{"title":"同步加速器情景中的伽马射线暴光谱-光度相关性","authors":"Alessio Mei, Gor Oganesyan, Samanta Macera","doi":"arxiv-2409.08341","DOIUrl":null,"url":null,"abstract":"For over two decades, gamma-ray burst (GRB) prompt emission spectra were\nmodelled with smoothly-broken power laws (Band function), and a positive and\ntight correlation between the spectral rest-frame peak energy $E_p$ and the\ntotal isotropic-equivalent luminosity $L_{iso}$ was found, constituting the\nso-called Yonetoku relation. However, more recent studies show that many prompt\nemission spectra are well described by the synchrotron radiation model, hence\nsignificantly deviating from the Band function. In this work, we test the\nimpact of a more suited spectral model such as an idealized synchrotron\nspectrum from non-thermal electrons on the Yonetoku relation and its connection\nwith physical parameters. We select GRBs with measured redshift observed by\nFermi/GBM together with high energy observations (>30 MeV), and perform\nspectral analysis dividing them in two samples: the single-bin sample, using\nthe light curve peak spectrum of each GRB, and the multiple-bins sample, where\nwe explore the whole duration of 13 bright bursts with time-resolved spectral\nanalysis. We observed that the $E_p$ of synchrotron spectra in fast-cooling\nregime ($\\nu_m/\\nu_c\\gg1$) is generally larger than the one provided by the\nBand function. For this reason, we do not find any $E_p-L_{iso}$ correlation in\nour samples except for the GRBs in an intermediate-cooling regime\n($1<\\nu_m/\\nu_c<3$), namely where peak and break energies are very close. We\ninstead find in both our samples a new tight correlation between the rest-frame\ncooling frequency $\\nu_{c,z}$ and $L_{iso}$: $\\nu_{c,z} \\propto L_{iso}^{(0.53\n\\pm 0.06)}$. These results suggest that, assuming that prompt emission spectra\nare produced by synchrotron radiation, the physical relation is between\n$\\nu_{c,z}$ and $L_{iso}$. The fit of the Band function to an intrinsic\nsynchrotron spectrum returns peak energy values $E_{p,z}^{Band} \\sim\n\\nu_{c,z}$.","PeriodicalId":501343,"journal":{"name":"arXiv - PHYS - High Energy Astrophysical Phenomena","volume":"29 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Gamma-ray burst spectral-luminosity correlations in the synchrotron scenario\",\"authors\":\"Alessio Mei, Gor Oganesyan, Samanta Macera\",\"doi\":\"arxiv-2409.08341\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"For over two decades, gamma-ray burst (GRB) prompt emission spectra were\\nmodelled with smoothly-broken power laws (Band function), and a positive and\\ntight correlation between the spectral rest-frame peak energy $E_p$ and the\\ntotal isotropic-equivalent luminosity $L_{iso}$ was found, constituting the\\nso-called Yonetoku relation. However, more recent studies show that many prompt\\nemission spectra are well described by the synchrotron radiation model, hence\\nsignificantly deviating from the Band function. In this work, we test the\\nimpact of a more suited spectral model such as an idealized synchrotron\\nspectrum from non-thermal electrons on the Yonetoku relation and its connection\\nwith physical parameters. We select GRBs with measured redshift observed by\\nFermi/GBM together with high energy observations (>30 MeV), and perform\\nspectral analysis dividing them in two samples: the single-bin sample, using\\nthe light curve peak spectrum of each GRB, and the multiple-bins sample, where\\nwe explore the whole duration of 13 bright bursts with time-resolved spectral\\nanalysis. We observed that the $E_p$ of synchrotron spectra in fast-cooling\\nregime ($\\\\nu_m/\\\\nu_c\\\\gg1$) is generally larger than the one provided by the\\nBand function. For this reason, we do not find any $E_p-L_{iso}$ correlation in\\nour samples except for the