Optical observations of the Galactic SNR HB9 and H II region G159.2+3.3

TL;DR

This study uses multi-wavelength optical observations to analyze the properties and potential connections of the Galactic SNR HB9 and the H II region G159.2+3.3, revealing differences in their gas dynamics and ionization states.

Contribution

It provides detailed optical spectral analysis of HB9 and G159.2+3.3, clarifying their physical properties and suggesting they are not physically connected despite apparent proximity.

Findings

HB9 shows higher radial velocity dispersion indicating shock-triggered motion.

G159.2+3.3's electron density is lower, implying a greater distance.

Shock ionization contributes to the emission in HB9's SE shell.

Abstract

Context. We present multi-wavelength observations of the Galactic SNR HB9 and the H II region G159.2+3.3 apparently projected nearby, in order to study their properties and potential physical connections. Results. HB9 is bright in $\gamma$-rays, but the $\gamma$-ray morphology is centrally filled and most of it is not clearly associated with the surrounding molecular clouds. There is a weak apparent connection of HB9 to the IR bright enclosing shell of G159.2+3.3 in $\gamma$-ray. The diffuse Balmer line has almost identical morphology as the radio emission in G159.2+3.3, indicating they two are thermal in origin. Using medium-band high-resolution optical spectra from selected regions of the southeast (SE) shell of HB9 and G159.2+3.3, we found the radial velocity dispersion of HB9 along the slit is significantly higher than the FWHM of the lines. In contrast, these two values are both smaller and comparable to each other in G159.2+3.3. This indicates that the gas in HB9 may have additional global motion triggered by the SNR shock. The [N II] $\lambda$6583A/H$\alpha$ line ratio of both objects can be interpreted with photo-ionisation by hot stars or low velocity shocks, except for the post-shock region in the SE shell of HB9, where the elevated [N II]/H$\alpha$ line ratio suggests contribution from shock ionisation. The measured electron density from the [S II] 6716/6730 line ratio is significantly lower in the brighter G159.2+3.3 compared to the SE shell of HB9. Conclusions. Our density estimate suggests that G159.2+3.3, although appearing brighter and more compact, is likely located at a much larger distance than HB9, so the two objects have no physical connections, unless the shock compressed gas in HB9 has a significantly lower filling factor.