scholarly journals Dynamical measurement of the stellar surface density of face-on galaxies

2015 ◽  
Vol 585 ◽  
pp. A17 ◽  
Author(s):  
G. W. Angus ◽  
G. Gentile ◽  
B. Famaey
2008 ◽  
Vol 4 (S254) ◽  
pp. 307-312
Author(s):  
Leo Blitz

AbstractThe molecular gas in galaxy disks shows much more galaxy to galaxy variation than does the atomic gas. Detailed studies show that this variation can be attributed to differences in hydrostatic pressure in the disks due largely to variations in the stellar surface density and the total gas surface density. One prediction of pressure modulated H2 formation is that the location where HI and H2 have equal surface densities occurs at a constant value of the stellar surface density in the disk. Observations confirm this constancy to 40%.


2018 ◽  
Vol 483 (4) ◽  
pp. 5548-5553 ◽  
Author(s):  
Michael Y Grudić ◽  
Philip F Hopkins ◽  
Eliot Quataert ◽  
Norman Murray

2017 ◽  
Vol 468 (4) ◽  
pp. 4494-4501 ◽  
Author(s):  
Guangtun Ben Zhu ◽  
Jorge K. Barrera-Ballesteros ◽  
Timothy M. Heckman ◽  
Nadia L. Zakamska ◽  
Sebastian F. Sánchez ◽  
...  

2010 ◽  
Vol 401 (1) ◽  
pp. L19-L23 ◽  
Author(s):  
Philip F. Hopkins ◽  
Norman Murray ◽  
Eliot Quataert ◽  
Todd A. Thompson

2020 ◽  
Vol 496 (1) ◽  
pp. 864-869
Author(s):  
Chih-Teng Ling ◽  
Tetsuya Hashimoto ◽  
Tomotsugu Goto ◽  
Ting-Yi Lu ◽  
Alvina Y L On ◽  
...  

ABSTRACT Observationally, it has been reported that the densest stellar system in the Universe does not exceed a maximum stellar surface density, $\Sigma ^{\max }_{*}$ = $3\times 10^5\, {\rm M}_{\odot }\,{\rm pc}^{-2}$, throughout a wide physical scale ranging from star cluster to galaxy. This suggests that there exists a fundamental physics that regulates the star formation and stellar density. However, factors that determine this maximum limit are not clear. In this study, we show that $\Sigma ^{\max }_{*}$ of galaxies is not a constant as previous work reported, but actually it depends on the stellar mass. We select galaxy sample from the Sloan Digital Sky Survey Data Release 12 at z = 0.01–0.5. In contrast to a constant maximum predicted by theoretical models, $\Sigma ^{\max }_{*}$ strongly depends on stellar mass, especially for less massive galaxies with $\text{$\sim$}10^{10}\, {\rm M}_{\odot }$. We also found that a majority of high-Σ* galaxies show red colours and low star formation rates. These galaxies probably reach the $\Sigma ^{\max }_{*}$ as a consequence of the galaxy evolution from blue star forming to red quiescent by quenching star formation. One possible explanation of the stellar-mass dependence of $\Sigma ^{\max }_{*}$ is a mass-dependent efficiency of stellar feedback. The stellar feedback could be relatively more efficient in a shallower gravitational potential, which terminates star formation quickly before the stellar system reaches a high stellar density.


1967 ◽  
Vol 31 ◽  
pp. 265-278 ◽  
Author(s):  
A. Blaauw ◽  
I. Fejes ◽  
C. R. Tolbert ◽  
A. N. M. Hulsbosch ◽  
E. Raimond

Earlier investigations have shown that there is a preponderance of negative velocities in the hydrogen gas at high latitudes, and that in certain areas very little low-velocity gas occurs. In the region 100° <l< 250°, + 40° <b< + 85°, there appears to be a disturbance, with velocities between - 30 and - 80 km/sec. This ‘streaming’ involves about 3000 (r/100)2solar masses (rin pc). In the same region there is a low surface density at low velocities (|V| < 30 km/sec). About 40% of the gas in the disturbance is in the form of separate concentrations superimposed on a relatively smooth background. The number of these concentrations as a function of velocity remains constant from - 30 to - 60 km/sec but drops rapidly at higher negative velocities. The velocity dispersion in the concentrations varies little about 6·2 km/sec. Concentrations at positive velocities are much less abundant.


2015 ◽  
Vol 25 (1) ◽  
pp. 47-80 ◽  
Author(s):  
Bejoy Mandumpala Devassy ◽  
Chawki Habchi ◽  
Eric Daniel
Keyword(s):  

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