论文标题

可能的GRB祖细胞的磁核核心崩溃。 ii。原磁和折叠的形成

Magnetorotational core collapse of possible GRB progenitors. II. Formation of protomagnetars and collapsars

论文作者

Aloy, Miguel-Ángel, Obergaulinger, Martin

论文摘要

我们在旋转程度和选定前苏佩诺诺娃核的旋转程度和磁场的较小变化下,评估紧凑,巨大,低金属恒星的后爆发后进化遗迹的方差。这些恒星模型通常被认为是长伽马射线爆发的祖细胞。倒塌后形成的原始中子恒星(PNS)的命运,其质量可能由于积聚而不断增长,严重取决于反弹时的poloidal磁场强度。如果多型磁场足够弱,则PNS在几秒钟内倒入黑洞(BH)。此进化轨道上的模型包含有希望的折叠引擎。在较大的径向尺度(例如偶极场)上平滑或相对于原始的supernova核心产生长期持久的PNSS,多型磁场平滑。在这些模型中,长期避免或养成BH的形成,因此它们可能会产生原始磁力(PMS)。我们的一些PM候选人在核心反弹后以$ \ Lessim 10 \的价格运行,但他们尚未进入Kelvin-Helmholtz阶段。在这些模型中,一些显示旋转的情节事件在此期间,我们发现属性与PMS的理论期望($ m_ {pns} \大约1.85 \,m_ \ odot -2.5 \,m_ \ odot $,m_ \ odot $冲浪} _ {pns} \ Lessim 10^{15} \,$ g),他们非常准直的超新星弹射器几乎达到了恒星表面,而(仍在增长)爆炸能量$ \ gtrsim 2 \ times times times times times times times times times times 10^{51}}} \,$ erg。

We assess the variance of the post-collapse evolution remnants of compact, massive, low-metallicity stars, under small changes in the degrees of rotation and magnetic field of selected pre-supernova cores. These stellar models are commonly considered progenitors of long gamma-ray bursts. The fate of the proto-neutron star (PNS) formed after collapse, whose mass may continuously grow due to accretion, critically depends on the poloidal magnetic field strength at bounce. Should the poloidal magnetic field be sufficiently weak, the PNS collapses to a black hole (BH) within a few seconds. Models on this evolutionary track contain promising collapsar engines. Poloidal magnetic fields smooth over large radial scales (e.g. dipolar fields) or slightly augmented with respect to the original pre-supernova core yield long-lasting PNSs. In these models, BH formation is avoided or staved off for a long time, hence, they may produce proto-magnetars (PMs). Some of our PM candidates have been run for $\lesssim 10\,$s after core bounce, but they have not entered the Kelvin-Helmholtz phase yet. Among these models, some display episodic events of spin-down during which we find properties broadly compatible with the theoretical expectations for PMs ($M_{PNS} \approx 1.85\,M_\odot - 2.5\,M_\odot$, $\bar{P}_{PNS} \approx 1.5 - 4\,$ms, and $b^{\rm surf}_{PNS} \lesssim 10^{15}\,$G) and their very collimated supernova ejecta has nearly reached the stellar surface with (still growing) explosion energies $\gtrsim 2\times 10^{51}\,$erg.

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