GRBs in an intermediate-cooling regime\\n($1<\\\\nu_m/\\\\nu_c<3$), namely where peak and break energies are very close. We\\ninstead find in both our samples a new tight correlation between the rest-frame\\ncooling frequency $\\\\nu_{c,z}$ and $L_{iso}$: $\\\\nu_{c,z} \\\\propto L_{iso}^{(0.53\\n\\\\pm 0.06)}$. These results suggest that, assuming that prompt emission spectra\\nare produced by synchrotron radiation, the physical relation is between\\n$\\\\nu_{c,z}$ and $L_{iso}$. The fit of the Band function to an intrinsic\\nsynchrotron spectrum returns peak energy values $E_{p,z}^{Band} \\\\sim\\n\\\\nu_{c,z}$.\",\"PeriodicalId\":501343,\"journal\":{\"name\":\"arXiv - PHYS - High Energy Astrophysical Phenomena\",\"volume\":\"29 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-09-12\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - PHYS - High Energy Astrophysical Phenomena\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2409.08341\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - High Energy Astrophysical Phenomena","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.08341","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
摘要
二十多年来,伽马射线暴(GRB)的瞬时发射光谱是用平滑断裂幂律(Band函数)来建模的,并且发现光谱静帧峰值能量$E_p$和各向同性等效总光度$L_{iso}$之间存在紧密的正相关关系,这就是所谓的Yonetoku关系。然而,最近的研究表明,许多瞬发光谱都可以用同步辐射模型很好地描述,但却明显偏离了Band函数。在这项工作中,我们测试了一个更合适的光谱模型(如来自非热电子的理想化同步辐射光谱)对Yonetoku关系的影响及其与物理参数的联系。我们选取了费米/GBM观测到的红移和高能量观测到的GRB(>30 MeV),并将它们分为两个样本进行光谱分析:单箱样本,使用每个GRB的光曲线峰值光谱;多箱样本,使用时间分辨光谱分析方法探索13个亮暴的整个持续时间。我们观察到,在快速冷却状态下($\nu_m/\nu_c\gg1$),同步辐射光谱的$E_p$通常比波段函数提供的要大。由于这个原因,我们在样本中没有发现任何$E_p-L_{iso}$相关性,除了处于中等冷却状态($1<\nu_m/\nu_c<3$)的GRB,即峰值能量和断裂能量非常接近的GRB。相反,我们在两个样本中都发现了静帧冷却频率$\nu_{c,z}$和$L_{iso}$之间新的紧密相关性:$\nu_{c,z}.\propto L_{iso}^{(0.53\pm 0.06)}$。这些结果表明,假设瞬发光谱是由同步辐射产生的,那么$\nu_{c,z}$和$L_{iso}$之间存在物理关系。将 Band 函数拟合到本征同步辐射光谱会得到峰值能量值 $E_{p,z}^{Band}\sim/nu_{c,z}$。
Gamma-ray burst spectral-luminosity correlations in the synchrotron scenario
For over two decades, gamma-ray burst (GRB) prompt emission spectra were
modelled with smoothly-broken power laws (Band function), and a positive and
tight correlation between the spectral rest-frame peak energy $E_p$ and the
total isotropic-equivalent luminosity $L_{iso}$ was found, constituting the
so-called Yonetoku relation. However, more recent studies show that many prompt
emission spectra are well described by the synchrotron radiation model, hence
significantly deviating from the Band function. In this work, we test the
impact of a more suited spectral model such as an idealized synchrotron
spectrum from non-thermal electrons on the Yonetoku relation and its connection
with physical parameters. We select GRBs with measured redshift observed by
Fermi/GBM together with high energy observations (>30 MeV), and perform
spectral analysis dividing them in two samples: the single-bin sample, using
the light curve peak spectrum of each GRB, and the multiple-bins sample, where
we explore the whole duration of 13 bright bursts with time-resolved spectral
analysis. We observed that the $E_p$ of synchrotron spectra in fast-cooling
regime ($\nu_m/\nu_c\gg1$) is generally larger than the one provided by the
Band function. For this reason, we do not find any $E_p-L_{iso}$ correlation in
our samples except for the GRBs in an intermediate-cooling regime
($1<\nu_m/\nu_c<3$), namely where peak and break energies are very close. We
instead find in both our samples a new tight correlation between the rest-frame
cooling frequency $\nu_{c,z}$ and $L_{iso}$: $\nu_{c,z} \propto L_{iso}^{(0.53
\pm 0.06)}$. These results suggest that, assuming that prompt emission spectra
are produced by synchrotron radiation, the physical relation is between
$\nu_{c,z}$ and $L_{iso}$. The fit of the Band function to an intrinsic
synchrotron spectrum returns peak energy values $E_{p,z}^{Band} \sim
\nu_{c,z}$.