We present two grids of evolutionary stellar models covering the phases of core H- and He-burning for stars having masses in the range 0.6M. to 100M. with composition (Y = 0.25 and Z = 0.008). The computations were performed for two different mixing schemes in the convective regions, i.e. either the classical definition of the convective core during the central H-burning phase and semiconvection during the core He-burning phase or non local overshoot from convective regions all over the major nuclear phases. All the evolutionary models were computed from the main sequence up to the stage of central carbon ignition or to the beginning of the thermally pulsing regime of the asymptotic giant branch phase as appropriate to the value of the init...
We supplement recent evolutionary computations of canonical stellar models (i.e. with inefficient co...
We supplement recent evolutionary computations of canonical stellar models (i.e. with inefficient co...
Uncertainties on central mixing in main-sequence (MS) and core He-burning (He-B) phases affect key p...
We present two grids of evolutionary stellar models covering the phases of core H- and He-burning fo...
The evolution of Pop I intermediate mass stars is followed from the zero-age main sequence until the...
We present a large grid of stellar evolutionary models with the initial chemical composition [Z = 0....
We present a large grid of stellar evolutionary models with the initial chemical composition [Z = 0....
We present a large grid of stellar evolutionary models with the initial chemical composition $[Z=0....
Massive stars are key sources of radiative, kinetic, and chemical feedback in the universe. Grids of...
We present a large grid of stellar evolutionary models with the initial chemical composition $[Z=0....
Massive stars are key sources of radiative, kinetic, and chemical feedback in the universe. Grids of...
Reliable evolutionary tracks are a backbone of stellar astrophysics; they are an essential ingredien...
The problem of determining the boundary of convective cores in massive stars (having a mass greater ...
Some models are computed for very massive stars (M=46.8MG) cons1stmg of four regions: (I) a homogene...
The models similar to those proposed by Sakashita and Hayashi to represent the main sequence evoluti...
We supplement recent evolutionary computations of canonical stellar models (i.e. with inefficient co...
We supplement recent evolutionary computations of canonical stellar models (i.e. with inefficient co...
Uncertainties on central mixing in main-sequence (MS) and core He-burning (He-B) phases affect key p...
We present two grids of evolutionary stellar models covering the phases of core H- and He-burning fo...
The evolution of Pop I intermediate mass stars is followed from the zero-age main sequence until the...
We present a large grid of stellar evolutionary models with the initial chemical composition [Z = 0....
We present a large grid of stellar evolutionary models with the initial chemical composition [Z = 0....
We present a large grid of stellar evolutionary models with the initial chemical composition $[Z=0....
Massive stars are key sources of radiative, kinetic, and chemical feedback in the universe. Grids of...
We present a large grid of stellar evolutionary models with the initial chemical composition $[Z=0....
Massive stars are key sources of radiative, kinetic, and chemical feedback in the universe. Grids of...
Reliable evolutionary tracks are a backbone of stellar astrophysics; they are an essential ingredien...
The problem of determining the boundary of convective cores in massive stars (having a mass greater ...
Some models are computed for very massive stars (M=46.8MG) cons1stmg of four regions: (I) a homogene...
The models similar to those proposed by Sakashita and Hayashi to represent the main sequence evoluti...
We supplement recent evolutionary computations of canonical stellar models (i.e. with inefficient co...
We supplement recent evolutionary computations of canonical stellar models (i.e. with inefficient co...
Uncertainties on central mixing in main-sequence (MS) and core He-burning (He-B) phases affect key p...