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Joule-Thomson expansion, motion of particles and QPOs around Bardeen-AdS black hole immersed in a fluid of strings 焦耳-汤姆森膨胀、浸没在弦流体中的巴丁-AdS 黑洞周围的粒子运动和 QPOs
IF 10.2 4区 物理与天体物理 Q1 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-11-01 DOI: 10.1016/j.jheap.2024.10.017
G. Mustafa , Faisal Javed , S.K. Maurya , Shalan Alkarni , Orhan Donmez , Arzu Cilli , Ertan Güdekli
In this work, we investigate the dynamics of particles around a Bardeen AdS black hole immersed in a fluid of strings, focusing on how the black hole parameters affect particle motion. We observe the black hole's Joule-Thomson expansion and the impact of physical parameters on the cooling and heating zones. Using Joule-Thomson coefficients, we also discuss the stable and unstable configuration of the considered black hole for both cases. The stability of circular equatorial orbits is analyzed using the effective potential approach. We derive analytical expressions for the energy and angular momentum of these circular orbits as functions of the black hole parameters. We also explore the impact of these parameters on the innermost stable circular orbits and discuss the effective forces acting on the particles. In addition, we examine the epicyclic oscillations of particles near a stable equatorial orbits and calculate the corresponding oscillation frequencies as function of black hole parameters. The periastron frequency is also analyzed. Furthermore, we study particle collisions and the resulting center of mass-energy in the vicinity of the black hole. We show that the parameters of the model significantly influence particle motion. Lastly, we compare the particle dynamics around the Bardeen AdS black hole immersed in a fluid of strings with those around the Bardeen black hole and the Bardeen Reissner-Nordström black hole.
在这项工作中,我们研究了沉浸在弦流体中的巴丁 AdS 黑洞周围粒子的动力学,重点是黑洞参数如何影响粒子运动。我们观察了黑洞的焦耳-汤姆森膨胀以及物理参数对冷却区和加热区的影响。利用焦耳-汤姆逊系数,我们还讨论了所考虑的黑洞在两种情况下的稳定和不稳定构型。我们使用有效势方法分析了圆形赤道轨道的稳定性。我们推导出了这些圆形轨道的能量和角动量的分析表达式,它们是黑洞参数的函数。我们还探讨了这些参数对最内层稳定圆形轨道的影响,并讨论了作用在粒子上的有效力。此外,我们还研究了稳定赤道轨道附近粒子的后圆振荡,并计算出相应的振荡频率与黑洞参数的函数关系。我们还分析了近天体频率。此外,我们还研究了黑洞附近的粒子碰撞和由此产生的质能中心。结果表明,模型参数对粒子运动有显著影响。最后,我们将浸泡在弦流体中的巴丁 AdS 黑洞周围的粒子动力学与巴丁黑洞和巴丁 Reissner-Nordström 黑洞周围的粒子动力学进行了比较。
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引用次数: 0
Spin and spectral properties of Cygnus X-1 observed with Insight-HXMT 用 Insight-HXMT 观测到的天鹅座 X-1 的自旋和光谱特性
IF 10.2 4区 物理与天体物理 Q1 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-11-01 DOI: 10.1016/j.jheap.2024.10.013
Yihao Zhu, Hanji Wu, Wei Wang
<div><div>Cygnus X-1 is a Galactic black hole X-ray binary with persistent X-ray emissions. We examine the spectral data from 2 – 22 keV gathered by Insight-HXMT observations conducted from 2020 to 2022. We use the continuum-fitting method to constrain three parameters of Cygnus X-1: the black hole spin <span><math><msup><mrow><mi>a</mi></mrow><mrow><mo>⁎</mo></mrow></msup></math></span>, the hydrogen column density <span><math><msub><mrow><mi>N</mi></mrow><mrow><mi>H</mi></mrow></msub></math></span>, and the photon index of the powerlaw component Γ. The fittings constrain <span><math><msub><mrow><mi>N</mi></mrow><mrow><mi>H</mi></mrow></msub><mo>=</mo><mo>(</mo><mn>1.1</mn><mo>±</mo><mn>0.1</mn><mo>)</mo><mo>×</mo><msup><mrow><mn>10</mn></mrow><mrow><mn>22</mn></mrow></msup></math></span> atom cm<sup>−2</sup>, and Γ evolving from ∼2.4 in 2020 to ∼1.9 in 2022. We find the dimensionless spin parameter <span><math><msup><mrow><mi>a</mi></mrow><mrow><mo>⁎</mo></mrow></msup><mo>></mo><mn>0.977</mn></math></span> <span><math><mo>(</mo><mn>3</mn><mi>σ</mi><mo>)</mo></math></span> assuming the distance of the source <span><math><mi>D</mi><mo>=</mo><mn>2.22</mn></math></span> kpc, the mass of the black hole <span><math><msub><mrow><mi>M</mi></mrow><mrow><mi>BH</mi></mrow></msub><mo>=</mo><mn>21.4</mn><msub><mrow><mi>M</mi></mrow><mrow><mo>⊙</mo></mrow></msub></math></span>, and the inclination of the system <span><math><mi>i</mi><mo>=</mo><msup><mrow><mn>27.47</mn></mrow><mrow><mo>∘</mo></mrow></msup></math></span>. Furthermore, considering the uncertainty of <em>D</em> from 1.22 kpc to 3.22 kpc, <span><math><mn>16</mn><msub><mrow><mi>M</mi></mrow><mrow><mo>⊙</mo></mrow></msub><mo><</mo><msub><mrow><mi>M</mi></mrow><mrow><mi>BH</mi></mrow></msub><mo><</mo><mn>25</mn><msub><mrow><mi>M</mi></mrow><mrow><mo>⊙</mo></mrow></msub></math></span>, <span><math><msup><mrow><mn>22</mn></mrow><mrow><mo>∘</mo></mrow></msup><mo><</mo><mi>i</mi><mo><</mo><msup><mrow><mn>31</mn></mrow><mrow><mo>∘</mo></mrow></msup></math></span>, the Monte Carlo analysis is performed and still confirms a large spin of the limitation <span><math><msup><mrow><mi>a</mi></mrow><mrow><mo>⁎</mo></mrow></msup><mo>></mo><mn>0.999</mn><mo>(</mo><mn>1</mn><mi>σ</mi><mo>)</mo></math></span> without the <em>D</em>, <em>i</em>, and <span><math><msub><mrow><mi>M</mi></mrow><mrow><mi>BH</mi></mrow></msub></math></span> bias for Cygnus X-1. We also try to use the limits of <span><math><msup><mrow><mi>a</mi></mrow><mrow><mo>⁎</mo></mrow></msup></math></span> to reversely constrain the range of <em>D</em>, <em>i</em>, and <span><math><msub><mrow><mi>M</mi></mrow><mrow><mi>BH</mi></mrow></msub></math></span>, and find that for the extreme situation (<span><math><msup><mrow><mi>a</mi></mrow><mrow><mo>⁎</mo></mrow></msup><mo>></mo><mn>0.99</mn></math></span>), the derived distributions prefer a low <em>i</em>, large <span><math><msub><mrow><mi>M</mi></mrow><mrow><mi>BH</mi></mrow></msub
天鹅座 X-1 是一个银河系黑洞 X 射线双星,具有持续的 X 射线辐射。我们研究了从 2020 年到 2022 年进行的 Insight-HXMT 观测收集到的 2 - 22 keV 光谱数据。我们使用连续拟合方法来约束天鹅座 X-1 的三个参数:黑洞自旋 a⁎、氢柱密度 NH 和幂律分量 Γ 的光子指数。根据拟合结果,NH=(1.1±0.1)×1022原子厘米-2,Γ从2020年的∼2.4演化到2022年的∼1.9。假设星源距离D=2.22 kpc,黑洞质量MBH=21.4M⊙,系统倾角i=27.47∘,我们发现无量纲自旋参数a⁎>0.977(3σ)。此外,考虑到 D 的不确定性从 1.22 kpc 到 3.22 kpc,16M⊙<MBH<25M⊙,22∘<i<31∘,我们进行了蒙特卡洛分析,在没有 D、i 和 MBH 偏差的情况下,仍然证实了天鹅座 X-1 的极限 a⁎>0.999(1σ)。我们还尝试使用 a⁎的限制来反向约束 D、i 和 MBH 的范围,结果发现在极端情况下(a⁎>0.99),得出的分布更倾向于低 i、大 MBH 和 2 - 3 kpc 左右的距离。此外,还讨论了改变硬化因子对测量 a⁎ 的影响。
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The fittings constrain &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;N&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;H&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mn&gt;1.1&lt;/mn&gt;&lt;mo&gt;±&lt;/mo&gt;&lt;mn&gt;0.1&lt;/mn&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;22&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;&lt;/span&gt; atom cm&lt;sup&gt;−2&lt;/sup&gt;, and Γ evolving from ∼2.4 in 2020 to ∼1.9 in 2022. We find the dimensionless spin parameter &lt;span&gt;&lt;math&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;a&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;⁎&lt;/mo&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;mn&gt;0.977&lt;/mn&gt;&lt;/math&gt;&lt;/span&gt; &lt;span&gt;&lt;math&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;mi&gt;σ&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; assuming the distance of the source &lt;span&gt;&lt;math&gt;&lt;mi&gt;D&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;2.22&lt;/mn&gt;&lt;/math&gt;&lt;/span&gt; kpc, the mass of the black hole &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;M&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;BH&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;21.4&lt;/mn&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;M&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;⊙&lt;/mo&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;, and the inclination of the system &lt;span&gt;&lt;math&gt;&lt;mi&gt;i&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mn&gt;27.47&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;∘&lt;/mo&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;&lt;/span&gt;. Furthermore, considering the uncertainty of &lt;em&gt;D&lt;/em&gt; from 1.22 kpc to 3.22 