Figure 6.
Mg ii λλ2796, 2803 absorption profiles of halo gas around the super-L* barred spiral galaxy G2 at z = 0.7818. Absorption spectra of QSO sightlines A′, C ′ and D′ (corrected lensed image positions at the redshift plane of G2; see the image in Fig. 7) obtained with MagE are available. Zero relative velocity corresponds to the systemic redshift of the galaxy at z = 0.7818. Despite a lower spectral resolution, the MagE spectra show remarkably distinct absorption morphology across different sightlines. In particular, sightlines C ′ and D′ occur at a similar projected distance from G2 and are roughly 6 kpc in projected separation. The observed Mg ii absorption is spread over 130 km s−1 along the sightline towards C ′, whereas more concentrated absorption is found within a narrow FWHM ≈ 42 km s−1 along the sightline towards D′.

Mg ii λλ2796, 2803 absorption profiles of halo gas around the super-L* barred spiral galaxy G2 at z = 0.7818. Absorption spectra of QSO sightlines A, C and D (corrected lensed image positions at the redshift plane of G2; see the image in Fig. 7) obtained with MagE are available. Zero relative velocity corresponds to the systemic redshift of the galaxy at z = 0.7818. Despite a lower spectral resolution, the MagE spectra show remarkably distinct absorption morphology across different sightlines. In particular, sightlines C and D occur at a similar projected distance from G2 and are roughly 6 kpc in projected separation. The observed Mg ii absorption is spread over 130 km s−1 along the sightline towards C, whereas more concentrated absorption is found within a narrow FWHM ≈ 42 km s−1 along the sightline towards D.

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