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Gas fraction and star formation efficiency at z \< 1.0⋆⋆⋆⋆⋆⋆
Gas fraction and star formation efficiency at z \< 1.0⋆⋆⋆⋆⋆⋆

... et al. 2007), or to be a constant with M∗ (Wuyts et al. 2011). The global SFR decreases with cosmic time as SFR ∝ (1 + z)2.7 out to z = 1–2. At each epoch, there is a population of non-starforming (quiescent) galaxies of high mass and high Sersic index. These galaxies might correspond to quenched ga ...
Planetary Systems and Planets in Systems (pdf file 10.5
Planetary Systems and Planets in Systems (pdf file 10.5

... planet connection. We show that planet-host stars are more metal-rich than average field dwarfs, a trend that remains after the discovery of now more than about 100 planets. Current results also point out that the planetary frequency is rising as a function of the [Fe/H]. Furthermore, the source of ...
20. Meteorites and the chemical evolution of the Milky Way
20. Meteorites and the chemical evolution of the Milky Way

... by nucleosynthesis in stars of various types are required. These are determined by stellar evolutionary calculations coupled to nuclear reaction networks (e.g., Meyer and Zinner, 2006). In general, the nucleosynthesis abundance patterns ejected by stars depend critically on the stellar mass and meta ...
The Habitability of Planets Orbiting M
The Habitability of Planets Orbiting M

... orbiting other stars1 . Many of these planets are especially captivating because of their orbital distances, which place them in their stars’ canonical habitable zone—the region around a star where an orbiting planet with an Earth-like atmosphere (CO2 -H2 O-N2 ) could maintain water in liquid form o ...
Characterization of exoplanetary systems with the direct
Characterization of exoplanetary systems with the direct

... In the year of the 20th anniversary of the discovery of the first extrasolar planet we can count more than 1800 companions found with different techniques. The majority of them are indirect methods that infer the presence of an orbiting body by observing the parent star (radial velocity, transits, a ...
17_Testbank
17_Testbank

... 44) You discover a binary star system in which one member is a 15MSun main-sequence star and the other star is a 10MSun giant. Why should you be surprised, at least at first? A) It doesn't make sense to find a giant in a binary star system. B) The odds of ever finding two such massive stars in the s ...
talk
talk

...  Baryonic fraction for NGC 3741 (within the extent of the gas disk) ~ 0.18 ► comparable to other galaxies with less extended HI disk  No evidence for baryon loss (measured within the extent of gas disk) in faint dwarf galaxies (contradiction to simulations of galaxy formation !)  To reconcile rot ...
Constraints on Long-Period Planets from an L
Constraints on Long-Period Planets from an L

... is adaptive optics (AO), which allows 6-10m ground-based telescopes to obtain diffraction limited IR images several times sharper than those from HST, despite Earth’s turbulent atmosphere. Theoretical models of giant planets indicate that such telescopes should be capable of detecting self-luminous ...
IXO as an observatory in the large telescopes era
IXO as an observatory in the large telescopes era

... models propose that mergers of small gas-rich proto-galaxies in deep potential wells at high redshift drive star formation and black hole growth (in proto-quasar active galaxies) until a luminous quasar forms. At this point, a black hole driven wind evacuates gas from the nascent galaxy, limiting ad ...
Full Program with Abstracts - CIERA
Full Program with Abstracts - CIERA

... accurately the masses and infer compositions for a sample of these small worlds. Here I report on our conclusions from the first three years. After analyzing the Kepler light curves to vet potential targets, favoring those with asteroseismic estimates of the stellar properties and excluding those li ...
Collisional processes in extrasolar planetesimal discs
Collisional processes in extrasolar planetesimal discs

Project Description - SDSS-III
Project Description - SDSS-III

... the overall constraints on evolving dark energy when combined with complementary measurements that use supernovae, weak gravitational lensing, or galaxy clusters. BOSS will also provide rich insights into the matter contents of the Universe, the origin of cosmic structure, and the evolution of massi ...
The High Resolution Camera CXC Newsletter
The High Resolution Camera CXC Newsletter

... IR excess due a a massive debris disk surrounding the star, made up from dust and cometary bodies. There are at least three scenarios for the origin of this X-ray emission: (i) a stellar corona, (ii) a boundary layer where mass is accreted from the disk or (iii) charge-exchange between the stellar w ...
Gas fraction and star formation efficiency at z< 1.0
Gas fraction and star formation efficiency at z< 1.0

The Deaths of Very Massive Stars
The Deaths of Very Massive Stars

... sequence mass for stars of solar metallicity. O’Connor and Ott and Ugliano et al (2012) have both shown that it becomes difficult to explode the star by neutrino transport alone if ξ2.5 becomes very large. The critical value is not certain and may vary with other properties of the star, but in Uglia ...
Starburst Galaxies Under the Microscope: High
Starburst Galaxies Under the Microscope: High

... stars with a mass of about 8 M (the most numerous stars still producing supernovae), which have a lifetime of about 3 10 7 years, the BrG and [Fe II] emission trace phases of the starbursts that are temporally separated by this amount of time. In principle, one could use these results then to calcu ...
Lecture 8: Spiral Structure
Lecture 8: Spiral Structure

