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Article: GRB 110213A: A Study of Afterglow Electromagnetic Cascade Radiation
| Title | GRB 110213A: A Study of Afterglow Electromagnetic Cascade Radiation |
|---|---|
| Authors | Wang, Xiang GaoChen, Yuan ZhuoHuang, Xiao LiChen, Liang JunZheng, Wei KangD’Elia, ValerioPasquale, Massimiliano DePozanenko, Alexei S.Xin, Li PingStratta, GiuliaUkwatta, TilanAkerlof, CarlGeng, Jin JunHan, Xu HuiHentunen, Veli PekkaKlunko, E. V.M. Kuin, N. PaulNissinen, MarkkuRujopakarn, W.Rumyantsev, V. V.Rykoff, E. S.Salmi, TuomoSchaefer, B. E.Volnova, A. A.Wu, Xue FengWei, Jian YanLiang, En WeiZhang, BingFilippenko, Alexei V. |
| Issue Date | 2022 |
| Citation | Astrophysical Journal, 2022, v. 939, n. 1, article no. 39 How to Cite? |
| Abstract | We obtained well-sampled optical photometry of GRB 110213A, including Swift/UVOT and XRT. Combining our data from those of other ground-based telescopes, we present 15 optical multicolor light curves showing similar shapes with two peaks. In contrast, in the X-ray band, only a single peak is observed between the two optical peaks. Temporal and spectral analysis of GRB 110213A shows that the X-rays differ from the optical for Phases I-III (before the second peak of the optical band at ∼5.6 ks). Moreover, they have the same spectral behavior at late times (Phases IV-VI). These data indicate that the optical and X-ray emission are dominated by different components. The synchrotron-supported pair cascade emission is included in the standard external forward-shock model, which is dominated by synchrotron radiation and synchrotron self-Compton (SSC). We find that the optical bands of GRB 110213A are dominated by the cascade emission from synchrotron radiation + SSC at the early stage, while the primary synchrotron + SSC radiation dominates the X-ray band. At late stages, both the X-ray and optical bands are dominated by emission from primary synchrotron + SSC radiation. The cascade component can reasonably explain the first optical peak. In contrast, the primary synchrotron + SSC emission mainly contributes to the second peak. |
| Persistent Identifier | http://hdl.handle.net/10722/361686 |
| ISSN | 2023 Impact Factor: 4.8 2023 SCImago Journal Rankings: 1.905 |
| DC Field | Value | Language |
|---|---|---|
| dc.contributor.author | Wang, Xiang Gao | - |
| dc.contributor.author | Chen, Yuan Zhuo | - |
| dc.contributor.author | Huang, Xiao Li | - |
| dc.contributor.author | Chen, Liang Jun | - |
| dc.contributor.author | Zheng, Wei Kang | - |
| dc.contributor.author | D’Elia, Valerio | - |
| dc.contributor.author | Pasquale, Massimiliano De | - |
| dc.contributor.author | Pozanenko, Alexei S. | - |
| dc.contributor.author | Xin, Li Ping | - |
| dc.contributor.author | Stratta, Giulia | - |
| dc.contributor.author | Ukwatta, Tilan | - |
| dc.contributor.author | Akerlof, Carl | - |
| dc.contributor.author | Geng, Jin Jun | - |
| dc.contributor.author | Han, Xu Hui | - |
| dc.contributor.author | Hentunen, Veli Pekka | - |
| dc.contributor.author | Klunko, E. V. | - |
| dc.contributor.author | M. Kuin, N. Paul | - |
| dc.contributor.author | Nissinen, Markku | - |
| dc.contributor.author | Rujopakarn, W. | - |
| dc.contributor.author | Rumyantsev, V. V. | - |
| dc.contributor.author | Rykoff, E. S. | - |
| dc.contributor.author | Salmi, Tuomo | - |
| dc.contributor.author | Schaefer, B. E. | - |
| dc.contributor.author | Volnova, A. A. | - |
| dc.contributor.author | Wu, Xue Feng | - |
| dc.contributor.author | Wei, Jian Yan | - |
| dc.contributor.author | Liang, En Wei | - |
| dc.contributor.author | Zhang, Bing | - |
| dc.contributor.author | Filippenko, Alexei V. | - |
| dc.date.accessioned | 2025-09-16T04:19:13Z | - |
| dc.date.available | 2025-09-16T04:19:13Z | - |
| dc.date.issued | 2022 | - |
| dc.identifier.citation | Astrophysical Journal, 2022, v. 939, n. 1, article no. 39 | - |
| dc.identifier.issn | 0004-637X | - |
| dc.identifier.uri | http://hdl.handle.net/10722/361686 | - |
| dc.description.abstract | We obtained well-sampled optical photometry of GRB 110213A, including Swift/UVOT and XRT. Combining our data from those of other ground-based telescopes, we present 15 optical multicolor light curves showing similar shapes with two peaks. In contrast, in the X-ray band, only a single peak is observed between the two optical peaks. Temporal and spectral analysis of GRB 110213A shows that the X-rays differ from the optical for Phases I-III (before the second peak of the optical band at ∼5.6 ks). Moreover, they have the same spectral behavior at late times (Phases IV-VI). These data indicate that the optical and X-ray emission are dominated by different components. The synchrotron-supported pair cascade emission is included in the standard external forward-shock model, which is dominated by synchrotron radiation and synchrotron self-Compton (SSC). We find that the optical bands of GRB 110213A are dominated by the cascade emission from synchrotron radiation + SSC at the early stage, while the primary synchrotron + SSC radiation dominates the X-ray band. At late stages, both the X-ray and optical bands are dominated by emission from primary synchrotron + SSC radiation. The cascade component can reasonably explain the first optical peak. In contrast, the primary synchrotron + SSC emission mainly contributes to the second peak. | - |
| dc.language | eng | - |
| dc.relation.ispartof | Astrophysical Journal | - |
| dc.title | GRB 110213A: A Study of Afterglow Electromagnetic Cascade Radiation | - |
| dc.type | Article | - |
| dc.description.nature | link_to_subscribed_fulltext | - |
| dc.identifier.doi | 10.3847/1538-4357/ac937c | - |
| dc.identifier.scopus | eid_2-s2.0-85141681532 | - |
| dc.identifier.volume | 939 | - |
| dc.identifier.issue | 1 | - |
| dc.identifier.spage | article no. 39 | - |
| dc.identifier.epage | article no. 39 | - |
| dc.identifier.eissn | 1538-4357 | - |
