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arXiv 2501.07080astro-ph.HE
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旋转黑洞周围含激波的中微子主导相对论粘性吸积流

Neutrino-dominated relativistic viscous accretion flows around rotating black holes with shocks

Amit Kumar, Sayan Chakrabarti, Santabrata Das

AI总结:

本文构建含中微子冷却的旋转黑洞NDAF全局跨声速模型,分析驻激波条件及中微子与湮灭光度,并用5个已知红移GRB约束中心黑洞自旋和吸积率。

摘要:

我们研究了旋转恒星级黑洞周围的相对论、粘性、平流、中微子主导吸积流(NDAFs),并纳入中微子冷却。通过采用有效势描述旋转黑洞周围的时空几何,我们自洽地求解控制NDAF的方程,以获得全局跨声速吸积解。研究结果表明,取决于模型参数,即能量(ε)、角动量(λ)、吸积率($\dot{m}$)、粘度(α)和黑洞自旋($a_{\rm k}$),NDAFs可能存在满足Rankine-Hugoniot激波条件(RHCs)的驻激波。利用这些由激波诱导的NDAF解,我们在广泛的模型参数范围内计算了中微子光度($L_ν$)和中微子湮灭光度($L_{ν\barν}$)。我们进一步计算了最大中微子光度($L_ν^{\rm max}$)和最大中微子湮灭光度($L_{ν\barν}^{\rm max}$),对于$a_{\rm k}=0.99$(0.0),得到$L_ν^{\rm max}\sim10^{51-53}$ erg s$^{-1}$($10^{48-51}$ erg s$^{-1}$)以及$L_{ν\barν}^{\rm max}\sim10^{48-52}$ erg s$^{-1}$($10^{42-49}$ erg s$^{-1}$)。这些发现表明,含激波的NDAF解在解释伽马射线暴(GRBs)的能量输出方面可能具有前景。我们采用NDAF模型形式来阐明5个具有已知红移的GRBs的观测中微子湮灭光度$L^{\rm obs}_{ν\barν}$,并根据所考虑GRBs中心源的自旋($a_{\rm k}$)估计其吸积率($\dot{m}$)。

英文摘要:

We investigate the relativistic, viscous, advective, neutrino-dominated accretion flows (NDAFs) around rotating stellar mass black holes, incorporating neutrino cooling. By adopting an effective potential to describe the spacetime geometry around the rotating black holes, we self-consistently solve the governing NDAF equations to obtain global transonic accretion solutions. Our findings indicate that, depending on the model parameters, namely energy ($\varepsilon$), angular momentum ($λ$), accretion rate ($\dot{m}$), viscosity ($α$) and black hole spin ($a_{\rm k}$), NDAFs may harbor standing shocks where the Rankine-Hugoniot shock conditions (RHCs) are satisfied. Utilizing these shock-induced NDAF solutions, we compute the neutrino luminosity ($L_ν$) and neutrino annihilation luminosity ($L_{ν\barν}$) across a wide range of model parameters. We further calculate maximum neutrino luminosity ($L_ν^{\rm max}$) and neutrino annihilation luminosity ($L_{ν\barν}^{\rm max}$) resulting in $L_ν^{\rm max} \sim 10^{51-53}$ erg s$^{-1}$ ($10^{48-51}$ erg s$^{-1}$) and $L_{ν\barν}^{\rm max} \sim 10^{48-52}$ erg s$^{-1}$ ($10^{42-49}$ erg s$^{-1}$) for $a_{\rm k}=0.99$ (0.0). These findings suggest that shocked NDAF solutions are potentially promising to explain the energy output of gamma-ray bursts (GRBs). We employ our NDAF model formalism to elucidate $L^{\rm obs}_{ν\barν}$ for five GRBs with known redshifts and estimate their accretion rate (${\dot m}$) based on the spin ($a_{\rm k}$) of the central source of GRBs under consideration.

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