Cultural advice

The Australian National University acknowledges, celebrates and pays our respects to the Ngunnawal and Ngambri people of the Canberra region and to all First Nations Australians on whose traditional lands we meet and work, and whose cultures are among the oldest continuing cultures in human history.

Aboriginal and Torres Strait Islander peoples are advised that ANU Library collections may include images, names, voices, and other representations of deceased persons.

Material in the collection may contain terms, language or views that reflect the period in which the item was created and may be considered inappropriate today.

The HI mass function in the Parkes HI Zone of Avoidance survey

Loading...
Thumbnail Image

Date

Authors

Said, Khaled
Kraan-Korteweg, Renee Christine
Staveley-Smith, Lister

Journal Title

Journal ISSN

Volume Title

Publisher

Royal Astronomical Society

Abstract

An H I mass function (HIMF) was derived for 751 galaxies selected from the deep Parkes H I survey across the Zone of Avoidance (HIZOA). HIZOA contains both the Great Attractor Wall and the Local Void, two of the most extreme environments in the local Universe, making the sample eminently suitable to explore the overall HIMF as well as its dependence on local environment. To avoid any selection bias because of the different distances of these large-scale structures, we first used the 2D stepwise maximum-likelihood method for the definition of an average HIMF. The resulting parameters of a Schechter-type HIMF for the whole sample are α = −1.33 ± 0.05, log(M∗ H I /M) = 9.93 ± 0.04, and φ∗ = (3.9 ± 0.6) × 10−3 Mpc−3. We then used the k-th nearest-neighbour method to subdivide the sample into four environments of decreasing local density and derived the Schechter parameters for each subsample. A strong trend is observed, for the slope α of the low-mass end of the HIMF. The slope changes from being nearly flat, i.e. α = −0.99 ± 0.19 for galaxies residing in the densest bin, to the steep value of α = −1.31 ± 0.10 in the lowest density bin. The characteristic mass, however, does not show a clear trend between the highest and lowest density bins. We find similar trends in the low-mass slope when we compare the results for a region dominated by the Great Attractor, and the Local Void, which are found to be over-, respectively underdense by 1.35 and 0.59 compared to the whole sample.

Description

Citation

Source

Monthly Notices of the Royal Astronomical Society

Book Title

Entity type

Access Statement

Open Access

License Rights

Restricted until