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Optical and near-infrared observations of SN 2023ixf for over 600 days after the explosion

Gaici LiDepartment of Physics, Tsinghua UniversityXiaofeng WangDepartment of Physics, Tsinghua UniversityYi YangDepartment of Astronomy, University of CaliforniaA. PastorelloINAF – Osservatorio Astronomico di PadovaA. ReguittiINAF – Osservatorio Astronomico di BreraG. ValerinINAF – Osservatorio Astronomico di PadovaP. OchnerDipartimento di Fisica e Astronomia, Università Degli Studi di PadovaYongzhi CaiInternational Centre of Supernovae, Yunnan Key LaboratoryT. IijimaINAF – Osservatorio Astronomico di PadovaU. MunariINAF – Osservatorio Astronomico di PadovaI. SalmasoINAF – Osservatorio Astronomico di PadovaA. FarinaDipartimento di Fisica e Astronomia, Università Degli Studi di PadovaR. CazzolaDipartimento di Fisica e Astronomia, Università Degli Studi di PadovaN. TrabacchinCISAS G. Colombo, University of PadovaS. FiscaleINAF, Osservatorio Astronomico di CapodimonteS. CiroiDipartimento di Fisica e Astronomia, Università Degli Studi di PadovaA. MuraDipartimento di Fisica e Astronomia, Università Degli Studi di PadovaA. SivieroDipartimento di Fisica e Astronomia, Università Degli Studi di PadovaF. CabrasDipartimento di Fisica e Astronomia, Università Degli Studi di PadovaM. PabstDipartimento di Fisica e Astronomia, Università Degli Studi di PadovaS. TaubenbergerMax-Planck-Institut fur AstrophysikC. VoglMax-Planck-Institut fur AstrophysikC. FiorinDipartimento di Fisica e Astronomia, Università Degli Studi di PadovaJ. LiuDepartment of Physics, Tsinghua UniversityL. ChenDepartment of Physics, Tsinghua UniversityDanfeng XiangBeijing Planetarium, Beijing Academy of Sciences and TechnologyJ. MoDepartment of Physics, Tsinghua UniversityL. LiInternational Centre of Supernovae, Yunnan Key LaboratoryZ. WangInternational Centre of Supernovae, Yunnan Key LaboratoryJujia ZhangInternational Centre of Supernovae, Yunnan Key LaboratoryQ. ZhaiKey Laboratory for the Structure and Evolution of Celestial Objects, Chinese Academy of SciencesD. O. MirzaqulovUlugh Beg Astronomical InstituteSh. A. EhgamberdievNational University of UzbekistanA. V. FilippenkoS. YanDepartment of Physics, Tsinghua UniversityM. HuDepartment of Physics, Tsinghua UniversityX. MaDepartment of Physics, Tsinghua UniversityQ. XiaDepartment of Physics, Tsinghua UniversityX. GaoXingming ObservatoryW. LiNational Astronomical Observatories, Chinese Academy of Sciences
ABI

Аннотация

Context. We present a comprehensive photometric and spectroscopic study of the nearby Type II supernova (SN) 2023ixf; our extensive observations span the phases from ∼3 to over 600 days after the first light. Aims. The aim of this study is to obtain key information on the explosion properties of SN 2023ixf and the nature of its progenitor. Methods. The observational properties of SN 2023ixf were compared with those of a representative sample of Type IIP and IIL SNe to investigate commonalities and diversities. We conducted a detailed analysis of the temporal evolution of major spectral features observed throughout different phases of the SN 2023ixf explosion. Several key interpretations are addressed through a comparison between the data and the model spectra predicted by nonlocal thermodynamic equilibrium (non-LTE) radiative-transfer calculations for progenitor stars within a range of zero-age main sequence (ZAMS) masses. Results. Our observations indicate that SN 2023ixf is a transitional SN that bridges the gap between the Type IIP and IIL subclasses of H-rich SNe; it is characterized by a relatively short plateau (≲70 d) in the light curve. It shows a rather prompt spectroscopic evolution toward the nebular phase; emission lines of Na, O, H, and Ca in nebular spectra all exhibit multi-peak profiles, which might be due to a bipolar distribution of the ejecta. In particular, the H α profile can be separated into two central peaked components (with velocities of about 1500 km s −1 ) that are likely due to nickel-powered ejecta and two outer box components (with velocities of up to ∼8000 km s −1 ) that can arise from interactions of the outermost ejecta with a circumstellar shell at a distance of ∼6.2 × 10 15 cm. The nebular-phase spectra of SN 2023ixf show good agreement with those predicted by a non-LTE radiative-transfer code for progenitor stars with ZAMS masses ranging from 15 to 19 M ⊙ . A distance of 6.35 +0.31 −0.39 Mpc is estimated for M101 based on the expanding photosphere method.

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