I discuss errors in theory and in interpreting observations that are produced by the failure to consider resolution in space, time, and energy. I discuss convection in stellar model atmospheres and in stars. Large errors in abundances are possible such as the factor of ten error in the Li abundance for extreme Population II stars. Finally I discuss the variation of microturbulent velocity with depth, effective temperature, gravity, and abundance. These variations must be dealt with in computing models and grids and in any type of photometric calibration. I have also developed a new opacity-sampling version of my model atmosphere program called ATLAS12. It recognizes more than 1000 atomic and molecular species, each in up to 10 isotopic form...
I describe recent progress in terms of 3D hydrodynamical model atmospheres and 3D line formation and...
The model atmosphere code STERNE has evolved considerably over the years. Most recently, attention h...
A grid of ATLAS9 model atmospheres has been computed, spanning 3500 K ≤ T_(eff) ≤ 8000 K, 0.0 ≤ log ...
I discuss errors in theory and in interpreting observations that are produced by the failure to cons...
Aims. In an effort to improve spectroscopic methods of stellar parameters determination, we implemen...
We present a new opacity sampling model atmosphere code, named MAFAGS-OS. This code, designed for ...
The model atmosphere code Sterne, first developed in the 1970s to study hydrogen-deficient stars, ha...
As stars evolve, their surfaces may be altered by several different mechanisms. These introduce dist...
Stellar model atmospheres form the basis for any element abundance determination and hence are cruci...
The revision of the standard Los Alamos opacities in the 1980–1990s by a group from the Lawren...
An opacity sampling (OS) technique for treating the radiative opacity of large numbers of atomic and...
International audienceAvailability of reliable atomic and molecular opacity tables is essential in a...
We present four model series of the CODEX dynamical opacity-sampling models of Mira variables with s...
Author Institution: Niels Bohr InstitueThe light that reach us from distant star, pass through a ``l...
We describe an opacity sampled version of the LTE model atmosphere code STERNE with revised continuo...
I describe recent progress in terms of 3D hydrodynamical model atmospheres and 3D line formation and...
The model atmosphere code STERNE has evolved considerably over the years. Most recently, attention h...
A grid of ATLAS9 model atmospheres has been computed, spanning 3500 K ≤ T_(eff) ≤ 8000 K, 0.0 ≤ log ...
I discuss errors in theory and in interpreting observations that are produced by the failure to cons...
Aims. In an effort to improve spectroscopic methods of stellar parameters determination, we implemen...
We present a new opacity sampling model atmosphere code, named MAFAGS-OS. This code, designed for ...
The model atmosphere code Sterne, first developed in the 1970s to study hydrogen-deficient stars, ha...
As stars evolve, their surfaces may be altered by several different mechanisms. These introduce dist...
Stellar model atmospheres form the basis for any element abundance determination and hence are cruci...
The revision of the standard Los Alamos opacities in the 1980–1990s by a group from the Lawren...
An opacity sampling (OS) technique for treating the radiative opacity of large numbers of atomic and...
International audienceAvailability of reliable atomic and molecular opacity tables is essential in a...
We present four model series of the CODEX dynamical opacity-sampling models of Mira variables with s...
Author Institution: Niels Bohr InstitueThe light that reach us from distant star, pass through a ``l...
We describe an opacity sampled version of the LTE model atmosphere code STERNE with revised continuo...
I describe recent progress in terms of 3D hydrodynamical model atmospheres and 3D line formation and...
The model atmosphere code STERNE has evolved considerably over the years. Most recently, attention h...
A grid of ATLAS9 model atmospheres has been computed, spanning 3500 K ≤ T_(eff) ≤ 8000 K, 0.0 ≤ log ...