:4 30K
E29.NK E29.PSC CO:CO2 = 100:8 10K
E30.NK E30.PSC CO:CO2 = 100:8 30K
E31.NK E31.PSC CO:CO2 = 100:16 10K
E32.NK E32.PSC CO:CO2 = 100:16 30K
E33.NK E33.PSC CO:CO2 = 100:21 10K
E34.NK E34.PSC CO:CO2 = 100:21 30K
E35.NK E35.PSC CO:CO2 = 100:23 10K
E36.NK E36.PSC CO:CO2 = 100:23 30K
E37.NK E37.PSC CO:CO2 = 100:26 10K
E38.NK E38.PSC CO:CO2 = 100:26 30K
E39.NK E39.PSC CO:CO2 = 100:70 10K
E40.NK E40.PSC H2O:CO:CO2 = 1:50:56 10K
E41.NK E41.PSC H2O:CO:CO2 = 1:50:56 45K
E42.NK E42.PSC CO2:O2 = 1:1 10K
E43.NK E43.PSC CO:O2:CO2 = 100:50:4 10K
E44.NK E44.PSC CO:O2:CO2 = 100:50:4 30K
E45.NK E45.PSC CO:O2:CO2 = 100:50:8 10K
E46.NK E46.PSC CO:O2:CO2 = 100:50:16 10K
E47.NK E47.PSC CO:O2:CO2 = 100:50:16 30K
E48.NK E48.PSC CO:O2:CO2 = 100:50:21 10K
E49.NK E49.PSC CO:O2:CO2 = 100:50:21 30K
E50.NK E50.PSC CO:O2:CO2 = 100:50:32 10K
E51.NK E51.PSC CO:O2:CO2 = 100:54:10 10K
E52.NK E52.PSC CO:O2:CO2 = 100:54:10 30K
E53.NK E53.PSC CO:O2:CO2 = 100:20:11 10K
E54.NK E54.PSC CO:O2:CO2 = 100:20:11 30K
E55.NK E55.PSC CO:O2:CO2 = 100:11:20 10K
E56.NK E56.PSC CO:O2:CO2 = 100:11:20 30K
E57.NK E57.PSC CO:O2:CO2 = 100:10:23 10K
E58.NK E58.PSC CO:O2:CO2 = 100:10:23 30K
E59.NK E59.PSC H2O:CO:N2 = 1:50:50 10K
E60.NK E60.PSC H2O:CO:N2 = 1:50:50 30K
E61.NK E61.PSC CO:O2:N2 = 100:50:25 10K
E62.NK E62.PSC H2O:CO:O2:N2 = 1:40:40:15 10K
E63.NK E63.PSC H2O:CO:O2:N2 = 1:40:40:15 30K
E64.NK E64.PSC CO:N2:CO2 = 100:50:20 10K
E65.NK E65.PSC CO:N2:CO2 = 100:50:20 30K
E66.NK E66.PSC CO:O2:N2:CO2 = 100:50:25:32 10K
E67.NK E67.PSC CO:O2:N2:CO2 = 100:50:25:32 30K
E68.NK E68.PSC H2O:CO:O2:N2:CO2=1:50:35:15:3 10K thick sample
E69.NK E69.PSC H2O:CO:O2:N2:CO2=1:50:35:15:3 10K thin sample
E70.NK E70.PSC H2O:CO:O2:N2:CO2=1:25:25:10:13 10K
POLAR ICES
E71.NK   H2O:CO = 100:6 10K
E72.NK   H2O:CO = 100:10 10K
E73.NK   H2O:CO = 100:20 10K
E74.NK E74.PSC H20:CO2 = 100:14 10K
E75.NK E75.PSC H20:CO2:CO = 100:20:3 20K

Contact

More spectra are available. For questions please contact:
Pascale Ehrenfreund