... • The best current tracers of spiral arms are the Giant Molecular Clouds (GMCs), from which massive stars are born. Their millimeter-line emission is Doppler shifted by radial motions, and so their locations can be determined in a way similar to that of H I (see Figure 20-7B). ...
The empirical mass distribution of hot B subdwarfs
The empirical mass distribution of hot B subdwarfs

... systems, while longer period binaries would result from RLOF, and the merger channel would explain the population of single sdB stars. These 3 scenarios have been studied in detail by [5, 6] from synthetic binary population simulations that provide, e.g., theoretical mass distributions for the resul ...
MASSIVE CLOSE BINARIES
MASSIVE CLOSE BINARIES

... reviewed by Kudritzki and Puls (2000) (see also P. Crowther, in these proceedings). Note that ...
Galactic Stellar and Substellar Initial Mass Function Invited Review Gilles Chabrier
Galactic Stellar and Substellar Initial Mass Function Invited Review Gilles Chabrier

... power-law approximations, dN/dm ∝ m!a, as initially suggested by Salpeter (1955), with an exponent close to the Salpeter value a p 2.35. A departure from this monotonic behavior, with a flattening of the MF below ∼1 M,, was first proposed by MS79, who suggested a lognormal form. The tremendous progr ...
arXiv:astro-ph/0508448v1 22 Aug 2005
arXiv:astro-ph/0508448v1 22 Aug 2005

Preface
Preface

... black holes sitting at the center of a galaxy at that age of the Universe. Since then dust has been continuously produced, processed, and destroyed in every single phase of the Universe. Dust forms by condensation out of rapidly cooling materials that flow outward from a dying star. Once injected in ...
Spitzer Spectroscopy of Circumstellar Disks in the 5 Myr Old Upper
Spitzer Spectroscopy of Circumstellar Disks in the 5 Myr Old Upper

Downloadable Full Text
Downloadable Full Text

... confirmed to be one of the most metal-poor galaxies known14. On 1-4 Oct 2015, we obtained high-resolution spectra of the nine brightest member stars in Ret II (see Table 1, Extended Data Figure 1). The abundances of non-neutron-capture elements in all nine stars are consistent with abundances in oth ...
Celebrating Astronomy: The Life of a Star
Celebrating Astronomy: The Life of a Star

< 1 ... 6 7 8 9 10 11 12 13 14 ... 158 >

Nebular hypothesis

The nebular hypothesis is the most widely accepted model in the field of cosmogony to explain the formation and evolution of the Solar System. It suggests that the Solar System formed from nebulous material. The theory was developed by Immanuel Kant and published in his Universal Natural History and Theory of the Heaven. Originally applied to our own Solar System, this process of planetary system formation is now thought to be at work throughout the universe. The widely accepted modern variant of the nebular hypothesis is the solar nebular disk model (SNDM) or simply solar nebular model. This nebular hypothesis offered explanations for a variety of properties of the Solar System, including the nearly circular and coplanar orbits of the planets, and their motion in the same direction as the Sun's rotation. Some elements of the nebular hypothesis are echoed in modern theories of planetary formation, but most elements have been superseded.According to the nebular hypothesis, stars form in massive and dense clouds of molecular hydrogen—giant molecular clouds (GMC). These clouds are gravitationally unstable, and matter coalesces within them to smaller denser clumps, which then rotate, collapse, and form stars. Star formation is a complex process, which always produces a gaseous protoplanetary disk around the young star. This may give birth to planets in certain circumstances, which are not well known. Thus the formation of planetary systems is thought to be a natural result of star formation. A Sun-like star usually takes approximately 1 million years to form, with the protoplanetary disk evolving into a planetary system over the next 10-100 million years.The protoplanetary disk is an accretion disk that feeds the central star. Initially very hot, the disk later cools in what is known as the T tauri star stage; here, formation of small dust grains made of rocks and ice is possible. The grains eventually may coagulate into kilometer-sized planetesimals. If the disk is massive enough, the runaway accretions begin, resulting in the rapid—100,000 to 300,000 years—formation of Moon- to Mars-sized planetary embryos. Near the star, the planetary embryos go through a stage of violent mergers, producing a few terrestrial planets. The last stage takes approximately 100 million to a billion years.The formation of giant planets is a more complicated process. It is thought to occur beyond the so-called frost line, where planetary embryos mainly are made of various types of ice. As a result, they are several times more massive than in the inner part of the protoplanetary disk. What follows after the embryo formation is not completely clear. Some embryos appear to continue to grow and eventually reach 5–10 Earth masses—the threshold value, which is necessary to begin accretion of the hydrogen–helium gas from the disk. The accumulation of gas by the core is initially a slow process, which continues for several million years, but after the forming protoplanet reaches about 30 Earth masses (M⊕) it accelerates and proceeds in a runaway manner. Jupiter- and Saturn-like planets are thought to accumulate the bulk of their mass during only 10,000 years. The accretion stops when the gas is exhausted. The formed planets can migrate over long distances during or after their formation. Ice giants such as Uranus and Neptune are thought to be failed cores, which formed too late when the disk had almost disappeared.
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