scholarly journals Exploring the origins of a new, apparently metal-free gas cloud atz = 4.4

2018 ◽  
Vol 483 (2) ◽  
pp. 2736-2747 ◽  
Author(s):  
P Frédéric Robert ◽  
Michael T Murphy ◽  
John M O’Meara ◽  
Neil H M Crighton ◽  
Michele Fumagalli
Keyword(s):  
Free Gas ◽  
2012 ◽  
Author(s):  
Chalence Safranek-Shrader ◽  
Meghann Agarwal ◽  
Christoph Federrath ◽  
Anshu Dubey ◽  
Milos Milosavljevic ◽  
...  
Keyword(s):  
Free Gas ◽  

2019 ◽  
Vol 91 (20) ◽  
pp. 13158-13164 ◽  
Author(s):  
Li Li ◽  
Chudong Wei ◽  
Hongjie Song ◽  
Yongsheng Yang ◽  
Ying Xue ◽  
...  

1985 ◽  
Vol 106 ◽  
pp. 597-600 ◽  
Author(s):  
Cedric G. Lacey ◽  
S. Michael Fall

We have calculated models for the kinematical and chemical evolution of the Galactic disk that include the infall of metal-free gas and the stochastic acceleration of disk stars. Our models are similar in some respects to those of Chiosi (1980) and Vader & de Jong (1981), but the results are compared with a greater variety of observational data. A complete description of this work will appear shortly in Monthly Notices of the Royal Astronomical Society.


2009 ◽  
Vol 700 (2) ◽  
pp. 1672-1679 ◽  
Author(s):  
Michele Trenti ◽  
Massimo Stiavelli ◽  
J. Michael Shull

2003 ◽  
Vol 212 ◽  
pp. 334-340
Author(s):  
Paola Marigo ◽  
Cesare Chiosi ◽  
Léo Girardi ◽  
Rolf-Peter Kudritzki

We discuss the evolutionary properties of primordial massive and very massive stars, supposed to have formed from metal-free gas. Stellar models are presented over a large range of initial masses (8 M⊙ ≲ Mi ≲ 1000 M⊙), covering the hydrogen- and helium-burning phases up to the onset of carbon burning. In most cases the evolution is followed at constant mass. To estimate the possible effect of mass loss via stellar winds, recent analytic formalisms for the mass-loss rates are applied to the very massive models (Mi ≥ 120 M⊙).


Author(s):  
George C. Ruben

The formation of shadows behind small particles has been thought to be a geometric process (GP) where the metal cap build up on the particle creates a shadow width the same size as or larger than the particle. This GP cannot explain why gold particle shadow widths are generally larger than the gold particle and may have no appreciable metal cap build up (fig. 1). Ruben and Telford have suggested that particle shadow widths are formed by the width dependent deflection of shadow metal (SM) lateral to and infront of the particle. The trajectory of the deflected SM is determined by the incoming shadow angle (45°). Since there can be up to 1.4 times (at 45°) more SM directly striking the particle than the film surface, a ridge of metal nuclei lateral to and infront of the particle can be formed. This ridge in turn can prevent some SM from directly landing in the metal free shadow area. However, the SM that does land in the shadow area (not blocked by the particle or its ridge) does not stick and apparently surface migrates into the SM film behind the particle.


Nanoscale ◽  
2020 ◽  
Vol 12 (15) ◽  
pp. 8065-8094 ◽  
Author(s):  
Xudong Wen ◽  
Jingqi Guan

Different kinds of electrocatalysts used in NRR electrocatalysis (including single atom catalysts, metal oxide catalysts, nanocomposite catalysts, and metal free catalysts) are introduced.


2020 ◽  
Vol 7 (21) ◽  
pp. 3515-3520
Author(s):  
Wubing Yao ◽  
Jiali Wang ◽  
Aiguo Zhong ◽  
Shiliang Wang ◽  
Yinlin Shao

The selective catalytic reduction of amides to value-added amine products is a desirable but challenging transformation.


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