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arXiv 2403.08765astro-ph.HE
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千新星抛射物中电子热化过程的解析描述

An Analytic Description of Electron Thermalization in Kilonovae Ejecta

Ben Shenhar, Or Guttman, Eli Waxman

AI总结:

该研究针对中子星并合千新星抛射物中的β衰变电子热化过程,推导了适用于宽参数范围的能量沉积率解析公式,可简化千新星光变曲线计算并用于约束抛射物密度参数。

摘要:

本文针对中子星并合事件中抛射出的、作同源膨胀的放射性等离子体,给出了β衰变电子能量沉积率的一种简洁解析描述,该描述适用于范围广泛的抛射物参数——初始熵、电子丰度{s₀,Yₑ}以及密度ρt³。这些公式是通过追踪随时间演化的成分和β衰变发射谱(包含延迟沉积效应)的详细数值计算推导得出的。沉积效率主要取决于ρt³,而对{s₀,Yₑ}的依赖很弱。电子能量沉积率与能量产生率的比值降至1-e⁻¹的时刻tₑ满足公式tₑ=t₀ₑ(ρt³/(0.5(ρt³)₀))ᵃ,其中(ρt³)₀=0.05M⊙/(4π(0.2c)³),t₀ₑ(s₀,Yₑ)≈17天,且0.4≤a(s₀,Yₑ)≤0.5。由核物理不确定性导致的tₑ的分数不确定度约为10%。a≤0.5的结果反映了如下事实:特征β衰变电子能量不会随时间降低(这很大程度上源于“倒置衰变链”,即慢衰变同位素衰变为具有更高端点能量的快衰变同位素)。我们给出了随时间变化的电子能量沉积率的解析近似,在沉积率随时间下降3-4个数量级的范围内,该近似与数值结果的吻合度优于50%(通常<30%,远小于核物理不确定性带来的能量产生率的不确定度)。我们的结果可方便地纳入千新星光变曲线(具有一般密度和成分结构)的计算中,无需再通过数值追踪随时间演化的电子能谱。例如,通过在热光变曲线中识别tₑ,将能够约束(经适当平均的)抛射物的ρt³。

英文摘要:

A simple analytic description is provided of the rate of energy deposition by $β$-decay electrons in the homologously expanding radioactive plasma ejected in neutron star mergers, valid for a wide range of ejecta parameters -- initial entropy, electron fraction $\{s_0,Y_e\}$ and density $ρt^3$. The formulae are derived using detailed numerical calculations following the time-dependent composition and $β$-decay emission spectra (including the effect of delayed deposition). The deposition efficiency depends mainly on $ρt^3$ and only weakly on $\{s_0,Y_e\}$. The time $t_e$ at which the ratio between the rates of electron energy deposition and energy production drops to $1-e^{-1}$, is given by $t_e=t_{0e}\Big(\frac{ρt^3}{0.5(ρt^3)_0}\Big)^a$, where $(ρt^3)_0=\frac{0.05M_{\odot}}{4π(0.2c)^3}$, $t_{0e}(s_0,Y_e)\approx17$ days and $0.4\le a(s_0,Y_e)\le0.5$. The fractional uncertainty in $t_e$ due to nuclear physics uncertainties is $\approx10\%$. The result $a\le0.5$ reflects the fact that the characteristic $β$-decay electron energies do not decrease with time (largely due to "inverted decay chains" in which a slowly-decaying isotope decays to a rapidly-decaying isotope with higher end-point energy). We provide an analytic approximation for the time-dependent electron energy deposition rate, reproducing the numerical results to better than $50\%$ (typically $<30\%$, well within the energy production rate uncertainty due to nuclear physics uncertainties) over a 3-4 orders-of-magnitude deposition rate decrease with time. Our results may be easily incorporated in calculations of kilonovae light curves (with general density and composition structures), eliminating the need to numerically follow the time-dependent electron spectra. Identifying $t_e$, e.g. in the bolometric light curve, will constrain the (properly averaged) ejecta $ρt^3$.

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