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arXiv 2402.06003astro-ph.HE
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旋转原磁星风中重元素核合成的有利条件

Favorable conditions for heavy element nucleosynthesis in rotating proto-magnetar winds

Tejas Prasanna, Matthew S. B. Coleman, Todd A. Thompson

AI总结:

该研究利用二维磁流体动力学模拟表明,快速旋转的原磁星风可准周期喷出高熵物质,并定量给出产生第三r过程峰及p核的有利磁场、周期与产量条件。

摘要:

原中子星(PNSs)的中微子驱动风冷却阶段发生在成功的超新星之后。不包含磁场或旋转的风模型无法达到产生第三r过程峰所需的条件,但会在富中子风中稳定产生弱r过程。通过采用具有磁星级强度磁场和旋转的二维磁流体动力学模拟,我们表明PNS旋转速率会显著影响风的热力学条件。我们表明,高熵物质从PNS磁层的闭合区准周期性地喷出,并具有产生重元素所需的热力学条件。我们表明,喷出物质的最大熵S系统地取决于磁星自转周期P_star,并且对于足够快的旋转,其标度关系为S ∝ P_star^(-5/6)。我们给出了在恒定中微子光度下的模拟结果,该光度代表冷却开始后约1–2秒,P_star范围为5 ms至200 ms;同时给出了若干中微子光度随时间演化的模拟,其中我们追踪磁星风的演化直至冷却开始后10–14秒。在磁星极区磁场强度B0=3×10^15 G和10^15 G时,我们估计富中子磁星风分别可产生至少约1–5×10^-5 M⊙和约1–4×10^-7 M⊙具有合成第三r过程峰所需参数的物质,并按上述顺序分别处于冷却开始后1–2秒和10秒之内。我们表明,即使在适中的B0=5×10^14 G下,富质子磁星风也可具有产生p核的有利条件。

英文摘要:

The neutrino-driven wind cooling phase of proto-neutron stars (PNSs) follows successful supernovae. Wind models without magnetic fields or rotation fail to achieve the necessary conditions for production of the third $r-$process peak, but robustly produce a weak $r-$process in neutron-rich winds. Using 2D magnetohydrodynamic simulations with magnetar-strength magnetic fields and rotation, we show that the PNS rotation rate significantly affects the thermodynamic conditions of the wind. We show that high entropy material is quasi-periodically ejected from the closed zone of the PNS magnetosphere with the required thermodynamic conditions to produce heavy elements. We show that maximum entropy $S$ of the material ejected depends systematically on the magnetar spin period $P_{\star}$ and scales as $S \propto P_{\star}^{-5/6}$ for sufficiently rapid rotation. We present results from simulations at a constant neutrino luminosity representative of $\sim 1-2$ s after the onset of cooling for $P_{\star}$ ranging from 5 ms to 200 ms and a few simulations with evolving neutrino luminosity where we follow the evolution of the magnetar wind until $10-14$ s after the onset of cooling. We estimate at magnetar polar magnetic field strength $B_0=3\times 10^{15}$ G and $10^{15}$ G that neutron-rich magnetar winds can respectively produce at least $\sim 1-5\times 10^{-5}$ M$_{\odot}$ and $\sim 1-4\times 10^{-7}$ M$_{\odot}$ of material with the required parameters for synthesis of the third $r-$process peak, within $1-2$ s and 10 s respectively in that order after the onset of cooling. We show that proton-rich magnetar winds can have favorable conditions for production of $p-$nuclei, even at a modest $B_0=5\times 10^{14}$ G.

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