kpc, &lt;span&gt;&lt;math&gt;&lt;mn&gt;16&lt;/mn&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;M&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;⊙&lt;/mo&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;&lt;&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;M&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;BH&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;&lt;&lt;/mo&gt;&lt;mn&gt;25&lt;/mn&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;M&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;⊙&lt;/mo&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;, &lt;span&gt;&lt;math&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mn&gt;22&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;∘&lt;/mo&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;&lt;&lt;/mo&gt;&lt;mi&gt;i&lt;/mi&gt;&lt;mo&gt;&lt;&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mn&gt;31&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;∘&lt;/mo&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;&lt;/span&gt;, the Monte Carlo analysis is performed and still confirms a large spin of the limitation &lt;span&gt;&lt;math&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;a&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;⁎&lt;/mo&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;mn&gt;0.999&lt;/mn&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mi&gt;σ&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; without the &lt;em&gt;D&lt;/em&gt;, &lt;em&gt;i&lt;/em&gt;, and &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;M&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;BH&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; bias for Cygnus X-1. We also try to use the limits of &lt;span&gt;&lt;math&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;a&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;⁎&lt;/mo&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;&lt;/span&gt; to reversely constrain the range of &lt;em&gt;D&lt;/em&gt;, &lt;em&gt;i&lt;/em&gt;, and &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;M&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;BH&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;, and find that for the extreme situation (&lt;span&gt;&lt;math&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;a&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;⁎&lt;/mo&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;mn&gt;0.99&lt;/mn&gt;&lt;/math&gt;&lt;/span&gt;), the derived distributions prefer a low &lt;em&gt;i&lt;/em&gt;, large &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;M&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;BH&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub","PeriodicalId":54265,"journal":{"name":"Journal of High Energy Astrophysics","volume":"44 ","pages":"Pages 381-392"},"PeriodicalIF":10.2,"publicationDate":"2024-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142561353","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Neutrino emission due to pair – annihilation in the neutron star magnetic field 中子星磁场中的成对湮灭导致的中微子发射
IF 10.2 4区 物理与天体物理 Q1 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-11-01 DOI: 10.1016/j.jheap.2024.11.005
Shiladittya Debnath , Brajagopal Majumder
In this paper, we have calculated the energy loss in terms of luminosity for neutrinos produced by the annihilation of electron–positron pair in the light of Photo – Neutrino weak interaction with an intense magnetic field. After analytical calculation, we may conclude that the neutrino luminosity increases with the magnetic field in the temperature range of 108 to 1012 Kelvins giving rise to an energy loss channel. This may provide an alternate cooling mechanism for highly magnetized neutron stars. We have also conducted a comparative study of neutrino emission from magnetized neutron stars based on both Photo–Neutrino interaction and Conventional (current – current) weak interaction. We found a remarkable similarity between the two models on temperature versus energy loss behaviour of neutron stars. However, these are found to differ from one another on the overall time scale of evolution.
