Spitzer observations of supernova remnants: II. Physical conditions and comparison with HH7 and HH54

TL;DR

This study uses Spitzer and ISO spectroscopic data to analyze the physical conditions of shock-excited molecular regions in supernova remnants and Herbig-Haro objects, revealing density variations and shock geometries.

Contribution

It provides new constraints on gas densities, shock geometries, and ortho-to-para ratios in SNRs and HH objects using infrared spectroscopy.

Findings

Gas density in SNRs is estimated to be 2-4×10^3 cm^-3.

Shock front shape is flatter than a paraboloid, indicated by the power-law index.

Hot gas in SNRs has an ortho-to-para ratio close to LTE value 3.

Abstract

We have studied the shock-excited molecular regions associated with four supernova remnants (SNRs) - IC443C, W28, W44 and 3C391 - and two Herbig-Haro objects, HH7 and HH54, using Spitzer's Infrared Spectrograph (IRS). The physical conditions within the observed areas are inferred from spectroscopic data obtained from IRS and from SWS and LWS onboard ISO, together with photometric data from Spitzer's Infrared Array Camera (IRAC). Adopting a power-law distribution for the gas temperature in the observed region, the H2 S(0) to S(7) spectral line maps obtained with IRS were used to constrain the gas density, yielding estimated n(H2) in the range 2-4*10^3 cm^-3. The excitation of H2 S(9) to S(12) and high-J CO pure rotational lines, however, require environments several times denser. The inconsistency among the best-fit densities estimated from different species can be explained by density fluctuations within the observed regions. The best-fit power-law index b is smaller than the value 3.8 predicted for a paraboloidal C-type bow shock, suggesting that the shock front has a "flatter" shape than that of a paraboloid. The best-fit parameters for SNRs and Herbig-Haro objects do not differ significantly between the two classes of sources, except that for the SNRs the ortho-to-para ratio (OPR) of hot gas (T> 1000 K) is close to the LTE value 3, while for HH7 and HH54 even the hottest gas exhibits an OPR smaller than 3. Finally, we mapped the physical parameters within the regions observed with IRS and found that the mid-lying H2 emissions - S(3) to S(5) - tend to trace the hot component of the gas, while the intensities of S(6) and S(7) are more sensitive to the density of the gas compared to S(3) to S(5).