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Table 1
Different runs.
| Name | B0 (μ G) | Vshear (km s−1 kpc−1) | Particularities |
|---|---|---|---|
| noSH_hydro | 0 | 0 | – |
| SH14_hydro | 0 | 14 | – |
| SH28_hydro | 0 | 28 | – |
| SH28_hydro_VSAT_TSAT | 0 | 28 | Increased Tsat and Vsat |
| SH56_hydro | 0 | 56 | – |
| noSH_mhd | 4 | 0 | – |
| SH14_mhd | 4 | 14 | – |
| SH28_mhd | 4 | 28 | – |
| SH28_mhd_VSAT_TSAT | 4 | 28 | Increased Tsat and Vsat |
| SH28_mhd_vdisp | 4 | 28 | The massive stars are motionless around the sinks |
| SH28_mhd_lowsinkthres | 4 | 28 | The creation and accretion threshold of the sinks is 4x lower |
| SH28_mhd_highsinkthres | 4 | 28 | The creation and accretion threshold of the sinks is 4x higher |
| SH28_mhd_nosn | 4 | 28 | No supernovae feedback |
| SH28_mhd_nort | 4 | 28 | No H II regions feedback |
| SH28_mhd_nort_nosn | 4 | 28 | No H II and supernovae feedback |
| SH56_mhd | 4 | 56 | – |
| SH28_mhd_512 | 4 | 28 | Resolution 5123 |
| SH56_mhd_512 | 4 | 56 | Resolution 5123 |
| noSH_mhd_novir | 4 | 0 | No virial tests for the sink particles (see Sect. 2.5) |
| noSH_mhd_novir_trueperiodic | 4 | 0 | No virial tests, true periodic boundary conditions for gravity |
| SH28_mhd_novir | 4 | 28 | No virial tests |
| SH28_mhd_novir_lowsinkthres | 4 | 28 | No virial tests and the threshold of the sinks is 4x lower |
| SH28_mhd_novir_highsinkthres | 4 | 28 | No virial tests and the threshold of the sinks is 4x higher |
| SH56_mhd_novir | 4 | 56 | No virial tests |
Notes. Section 2.6 gives the meaning of Tsat and Vsat. The case Vshear = 28 km s−1 kpc−1 corresponds to the value near the Sun (see Sect. 3.2).
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