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A PCA approach to stellar effective temperatures⋆
A PCA approach to stellar effective temperatures⋆

... resolution spectroscopic analyses in the literature. When multiple values are available from different sources, the library catalog adopts a weighted average, giving preference to data with smaller errors. The goal is to end up with a homogeneous set of values for all parameters. Quality flags (Q) ar ...
December - Weasner
December - Weasner

... 924 (20 Gem). The following four doubles were best seen at high power: 38 Gem (white and bluish), Kappa (yellowish and bluish), STF 1035 (yellowish and bluish), and Delta (yellowish and lilac). I took another look at Castor at high power, and this time I spotted a companion star well to the south of ...
Document
Document

... • For M=105 Msun, b=1pc, show the central escape velocity = (GM/b)1/2 ~ 20km/s. • Argue why M must be the total mass. What fraction of the total mass is inside radius r=b=1pc? Calculate the local Vcir(b) and Vesc(b) and acceleration g(b). What is your unit of g? Draw log-log diagram of Vcir(r). • Wh ...
Optical and Infrared Colors of Stars Observed by the
Optical and Infrared Colors of Stars Observed by the

... whose listed positions agree to better than 2A. There are 63,341 such sources, or 97.9% of the 2MASS PSC sources and 8% of the SDSS sources, in the overlapping area. The probability of Ðnding an SDSS source within a circle with 2A radius is D1%, and the probability of associating a 2MASS source with ...
Explosion and Systematics for Core
Explosion and Systematics for Core

... including the effect of mass loss during the presupernova evolution which was neglected in Woosley and Weaver [1995] and increasing the number of progenitors studied. The predictions from all these works are summarized by Heger et al. [2003] in the diagram that is shown in Figure 1.1, which represen ...
Duplicity and masses
Duplicity and masses

... stars brighter than 14, the volume from which a complete sample can be extracted is limited by the apparent magnitude, not by the astrometric precision on distance. This limiting distance is about 500 pc for G stars, while it will be 150 pc for K stars, neglecting the interstellar extinction. In ord ...
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... (a) are the disk of material left over from a star formation that will form its planets (b) are made of a close group of stars that are hard to resolve (c) Are exploded stars (d) are a nebula that has yet contracted to form a star ...
Population synthesis for symbiotic stars with white dwarf accretors
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... still experience non-degenerate carbon ignition, but avoid electron captures on Ne and Mg in the core. We assume after Pols et al. (1998) that for solar metallicity stars the corresponding range of masses is 6.1 – 7.9 M⊙ . However, the range of masses of ONe WD progenitors still remains uncertain an ...
Highligh in Physics 2005
Highligh in Physics 2005

... a “puffed-up“ rim at the dust destruction radius (Natta et al. 2001, Dullemond et al. 2001). The concept of such an inner rim has been widely used to interpret near-IR interferometric data for Herbig Ae stars and T Tauri stars (low mass young stellar objects). To better understand the structure of t ...
Fundamentals of Stellar Evolution Theory: Understanding the HRD
Fundamentals of Stellar Evolution Theory: Understanding the HRD

... luminosity. The star climbs the RGB (Hayashi line), while convection in the outer layers gets deeper and deeper, eventually reaching those layers that were nuclearly processed in previous stages and generating a discontinuity in the chemical profile (first dredge-up). The steady outward migration of ...
Binary progenitor models of type IIb supernovae
Binary progenitor models of type IIb supernovae

... Massive stars that lose their hydrogen-rich envelope down to a few tenths of a solar mass explode as extended type IIb supernovae, an intriguing subtype that links the hydrogen-rich type II supernovae with the hydrogen-poor type Ib and Ic. The progenitors may be very massive single stars that lose t ...
1. INTRODUCTION 2. MASS AND LIGHT
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Turbulent Flow-Driven Molecular Cloud Formation: A Solution to the
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... by our MHD numerical simulations, in which large-scale H I streams collide to produce dense filamentary structures. This rapid evolution is possible because the H I flows producing and disrupting the cloud have much higher velocities (5-10 km s−1 ) than present in the molecular gas resulting from th ...
Model Atmosphere Results (Kurucz 1979, ApJS, 40, 1)
Model Atmosphere Results (Kurucz 1979, ApJS, 40, 1)

... • Teff = 5500 to 50000 K No cooler models since molecular opacities largely ignored. Models for Teff > 30000 K need non-LTE treatment (also in supergiants) • log g from main sequence to lower limit set by radiation pressure (see Fitzpatrick 1987, ApJ, 312, 596 for extensions) • Abundances 1, 1/10, 1 ...
SN 2011dh and the progenitors of Type IIb supernovae Mattias Ergon
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... decreasing temperature, and each class is further subdivided into subclasses 0-91 . In the MK system the Sun, Vega, Betelgeuse, and the progenitor star of SN 2011dh (Paper I) are of types G2, A0, M2, and F8, respectively. To visualize the observed properties, a Hertzsprung-Russel (HR) diagram is oft ...
Classical Oe Stars in the Field of the Small Magellanic Cloud
Classical Oe Stars in the Field of the Small Magellanic Cloud

