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首页> 外文期刊>The Astrophysical journal >Effects of Luminosity Functions Induced by Relativistic Beaming on the Statistics of Cosmological Gamma-Ray Bursts
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Effects of Luminosity Functions Induced by Relativistic Beaming on the Statistics of Cosmological Gamma-Ray Bursts

机译:相对论光束诱发的光度函数对宇宙伽马射线爆发统计的影响

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摘要

Most gamma-ray burst (GRB) models have predicted that the intrinsic isotropic energy is limited to below ~1053-1054 ergs. Recently claimed high redshifts, correlation with supernovae, and connections to cosmic star formation activity point to a different energy requirement and source evolution history, possibly with strong beaming. We study the effects of the beaming-induced luminosity function on statistics of observed GRBs, assuming the cosmological scenario. We select and divide the BATSE 4B data into 588 long bursts (T90 2.5 s) and 149 short bursts (T90 2.5 s), and compare the statistics calculated in each subgroup. The V/Vmax of the long bursts is 0.2901 ± 0.0113, and that of the short bursts is 0.4178 ± 0.0239. For luminosity function models, we consider a cylindrical beam and a conic beam. We take into account the spatial distribution of GRB sources as well. A broad luminosity function is naturally produced when one introduces beaming of GRBs. We calculate the maximum detectable redshift of GRBs, zmax. The estimated zmax for the cylindrical beam case is as high as ~14 (α = 1.0) and ~6 (α = 2.0) for the long bursts, and ~3 (α = 1.0) and ~1.6 (α = 2.0) for the short bursts, where α is the photon index. The large zmax value for the short bursts is rather surprising, in that the V/Vmax for this subgroup is close to the so-called Euclidean value, 0.5. We calculate the fraction of bursts whose redshifts are larger than a certain redshift z', i.e., f z'. When we take z' = 3.42 and apply the luminosity function derived for the cylindrical beam, the expected f z' is ~75% (α = 1.0) and ~50% (α = 2.0) for long bursts. When we increase the opening angle of the conic beam to Δθ = 30, f z' decreases to ~20% (α = 1.0) at z' = 3.42. If we assume α = 2.0, the conic beam with Δθ = 30 cannot explain the redshift distribution of the observed GRBs. We conclude that the beaming-induced luminosity functions are compatible with the redshift distribution of the observed GRBs, although the apparent "Euclidean" value of V/Vmax might be explained by the standard model.
机译:大多数伽马射线爆发(GRB)模型已预测,本征各向同性能量仅限于〜1053-1054 ergs以下。最近声称的高红移,与超新星的相关性以及与宇宙恒星形成活动的联系都指向不同的能量需求和源演化历史,可能是强烈的辐射作用。我们假设宇宙学情景,研究了光束诱导的光度函数对观测到的GRB统计的影响。我们选择BATSE 4B数据并将其分为588个长脉冲(T90> 2.5 s)和149个短脉冲(T90 <2.5 s),并比较每个子组中计算出的统计数据。长脉冲的V / Vmax为0.2901±0.0113,短脉冲的V / Vmax为0.4178±0.0239。对于光度函数模型,我们考虑圆柱光束和圆锥光束。我们还考虑了GRB源的空间分布。当引入GRB光束时,自然会产生广泛的发光度功能。我们计算GRB的最大可检测红移zmax。圆柱束情况下的估计zmax对于长脉冲串高达〜14(α= 1.0)和〜6(α= 2.0),而对于突波来说约为3(α= 1.0)和〜1.6(α= 2.0)。短脉冲,其中α是光子指数。短脉冲的大zmax值令人惊讶,因为该子组的V / Vmax接近所谓的欧几里得值0.5。我们计算其红移大于某个红移z'(即f> z')的突发分数。当我们取z'= 3.42并应用为圆柱光束得出的光度函数时,对于长脉冲,期望的f> z'为〜75%(α= 1.0)和〜50%(α= 2.0)。当我们将圆锥形光束的打开角度增加到Δθ= 30时,在z'= 3.42时,f> z'减小至〜20%(α= 1.0)。如果我们假设α= 2.0,则Δθ= 30的圆锥形光束无法解释观测到的GRB的红移分布。我们得出结论,尽管标准模型可能解释了V / Vmax的表观“欧几里得”值,但光束诱导的光度函数与观测到的GRB的红移分布兼容。

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