Issue |
A&A
Volume 643, November 2020
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|
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Article Number | C1 | |
Number of page(s) | 2 | |
Section | Letters to the Editor | |
DOI | https://doi.org/10.1051/0004-6361/201834222e | |
Published online | 09 November 2020 |
Letter to the Editor
Synchrotron emission in molecular cloud cores: the SKA view (Corrigendum)
INAF–Osservatorio Astrofisico di Arcetri, Largo E. Fermi 5, 50125 Firenze, Italy
e-mail: padovani@arcetri.astro.it, galli@arcetri.astro.it
Key words: ISM: clouds / ISM: magnetic fields / cosmic rays / errata / addenda
The specific intensity (Eq. (5)) has not been correctly evaluated1. This affects the computation of the flux densities, whose correct trends are shown in the new versions of Figs. 3 and 4. We recovered the signal-to-noise ratios (S/Ns) quoted in the paper by assuming a magnetic field strength B0 larger by a factor of 2.74 − 4.20, 2.02 − 2.72, and 1.55 − 1.80 than originally assumed for models A, B, and C, respectively (the lower and upper values corresponding to κ = 0.5 and κ = 0.7, respectively). The conclusions of the paper are unaffected.
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Fig. 3. Radial flux density profiles for the starless core models described in Sect. 5.1 (upper row) and for B68 and FeSt 1-457 (lower row, see Sect. 5.2). The observing frequency is shown in black at the top of each column, while numbers in the upper-right corner of each subplot represent the radius-averaged S/N for the two values of κ (0.5 and 0.7 for models A, B, C, and B68, and 0.68 and 0.88 for FeSt 1-457, see Eq. (9)). Shaded areas encompass the curves obtained with Eq. (9) by using the two values of κ (see Fig. 2 for colour-coding). The telescope beam is shown in the leftmost column for models A, B, and C (dotted black line, 300″), B68 (short-dashed black line, 330″), and FeSt 1-457 (long-dashed black line, 284″). Hatched areas display SKA sensitivities for one hour of integration at different frequencies. The two panels on the right side show the flux density as a function of frequency. Empty (solid) circles refer to an S/N smaller (larger) than 3, respectively. The spectral index α is shown on the right of each curve. |
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Fig. 4. Flux density at 60, 114, and 218 MHz (lower-left labels) as a function of magnetic field strength B0 for model B (see Sect. 5.1). Green shaded areas encompass the curves obtained with Eq. (9) by using κ = 0.5 and 0.7. Grey areas correspond to an S/N < 3 and dashed lines are power-law fits of |
© ESO 2020
All Figures
![]() |
Fig. 3. Radial flux density profiles for the starless core models described in Sect. 5.1 (upper row) and for B68 and FeSt 1-457 (lower row, see Sect. 5.2). The observing frequency is shown in black at the top of each column, while numbers in the upper-right corner of each subplot represent the radius-averaged S/N for the two values of κ (0.5 and 0.7 for models A, B, C, and B68, and 0.68 and 0.88 for FeSt 1-457, see Eq. (9)). Shaded areas encompass the curves obtained with Eq. (9) by using the two values of κ (see Fig. 2 for colour-coding). The telescope beam is shown in the leftmost column for models A, B, and C (dotted black line, 300″), B68 (short-dashed black line, 330″), and FeSt 1-457 (long-dashed black line, 284″). Hatched areas display SKA sensitivities for one hour of integration at different frequencies. The two panels on the right side show the flux density as a function of frequency. Empty (solid) circles refer to an S/N smaller (larger) than 3, respectively. The spectral index α is shown on the right of each curve. |
In the text |
![]() |
Fig. 4. Flux density at 60, 114, and 218 MHz (lower-left labels) as a function of magnetic field strength B0 for model B (see Sect. 5.1). Green shaded areas encompass the curves obtained with Eq. (9) by using κ = 0.5 and 0.7. Grey areas correspond to an S/N < 3 and dashed lines are power-law fits of |
In the text |
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