Table 1
Results from the Voigt-profile fitting of the six components in the DLA at zabs = 0.313 toward PKS 1127−145.
Comp. | vrest | b (Ca ii) | log N(H i) | log N(Ca ii) | log N(Ti ii) | log N(Mn ii) | log N(Na i) |
![]() |
![]() |
||||||
|
|||||||
1 | −46.5 | 11.2 | 20.97 | 11.85±0.01 | 11.96±0.03 | 12.44±0.02 | <11.21 |
2 | −12.3 (−11.25) | 6.8 | 21.04 | 11.92±0.01 | 12.37±0.02 | 12.72±0.01 | 12.28±0.07 |
3 | +4.0 ( + 2.31) | 2.6 | 20.99 | 11.87±0.01 | (10.12±1.08)a | 11.09±0.16 | 11.93±0.04 |
4 | +15.6 ( + 15.88) | 5.8 | 20.88 | 11.76±0.02 | 11.78±0.07 | 12.16±0.03 | 11.89±0.05 |
5 | +35.3 | 10.6 | 21.17 | 12.05±0.01 | 12.07±0.03 | 12.56±0.01 | <11.21 |
6 | +64.4 | 6.8 | 21.14 | 12.02±0.01 | 11.84±0.04 | 12.09±0.02 | <11.21 |
|
|||||||
Total | − | − | 21.71 | 12.59±0.02 | 12.76±0.04 | 13.16±0.02 | 12.55![]() |
Notes. The velocities are given in the z = 0.312710 restframe, as assumed by Kacprzak et al. (2010a). For Na i, we allowed fitlyman to vary the component’s centroid velocity within 2 km s-1 from the fixed values for the other ions. The values in brackets in column two are these slightly deviant velocities of the components in Na i. The upper limits for N(Na i) were derived from the signal-to-noise ratio without the need for specific component-velocities. The Doppler-parameters b are from the fits of the Ca ii lines. For the H i column densities, a proportionality between the column densities of Ca ii- & H i and an overall H i column density of log N(H i)= 21.71 are assumed.
Current usage metrics show cumulative count of Article Views (full-text article views including HTML views, PDF and ePub downloads, according to the available data) and Abstracts Views on Vision4Press platform.
Data correspond to usage on the plateform after 2015. The current usage metrics is available 48-96 hours after online publication and is updated daily on week days.
Initial download of the metrics may take a while.