在本文中,我们以光度的形式计算了在强磁场下电子-正电子对湮灭产生的中微子的能量损失。经过分析计算,我们可以得出这样的结论:在 108 至 1012 开尔文的温度范围内,中微子的光度会随着磁场的增加而增加,从而产生一个能量损失通道。这可能为高磁化中子星提供了另一种冷却机制。我们还根据光-中微子相互作用和常规(电流-电流)弱相互作用对磁化中子星的中微子发射进行了比较研究。我们发现这两种模型在中子星的温度与能量损失行为上有明显的相似性。然而,我们发现这两种模型在演化的总体时间尺度上有所不同。
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引用次数: 0
Constraining the equation of state parametrization in Hořava-Lifshitz gravity 限制霍扎瓦-利夫希茨引力中的状态方程参数化
IF 10.2 4区 物理与天体物理 Q1 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-11-01 DOI: 10.1016/j.jheap.2024.11.003
Himanshu Chaudhary , Ujjal Debnath , S.K. Maurya , G. Mustafa , Farruh Atamurotov
In this paper, we investigate the late-time cosmic accelerated expansion using various equations of state parametrizations within the framework of Hořava-Lifshitz gravity. We utilize Markov Chain Monte Carlo (MCMC) analysis to constrain the parameters of each proposed model, employing observational Hubble data and Type Ia supernovae. Additionally, we analyze and plot the deceleration parameters for each model. Our findings suggest that the Universe has recently transitioned from a phase of deceleration to acceleration in all the models considered. We also analyzed the behavior of the energy conditions for each proposed model within the framework of Hořava-Lifshitz gravity, specifically at the present epoch (z=0). To further assess the effectiveness of these models, we apply both the Akaike Information Criterion (AIC) and the Bayesian Information Criterion (BIC) to compare their performance against the standard ΛCDM model. Our results provide valuable insights into how different models perform relative to ΛCDM, offering a comprehensive evaluation of their viability in describing the Universe's accelerated expansion.
在本文中,我们利用霍热瓦-利夫希茨引力框架内的各种状态方程参数对晚期宇宙加速膨胀进行了研究。我们利用马尔可夫链蒙特卡罗(MCMC)分析法,利用哈勃观测数据和 Ia 型超新星来约束每个拟议模型的参数。此外,我们还分析并绘制了每个模型的减速参数。我们的研究结果表明,在所有考虑的模型中,宇宙最近都从减速阶段过渡到了加速阶段。我们还分析了在霍扎瓦-利夫希茨引力框架下,每个模型的能量条件行为,特别是在当前纪元(z=0)。为了进一步评估这些模型的有效性,我们应用阿凯克信息准则(AIC)和贝叶斯信息准则(BIC)将它们的性能与标准ΛCDM模型进行了比较。我们的结果为我们了解不同模型相对于ΛCDM的表现提供了宝贵的见解,为我们全面评估这些模型在描述宇宙加速膨胀方面的可行性提供了依据。
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引用次数: 0
Exploring the supernova remnant contribution to the first LHAASO source catalog via passively illuminated interstellar clouds 通过被动照亮的星际云探索超新星残余对首个 LHAASO 源目录的贡献
IF 10.2 4区 物理与天体物理 Q1 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-10-18 DOI: 10.1016/j.jheap.2024.10.011
Alison M.W. Mitchell , Silvia Celli
Supernova remnants (SNRs) are considered as the most promising source class to account for the bulk of the Galactic cosmic-ray flux. Yet amongst the population of ultra-high energy (UHE) sources that has recently emerged, due to high-altitude particle detector experiments such as LHAASO and HAWC, remarkably few are associated with known SNRs. These observations might well indicate that the highest energy particles would escape the remnant early during the shock evolution as a result of its reduced confinement capabilities. This flux of escaping particles may then encounter dense targets (gas and dust) for hadronic interactions in the form of both atomic and molecular material such as interstellar clouds, thereby generating a UHE gamma-ray flux. We explore such a scenario here, considering known SNRs in a physically driven model for particle escape, and as coupled to molecular clouds in the Galaxy. Our analysis allows the investigation of SNR-illuminated clouds in coincidence with sources detected in the first LHAASO catalogue. Indeed, the illuminated interstellar clouds may contribute to the total gamma-ray flux from several unidentified sources, as we discuss here. Yet we nevertheless find that further detailed studies will be necessary to verify or refute this scenario of passive UHE gamma-ray sources in future.
