Перейти к основному содержанию
AkademIndex

Продукты

Для разработчиков

AkademBaseОткрытый API экосистемы
Статья

Detection of [C <scp>i</scp> ] Emission in Nebular Spectra of a Peculiar Type Ia Supernova 2022pul

Jialian LiuPhysics Department, Tsinghua University, Beijing 100084, People’s Republic of China; [email protected], [email protected]Xiaofeng WangPhysics Department, Tsinghua University, Beijing 100084, People’s Republic of China; [email protected], [email protected]Yi YangDepartment of Astronomy, University of California, Berkeley, CA 94720-3411, USAA. V. FilippenkoDepartment of Astronomy, University of California, Berkeley, CA 94720-3411, USAThomas G. BrinkDepartment of Astronomy, University of California, Berkeley, CA 94720-3411, USAWeiKang ZhengDepartment of Astronomy, University of California, Berkeley, CA 94720-3411, USAJujia ZhangInternational Centre of Supernovae, Yunnan Key Laboratory, Kunming 650216, People’s Republic of ChinaGaici LiPhysics Department, Tsinghua University, Beijing 100084, People’s Republic of China; [email protected], [email protected]Shengyu YanPhysics Department, Tsinghua University, Beijing 100084, People’s Republic of China; [email protected], [email protected]
2025en
ABI

Аннотация

Abstract SN 2022pul gains special attention due to its possible origin as a super-Chandrasekhar-mass white dwarf (WD) explosion (also called a 03fg-like Type Ia supernova), which shows prominent [O i ], [Ne i ], and [Ca ii ] lines in its late-time spectra taken at ∼+300 days after the time of peak brightness. In this Letter, we present new optical observations of this peculiar object, extending up to over 500 days after peak brightness. In particular, in the t ∼ +515 days spectrum, we identified for the first time the presence of narrow emission from [C i ] λλ 9824, 9850, which appears asymmetric and quite similar to the accompanied [O i ] λ 6300 line in strength and profile. Based on the violent merger model that accounts well for previous observations but leaves little carbon in the center of the ejecta, this carbon line can be reproduced by increasing the degree of clumping in the ejecta and setting the carbon mass the same as that of oxygen (∼0.06 M ⊙ ) in the innermost region (≲2000 km s −1 ). In principle, the central carbon could come from the secondary WD if it is ignited when hit by the shock wave of the explosion of the primary WD and explodes as a Ca-rich supernova, whereas pure deflagration of a super-Chandrasekhar-mass WD can account for such unburnt carbon more naturally.

Перевод пока недоступен

Идентификаторы

Цитирования и источники

Цитирований: 2Использованных источников: 0