J.F. Agui Fernandez, A. de Ugarte Postigo, C. Thone, S. Kobayashi, A. Rossi, K. Toma, M. Jelínek, D. A. Kann, S. Covino, K. Wiersema, D. Hartmann, P. Jakobsson, A. Martin-Carrillo, A. Melandri, M. De Pasquale, G. Pugliese, S. Savaglio, R. Starling, J. Strobl, M. Della Valle, S. de Wet, T. Zafar
{"title":"无尘伽马射线暴 210610B 中的线性偏振变化","authors":"J.F. Agui Fernandez, A. de Ugarte Postigo, C. Thone, S. Kobayashi, A. Rossi, K. Toma, M. Jelínek, D. A. Kann, S. Covino, K. Wiersema, D. Hartmann, P. Jakobsson, A. Martin-Carrillo, A. Melandri, M. De Pasquale, G. Pugliese, S. Savaglio, R. Starling, J. Strobl, M. Della Valle, S. de Wet, T. Zafar","doi":"10.1051/0004-6361/202348572","DOIUrl":null,"url":null,"abstract":"Long gamma-ray bursts (GRBs) are produced by the collapse of some very massive stars, that emit ultra-relativistic jets. When the jets collide with the interstellar medium they decelerate and generate the so-called afterglow emission, which has been observed to be polarised. We study the polarimetric evolution of the GRB\\,210610B afterglow, at $z=1.1341$. This allows us to evaluate the role of geometric and/or magnetic mechanisms in the GRB afterglow polarisation. We observed GRB\\,210610B using imaging polarimetry with CAFOS on the 2.2 m Calar Alto Telescope and FORS2 on the $4 m Very Large Telescope. Complementary optical spectroscopy was obtained with OSIRIS on the 10.4 m Gran Telescopio Canarias. We studied the GRB light-curve from X-rays to the optical bands and the Spectral Energy Distribution (SED). This allowed us to strongly constrain the line-of-sight extinction. Finally, we studied the GRB host galaxy using optical to NIR data to fit the SED and derive its integrated properties. GRB\\,210610B had a bright afterglow with a negligible line-of-sight extinction. Polarimetry was obtained at three epochs: during an early plateau phase, at the time when the light curve breaks, and after the light curve steepened. We observe an initial polarisation of $ that goes to zero at the time of the break, and it then again increases to $ with a change in the position angle of $54 deg. The spectrum shows features with very low equivalent widths. This indicate a small amount of material in the line of sight within the host. The lack of dust and the low amount of material in the line of sight to GRB\\,210610B allowed us to study the intrinsic polarisation of the GRB optical afterglow. The GRB polarisation signals are consistent with ordered magnetic fields in refreshed shock or/and hydrodynamics-scale turbulent fields in the forward shock.","PeriodicalId":8585,"journal":{"name":"Astronomy & Astrophysics","volume":"11 7","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-07-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Varying linear polarisation in the dust-free gamma-ray burst 210610B\",\"authors\":\"J.F. Agui Fernandez, A. de Ugarte Postigo, C. Thone, S. Kobayashi, A. Rossi, K. Toma, M. Jelínek, D. A. Kann, S. Covino, K. Wiersema, D. Hartmann, P. Jakobsson, A. Martin-Carrillo, A. Melandri, M. De Pasquale, G. Pugliese, S. Savaglio, R. Starling, J. Strobl, M. Della Valle, S. de Wet, T. Zafar\",\"doi\":\"10.1051/0004-6361/202348572\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Long gamma-ray bursts (GRBs) are produced by the collapse of some very massive stars, that emit ultra-relativistic jets. When the jets collide with the interstellar medium they decelerate and generate the so-called afterglow emission, which has been observed to be polarised. We study the polarimetric evolution of the GRB\\\\,210610B afterglow, at $z=1.1341$. This allows us to evaluate the role of geometric and/or magnetic mechanisms in the GRB afterglow polarisation. We observed GRB\\\\,210610B using imaging polarimetry with CAFOS on the 2.2 m Calar Alto Telescope and FORS2 on the $4 m Very Large Telescope. Complementary optical spectroscopy was obtained with OSIRIS on the 10.4 m Gran Telescopio Canarias. We studied the GRB light-curve from X-rays to the optical bands and the Spectral Energy Distribution (SED). This allowed us to strongly constrain the line-of-sight extinction. Finally, we studied the GRB host galaxy using optical to NIR data to fit the SED and derive its integrated properties. GRB\\\\,210610B had a bright afterglow with a negligible line-of-sight extinction. Polarimetry was obtained at three epochs: during an early plateau phase, at the time when the light curve breaks, and after the light curve steepened. We observe an initial polarisation of $ that goes to zero at the time of the break, and it then again increases to $ with a change in the position angle of $54 deg. The spectrum shows features with very low equivalent widths. This indicate a small amount of material in the line of sight within the host. The lack of dust and the low amount of material in the line of sight to GRB\\\\,210610B allowed us to study the intrinsic polarisation of the GRB optical afterglow. The GRB polarisation signals are consistent with ordered magnetic fields in refreshed shock or/and hydrodynamics-scale turbulent fields in the forward shock.\",\"PeriodicalId\":8585,\"journal\":{\"name\":\"Astronomy & Astrophysics\",\"volume\":\"11 7\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-07-29\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Astronomy & Astrophysics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1051/0004-6361/202348572\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Astronomy & Astrophysics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1051/0004-6361/202348572","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Varying linear polarisation in the dust-free gamma-ray burst 210610B
Long gamma-ray bursts (GRBs) are produced by the collapse of some very massive stars, that emit ultra-relativistic jets. When the jets collide with the interstellar medium they decelerate and generate the so-called afterglow emission, which has been observed to be polarised. We study the polarimetric evolution of the GRB\,210610B afterglow, at $z=1.1341$. This allows us to evaluate the role of geometric and/or magnetic mechanisms in the GRB afterglow polarisation. We observed GRB\,210610B using imaging polarimetry with CAFOS on the 2.2 m Calar Alto Telescope and FORS2 on the $4 m Very Large Telescope. Complementary optical spectroscopy was obtained with OSIRIS on the 10.4 m Gran Telescopio Canarias. We studied the GRB light-curve from X-rays to the optical bands and the Spectral Energy Distribution (SED). This allowed us to strongly constrain the line-of-sight extinction. Finally, we studied the GRB host galaxy using optical to NIR data to fit the SED and derive its integrated properties. GRB\,210610B had a bright afterglow with a negligible line-of-sight extinction. Polarimetry was obtained at three epochs: during an early plateau phase, at the time when the light curve breaks, and after the light curve steepened. We observe an initial polarisation of $ that goes to zero at the time of the break, and it then again increases to $ with a change in the position angle of $54 deg. The spectrum shows features with very low equivalent widths. This indicate a small amount of material in the line of sight within the host. The lack of dust and the low amount of material in the line of sight to GRB\,210610B allowed us to study the intrinsic polarisation of the GRB optical afterglow. The GRB polarisation signals are consistent with ordered magnetic fields in refreshed shock or/and hydrodynamics-scale turbulent fields in the forward shock.