超新星残余(SNR)被认为是最有希望产生银河宇宙射线通量的源类。然而,在最近由于高空粒子探测器实验(如 LHAASO 和 HAWC)而出现的超高能量(UHE)源中,与已知 SNR 有关的超高能量源却少得可怜。这些观测结果很可能表明,在冲击演化过程中,由于残余物的束缚能力降低,能量最高的粒子会在早期逃离残余物。这些逃逸的粒子流可能会遇到高密度目标(气体和尘埃),以原子和分子物质(如星际云)的形式发生强子相互作用,从而产生超高辐射伽马射线通量。我们在这里探讨了这种情况,考虑了粒子逃逸物理驱动模型中的已知SNR,以及与银河系中分子云的耦合。通过我们的分析,可以研究SNR照亮的云与第一批LHAASO目录中探测到的源的重合情况。事实上,被照亮的星际云可能对来自几个未识别源的伽马射线总通量做出了贡献,我们在这里对此进行了讨论。尽管如此,我们发现今后还需要进一步的详细研究来验证或反驳这种被动超高辐射伽马射线源的情况。
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引用次数: 0
Towards a new model-independent calibration of Gamma-Ray Bursts 迈向与模型无关的伽马射线暴新校准方法
IF 10.2 4区 物理与天体物理 Q1 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-10-17 DOI: 10.1016/j.jheap.2024.10.010
Arianna Favale , Maria Giovanna Dainotti , Adrià Gómez-Valent , Marina Migliaccio
<div><div>Current data on baryon acoustic oscillations and Supernovae of Type Ia (SNIa) cover up to <span><math><mi>z</mi><mo>∼</mo><mn>2.5</mn></math></span>. These low-redshift observations play a very important role in the determination of cosmological parameters and have been widely used to constrain the ΛCDM and models beyond the standard, such as the ones with open curvature. To extend this investigation to higher redshifts, Gamma-Ray Bursts (GRBs) stand out as one of the most promising observables. In spite of being transient, they are extremely energetic and can be used to probe the universe up to <span><math><mi>z</mi><mo>∼</mo><mn>9.4</mn></math></span>. They exhibit characteristics that suggest they are potentially standardizable candles and this allows their use to extend the distance ladder beyond SNIa. The use of GRB correlations is still a challenge due to the spread in their intrinsic properties. One of the correlations that can be employed for the standardization is the fundamental plane relation between the peak prompt luminosity, the rest-frame end time of the plateau phase, and its corresponding luminosity, also known as the <em>three-dimensional Dainotti correlation</em>. In this work, we propose an innovative method of calibration of the Dainotti relation which is independent of cosmology. We employ state-of-the-art data on Cosmic Chronometers (CCH) at <span><math><mi>z</mi><mo>≲</mo><mn>2</mn></math></span> and use the Gaussian Processes Bayesian reconstruction tool. To match the CCH redshift range, we select 20 long GRBs in the range <span><math><mn>0.553</mn><mo>≤</mo><mi>z</mi><mo>≤</mo><mn>1.96</mn></math></span> from the <em>Platinum sample</em>, which consists of well-defined GRB plateau properties that obey the fundamental plane relation. To ensure the generality of our method, we verify that the choice of priors on the parameters of the Dainotti relation and the modeling of CCH uncertainties and covariance have negligible impact on our results. Moreover, we consider the case in which the redshift evolution of the physical features of the plane is accounted for. We find that the use of CCH allows us to identify a sub-sample of GRBs that adhere even more closely to the fundamental plane relation, with an intrinsic scatter of <span><math><msub><mrow><mi>σ</mi></mrow><mrow><mi>i</mi><mi>n</mi><mi>t</mi></mrow></msub><mo>=</mo><msubsup><mrow><mn>0.20</mn></mrow><mrow><mo>−</mo><mn>0.05</mn></mrow><mrow><mo>+</mo><mn>0.03</mn></mrow></msubsup></math></span> obtained in this analysis when evolutionary effects are considered. In an epoch in which we strive to reduce uncertainties on the variables of the GRB correlations in order to tighten constraints on cosmological parameters, we have found a novel model-independent approach to pinpoint a sub-sample that can thus represent a valuable set of standardizable candles. This allows us to extend the cosmic distance ladder presenting a new catalog of calibrated luminosity distanc
