Cosmic Filaments and the Birth of Stars express

Original: "A Salpeter-like filament linear density function across nearby molecular clouds"
arXiv:2604.14093 · 2026-04-15 · CC BY 4.0 · 1 min
Cold gas filaments in space turn out to mirror the mass distribution of newborn stars.

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Hidden in cold interstellar gas clouds are long, thin filaments, like threads in a tangle. It is within these filaments, as they collapse, that new stars are born. Astronomers selected seven such clouds, located between 140 and 920 light-years away, and counted how many filaments of various thicknesses each contains.

Strikingly, in every cloud, regardless of its level of activity, the same rule applies: the thicker the filament, the rarer it is. Plotting the data yields nearly a straight line with a slope of 1.40. Remarkably, this slope almost matches the value 1.35—the same number that describes how many stars of different masses are born.

Filaments act like highways along which gas flows toward star-forming sites. Their thickness dictates how much material ends up in a future star.

The matching slopes are no coincidence. It seems that the hierarchy of gas filaments, from thin to thick, directly determines which stars will emerge: light, intermediate, or heavy. This links the structure of cold gas to the long-standing puzzle of the stellar mass distribution, which has defied explanation since 1955.

Original abstract

as written by the authors arXiv:2604.14093

The high-mass slope of the stellar initial mass function (IMF), first measured by Salpeter in 1955, appears nearly universal across star-forming environments, yet its physical origin remains unknown. Using the multiscale extraction method getsf, we measure the filament linear density function (FLDF) across seven nearby molecular clouds ($$140-920$$ pc) spanning a wide range of star-forming activity. The FLDF slope shows no systematic trend with spatial scale. Combining all clouds and scales, the composite FLDF follows a power law $${\rm d}N/{\rm d}\log\Lambda \propto \Lambda^{-\alpha}$$ with $$\alpha \approx 1.40$$, close to the Salpeter value of $$1.35$$, and the same composite slope is found in every cloud despite an order-of-magnitude spread in their supercritical-filament fractions. The close similarity between the composite FLDF slope and the Salpeter value suggests a possible physical link between the hierarchical filamentary structure of the cold interstellar medium and the IMF.

The stellar mass distribution law was first derived by Edwin Salpeter in 1955. Since then, it has been observed in many corners of the universe, but why it takes this particular form has remained a mystery.

Scientists
James JeansSubrahmanyan ChandrasekharAdam RiessJohn Archibald WheelerTheodore LymanHans Bethe
Concepts
initial mass function star formation rate interplanetary magnetic field point spread function