... stellar winds and radiative feedback, which shock heat and ionize the surrounding gas, injecting energy into the interstellar medium (ISM). Moreover, when massive stars end their lives as core-collapse supernovae, the shockwaves can trigger or suppress star formation while enriching the ISM with met ...
Synergies between E-ELT and space instrumentation for
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Astronomy Astrophysics - Max Planck Institut für Radioastronomie
Astronomy Astrophysics - Max Planck Institut für Radioastronomie

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Dynamical Interactions Make Hot Jupiters in Open Star Clusters
Dynamical Interactions Make Hot Jupiters in Open Star Clusters

... In all standard simulations the outer Jupiters commonly migrate inwards to as close as a = 7.5 AU and outwards to as far as a = 12 AU. The former value means that outer Jupiters reach close to the dynamical stability limit for inner Jupiters that have not migrated. Some of the inner Jupiters migrate ...
Discussion Session A: “Evidence”
Discussion Session A: “Evidence”

... •  A)  Correla8ons  between  nuclear  SFR  and   instantaneous  LAGN   •  B)  Correla8on  of  SFR  and  average  LAGN  (or  BH   accre8on  rate)   •  C)    Increased  AGN  frac'on  in  SF  galaxies   •  D)  Radio  AGN  are  associated   ...
Draft paper (Published in ApJL)
Draft paper (Published in ApJL)

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Gaia - STScI
Gaia - STScI

... Huge impact on most other astronomical disciplines. But – Game Over! when Gaia publishes Intermediate catalog. • Anticipate mas astrometry, mmag photometry over all sky. • Guess: Release is politically and scientifically important. • Guess: As early as is reasonable – 2015 or 2016. ...
The chemical case for no winds in dwarf irregular galaxies
The chemical case for no winds in dwarf irregular galaxies

... of cloud formation,  μ , and cloud collision,  H (see Mollá & Dı́az 2005, for further details). Thus, the number of free parameters is reduced to three: τ ,  μ and  H . It is important to stress that the SFR is not an input of the model, but a result of the efficiencies selected and the amount ...
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... Just first 2 minutes https://www.youtube.com/watch?v=01U7ZUKVW8o https://www.youtube.com/watch?v=N3IgVidGjQk https://www.youtube.com/watch?v=Rj1sDWjvgjM ...
Massive Star Formation in the Galactic Center
Massive Star Formation in the Galactic Center

... 3. Present-day star formation in the GC Present-day star formation in the GC is somewhat subdued compared to the episodes that produced the massive clusters we now see. A dozen or so ultra-compact HII regions are distributed throughout the central 50 pc, each containing one or a few O-stars still em ...
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Main sequence



In astronomy, the main sequence is a continuous and distinctive band of stars that appears on plots of stellar color versus brightness. These color-magnitude plots are known as Hertzsprung–Russell diagrams after their co-developers, Ejnar Hertzsprung and Henry Norris Russell. Stars on this band are known as main-sequence stars or ""dwarf"" stars.After a star has formed, it generates thermal energy in the dense core region through the nuclear fusion of hydrogen atoms into helium. During this stage of the star's lifetime, it is located along the main sequence at a position determined primarily by its mass, but also based upon its chemical composition and other factors. All main-sequence stars are in hydrostatic equilibrium, where outward thermal pressure from the hot core is balanced by the inward pressure of gravitational collapse from the overlying layers. The strong dependence of the rate of energy generation in the core on the temperature and pressure helps to sustain this balance. Energy generated at the core makes its way to the surface and is radiated away at the photosphere. The energy is carried by either radiation or convection, with the latter occurring in regions with steeper temperature gradients, higher opacity or both.The main sequence is sometimes divided into upper and lower parts, based on the dominant process that a star uses to generate energy. Stars below about 1.5 times the mass of the Sun (or 1.5 solar masses (M☉)) primarily fuse hydrogen atoms together in a series of stages to form helium, a sequence called the proton–proton chain. Above this mass, in the upper main sequence, the nuclear fusion process mainly uses atoms of carbon, nitrogen and oxygen as intermediaries in the CNO cycle that produces helium from hydrogen atoms. Main-sequence stars with more than two solar masses undergo convection in their core regions, which acts to stir up the newly created helium and maintain the proportion of fuel needed for fusion to occur. Below this mass, stars have cores that are entirely radiative with convective zones near the surface. With decreasing stellar mass, the proportion of the star forming a convective envelope steadily increases, whereas main-sequence stars below 0.4 M☉ undergo convection throughout their mass. When core convection does not occur, a helium-rich core develops surrounded by an outer layer of hydrogen.In general, the more massive a star is, the shorter its lifespan on the main sequence. After the hydrogen fuel at the core has been consumed, the star evolves away from the main sequence on the HR diagram. The behavior of a star now depends on its mass, with stars below 0.23 M☉ becoming white dwarfs directly, whereas stars with up to ten solar masses pass through a red giant stage. More massive stars can explode as a supernova, or collapse directly into a black hole.
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