scholarly journals The luminosity function of nearby thick-disk sub-dwarfs

2007 ◽  
Vol 3 (S248) ◽  
pp. 484-485
Author(s):  
M. I. Arifyanto

AbstractWe derived the luminosity function of thick disk using V/Vmax method for nearby sub-dwarf stars based on the sample stars of Carney et al. (1994). Hipparcos parallaxes and proper motions and Tycho2 proper motions were combined with radial velocities and metallicities from CLLA. We found that the luminosity function in the absolute magnitude range MV = 4–6 mag agree well with the luminosity function derived from the initial mass function (Reyle & Robin 2001).

1998 ◽  
Vol 115 (5) ◽  
pp. 1946-1957 ◽  
Author(s):  
Jon A. Holtzman ◽  
Alan M. Watson ◽  
William A. Baum ◽  
Carl J. Grillmair ◽  
Edward J. Groth ◽  
...  

2011 ◽  
Vol 2011 ◽  
pp. 1-9 ◽  
Author(s):  
W. H. Elsanhoury ◽  
M. A. Hamdy ◽  
M. I. Nouh ◽  
A. S. Saad ◽  
S. M. Saad

We investigated the luminosity function (LF) and initial mass function (IMF) of some open clusters having different ages. To calculate the LF, we followed the classical definition by van Rhijn (1936). Statistical investigation of the dispersion around a range of magnitudes concerning what is called Wielen dip revealed that the dip is unreal. To confirm the unreality of the dip, we computed the IMF for these open clusters, the statistical investigation of the IMF confirmed the results obtained using the LF, that is, there is no dip for these open clusters under study.


2010 ◽  
Vol 56 ◽  
pp. 391-399
Author(s):  
Yervant Terzian

Edwin E. Salpeter was a towering figure in twentieth-century astrophysics. Among his major scientific accomplishments is his 1955 paper ‘The luminosity function and stellar evolution’, where he first derived the empirical stellar initial mass function and estimated the probability for the creation of stars of given mass at a particular time, known as the Salpeter initial mass function. Just before this major achievement he had explained how giant stars burn helium to form carbon in the triple-alpha process, in which three helium nuclei combine to form carbon. This crucial step opened the path for the formation of elements as heavy as iron in the core of the stars. Salpeter showed the way to put physics into astronomy, and astrophysics has made enormous strides to understand the Universe. He once observed that most successful scientists are golf players; that is, they map out their own strategy and then write a unified theory. Salpeter said that he belonged to the minority of scientists who are Ping-pong players that react to influences from outside players. This approach made Salpeter a generalist.


1999 ◽  
Vol 190 ◽  
pp. 254-256 ◽  
Author(s):  
M. Sirianni ◽  
A. Nota ◽  
C. Leitherer ◽  
M. Clampin ◽  
G. De Marchi

Multiple images of the R136 cluster in the Large Magellanic Cloud taken with the HST/WFPC2 and the F555W and F814W filters were combined to obtain very deep images of the cluster, with total exposure times of 1240 and 760 sec respectively. The objective of the study was to extend the luminosity function below the limit of 2.8 M⊙ published by Hunter et al. (1995, 1996).


2013 ◽  
pp. 19-41
Author(s):  
R. Caimmi

Linear [Q/H]-[O/H] relations, Q = Na, Mg, Si, Ca, Ti, Cr, Fe, Ni, are inferred from a sample (N = 67) of recently studied FGK-type dwarf stars in the solar neighbourhood including different populations (Nissen and Schuster 2010, Ramirez et al. 2012), namely LH (N = 24, low-? halo), HH (N = 25, high-? halo), KD (N = 16, thick disk), and OL (N = 2, globular cluster outliers). Regression line slope and intercept estimators and related variance estimators are determined. With regard to the straight line, [Q/H]=aQ[O/H]+bQ, sample stars are displayed along a "main sequence", [Q,O] = [aQ, bQ, ?bQ], leaving aside the two OL stars, which, in most cases (e.g. Na), lie outside. The unit slope, aQ = 1, implies Q is a primary element synthesised via SNII progenitors in the presence of a universal stellar initial mass function (defined as simple primary element). In this respect, Mg, Si, Ti, show ?Q = 1 within -+2^??Q; Cr, Fe, Ni, within -+3^??Q; Na, Ca, within -+r^??Q, r > 3. The empirical, differential element abundance distributions are inferred from LH, HH, KD, HA = HH + KD subsamples, where related regression lines represent their theoretical counterparts within the framework of simple MCBR (multistage closed box + reservoir) chemical evolution models. Hence, the fractional yields, ^pQ/^pO, are determined and (as an example) a comparison is shown with their theoretical counterparts inferred from SNII progenitor nucleosynthesis under the assumption of a power-law stellar initial mass function. The generalized fractional yields, CQ=ZQ/ZaQ O, are determined regardless of the chemical evolution model. The ratio of outflow to star formation rate is compared for different populations in the framework of simple MCBR models. The opposite situation of element abundance variation entirely due to cosmic scatter is also considered under reasonable assumptions. The related differential element abundance distribution fits to the data, as well as its counterpart inferred in the opposite limit of instantaneous mixing in the presence of chemical evolution, while the latter is preferred for HA subsample.


1998 ◽  
Vol 508 (1) ◽  
pp. 347-369 ◽  
Author(s):  
K. L. Luhman ◽  
G. H. Rieke ◽  
C. J. Lada ◽  
E. A. Lada

2015 ◽  
Vol 800 (1) ◽  
pp. 72 ◽  
Author(s):  
Ingo Thies ◽  
Jan Pflamm-Altenburg ◽  
Pavel Kroupa ◽  
Michael Marks

2016 ◽  
Vol 465 (1) ◽  
pp. 192-212 ◽  
Author(s):  
Simon Zieleniewski ◽  
Ryan C. W. Houghton ◽  
Niranjan Thatte ◽  
Roger L. Davies ◽  
Sam P. Vaughan

2016 ◽  
Vol 57 (2) ◽  
pp. 2.32-2.36 ◽  
Author(s):  
Ignacio Ferreras ◽  
Francesco La Barbera ◽  
Alexandre Vazdekis

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