SIMBAD references

In turbulent fragmentation, star formation occurs in condensations created by converging flows. The condensations must be sufficiently massive, dense and cool to be gravitationally unstable, so that they start to contract; and they must then radiate away thermal energy fast enough for self-gravity to remain dominant, so that they continue to contract. For the metallicities and temperatures in local star-forming clouds, this second requirement is only met robustly when the gas couples thermally to the dust, because this delivers the capacity to radiate across the full bandwidth of the continuum, rather than just in a few discrete spectral lines. This translates into a threshold for vigorous star formation, which can be written as a minimum ram pressure P_CRIT ∼ 4 x 10^–11 dyne. P_CRIT is independent of temperature, and corresponds to flows with molecular hydrogen number density and velocity v_FLOW satisfying . This in turn corresponds to a minimum molecular hydrogen column density for vigorous star formation, (Σ_CRIT ∼ 100 M_☉ pc^–2), and a minimum visual extinction A_V, CRIT_ ∼ 9 mag. The characteristic diameter and line density for a star-forming filament when this threshold is just exceeded - a sweet spot for local star formation regions - are 2R_FIL ∼ 0.1 pc and µ_FIL ∼ 13 M_☉ pc^–2. The characteristic diameter and mass for a prestellar core condensing out of such a filament are 2R_CORE ∼ 0.1 pc and M_CORE ∼ 1 M_☉. We also show that fragmentation of a shock-compressed layer is likely to commence while the convergent flows creating the layer are still ongoing, and we stress that, under this circumstance, the phenomenology and characteristic scales for fragmentation of the layer are fundamentally different from those derived traditionally for pre-existing layers.