Occurrence rate of stellar Type II radio bursts from a 100 star-year search for coronal mass ejections
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| Autores principales: | , , , , , , , , , , |
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| Formato: | Preprint |
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2025
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| _version_ | 1866915626520412160 |
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| author | Konijn, David C. Vedantham, Harish K. Tasse, Cyril Shimwell, Timothy W. Hardcastle, Martin J. Callingham, Joseph R. Ilin, Ekaterina Drabent, Alexander Zarka, Philippe van der Tak, Floris F. S. Bloot, Sanne |
| author_facet | Konijn, David C. Vedantham, Harish K. Tasse, Cyril Shimwell, Timothy W. Hardcastle, Martin J. Callingham, Joseph R. Ilin, Ekaterina Drabent, Alexander Zarka, Philippe van der Tak, Floris F. S. Bloot, Sanne |
| contents | Coronal mass ejections (CMEs) are major drivers of space weather in the Solar System, but their occurrence rate on other stars is unknown. A characteristic (deca-)metric radio burst with a time-frequency drift, known as a Type II radio burst, is a key observational signature of CMEs. We searched a total of 107 years of stellar data using time-frequency spectra that targeted all known stars within 100 parsecs in the LOFAR Two Metre Sky Survey (LoTSS) up to May 2023. This resulted in the largest unbiased search for circularly polarised stellar Type II metric radio bursts to date, with a typical 3$σ$ sensitivity of 2.5 mJy for an integration time of 1 minute. We detected two drifting stellar radio bursts: the published 2-minute burst from the M dwarf StKM 1-1262 and a new 13-minute burst from the M dwarf LP 215-56. The new burst is characterised by a drift rate of $-0.060^{+0.002}_{-0.002}$ MHz s$^{-1}$, an average Stokes V flux density of $-4.5^{+1.4}_{-1.3}$ mJy, and a temporal duration of $63^{+31}_{-11}$ seconds. We constrained the occurrence rate of drifting stellar bursts by calculating Poisson upper and lower limits based on the two drifting bursts. We also fitted a cumulative burst luminosity distribution to the data using the burst detections and the non-detections; this yielded a power law index ($α$) of $-0.7^{+0.9}_{-0.6}$ and a normalisation point (N) of one burst per year with $E>6.8\times10^{13}$ erg s$^{-1}$ Hz$^{-1}$. We find an agreement between this and the cumulative luminosity distribution of decametric SOHO/LASCO solar Type II data ($α= -0.81 \pm 0.06 \pm 0.02$), which suggests that the current scarcity of detected stellar Type II bursts is likely due to limited sensitivity rather than to the intrinsic rarity of these events. Additionally, we identify 19 circularly polarised stellar radio bursts without a time-frequency drift. |
| format | Preprint |
| id |
arxiv_https___arxiv_org_abs_2511_09296 |
| institution | arXiv |
| publishDate | 2025 |
| record_format | arxiv |
| spellingShingle | Occurrence rate of stellar Type II radio bursts from a 100 star-year search for coronal mass ejections Konijn, David C. Vedantham, Harish K. Tasse, Cyril Shimwell, Timothy W. Hardcastle, Martin J. Callingham, Joseph R. Ilin, Ekaterina Drabent, Alexander Zarka, Philippe van der Tak, Floris F. S. Bloot, Sanne Solar and Stellar Astrophysics Earth and Planetary Astrophysics Coronal mass ejections (CMEs) are major drivers of space weather in the Solar System, but their occurrence rate on other stars is unknown. A characteristic (deca-)metric radio burst with a time-frequency drift, known as a Type II radio burst, is a key observational signature of CMEs. We searched a total of 107 years of stellar data using time-frequency spectra that targeted all known stars within 100 parsecs in the LOFAR Two Metre Sky Survey (LoTSS) up to May 2023. This resulted in the largest unbiased search for circularly polarised stellar Type II metric radio bursts to date, with a typical 3$σ$ sensitivity of 2.5 mJy for an integration time of 1 minute. We detected two drifting stellar radio bursts: the published 2-minute burst from the M dwarf StKM 1-1262 and a new 13-minute burst from the M dwarf LP 215-56. The new burst is characterised by a drift rate of $-0.060^{+0.002}_{-0.002}$ MHz s$^{-1}$, an average Stokes V flux density of $-4.5^{+1.4}_{-1.3}$ mJy, and a temporal duration of $63^{+31}_{-11}$ seconds. We constrained the occurrence rate of drifting stellar bursts by calculating Poisson upper and lower limits based on the two drifting bursts. We also fitted a cumulative burst luminosity distribution to the data using the burst detections and the non-detections; this yielded a power law index ($α$) of $-0.7^{+0.9}_{-0.6}$ and a normalisation point (N) of one burst per year with $E>6.8\times10^{13}$ erg s$^{-1}$ Hz$^{-1}$. We find an agreement between this and the cumulative luminosity distribution of decametric SOHO/LASCO solar Type II data ($α= -0.81 \pm 0.06 \pm 0.02$), which suggests that the current scarcity of detected stellar Type II bursts is likely due to limited sensitivity rather than to the intrinsic rarity of these events. Additionally, we identify 19 circularly polarised stellar radio bursts without a time-frequency drift. |
| title | Occurrence rate of stellar Type II radio bursts from a 100 star-year search for coronal mass ejections |
| topic | Solar and Stellar Astrophysics Earth and Planetary Astrophysics |
| url | https://arxiv.org/abs/2511.09296 |