目前关于重子声振荡和 Ia 型超新星(SNIa)的数据覆盖到 z∼2.5。这些低红移观测数据在确定宇宙学参数方面起着非常重要的作用,并被广泛用于约束ΛCDM和标准模型之外的模型,如具有开放曲率的模型。为了将这一研究扩展到更高的红移,伽马射线暴(GRBs)成为最有前途的观测指标之一。尽管它们是瞬时的,但能量极高,可以用来探测高达 z∼9.4 的宇宙。它们所表现出的特征表明,它们是潜在的可标准化烛光,这使得它们的使用可以将距离阶梯扩展到 SNIa 以外。由于GRB内在特性的差异,使用GRB相关性仍然是一个挑战。其中一种可以用于标准化的相关性是峰值瞬发光度、高原阶段的静帧结束时间及其相应光度之间的基本平面关系,也称为三维 Dainotti 相关性。在这项工作中,我们提出了一种独立于宇宙学的创新方法来校准 Dainotti 关系。我们采用了 z≲2时宇宙计时器(CCH)的最新数据,并使用了高斯过程贝叶斯重建工具。为了与CCH的红移范围相匹配,我们从白金样本中选择了20个0.553≤z≤1.96范围内的长GRB,该样本由符合基本平面关系的定义明确的GRB高原特性组成。为了确保我们方法的通用性,我们验证了 Dainotti 关系参数先验的选择以及 CCH 不确定性和协方差的建模对我们结果的影响可以忽略不计。此外,我们还考虑了平面物理特征的红移演变情况。我们发现,使用 CCH 可以让我们识别出更接近基本平面关系的 GRB 子样本,在考虑演化效应的情况下,本分析得到的固有散度为σint=0.20-0.05+0.03。在我们努力减少GRB相关变量的不确定性以加强对宇宙学参数约束的时代,我们发现了一种新颖的与模型无关的方法,可以精确定位一个子样本,从而代表一组有价值的可标准化烛光。这使我们能够扩展宇宙距离阶梯,提出一个新的校准发光距离目录,直到z=5。
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引用次数: 0
A multiwavelength study of the most distant gamma-ray detected BL Lacertae object 4FGL J1219.0+3653 (z = 3.59) 对探测到的最遥远伽马射线BL Lacertae天体4FGL J1219.0+3653(z = 3.59)的多波长研究
IF 10.2 4区 物理与天体物理 Q1 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-10-16 DOI: 10.1016/j.jheap.2024.10.008
Srijita Hazra , Vaidehi S. Paliya , A. Domínguez , C. Cabello , N. Cardiel , J. Gallego
BL Lac objects are a class of jetted active galactic nuclei that do not exhibit or have weak emission lines in their optical spectra. Recently, the first γ-ray emitting BL Lac beyond z=3, 4FGL J1219.0 +3653 (hereafter J1219), was identified, i.e., within the first two billion years of the age of the universe. Here we report the results obtained from a detailed broadband study of this peculiar source by analyzing the new ∼58 ksec XMM-Newton and archival observations and reproducing the multiwavelength spectral energy distribution with the conventional one-zone leptonic radiative model. The XMM-Newton data revealed that J1219 is a faint X-ray emitter (F0.310 keV=1.020.24+0.47×1015 ergcm2s1) and exhibits a soft spectrum (0.3−10 keV photon index=2.280.46+0.58). By comparing the broadband physical properties of J1219 with z>3 γ-ray detected flat spectrum radio quasars (FSRQs), we have found that it has a relatively low jet power and, similar to FSRQs, the jet power is larger than the accretion disk luminosity. We conclude that deeper multiwavelength observations will be needed to fully explore the physical properties of this unique high-redshift BL Lac object.
BL Lac天体是一类在光学光谱中不显示或有微弱发射线的喷流活动星系核。最近,我们发现了第一个z=3以上的发射γ射线的BL Lac,即4FGL J1219.0 +3653(以下简称J1219),也就是宇宙年龄的前20亿年。在此,我们报告了通过分析新的∼58 ksec XMM-Newton和档案观测数据,并用传统的单区轻子辐射模型重现多波长光谱能量分布,对这一奇特来源进行详细宽带研究的结果。XMM-Newton数据显示,J1219是一个微弱的X射线发射器(F0.3-10 keV=1.02-0.24+0.47×10-15 ergcm-2s-1),并表现出柔和的光谱(0.3-10 keV光子指数=2.28-0.46+0.58)。通过比较 J1219 与 z>3 γ 射线探测到的平谱射电类星(FSRQs)的宽带物理特性,我们发现它的喷流功率相对较低,而且与 FSRQs 相似,喷流功率大于吸积盘光度。我们的结论是,要全面探索这个独特的高红移 BL Lac 天体的物理特性,还需要更深入的多波长观测。
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引用次数: 0
Matter bounce cosmology within Finsler-Randers geometry: A comprehensive study of anisotropic influences 芬斯勒-兰德斯几何中的物质反弹宇宙学:各向异性影响的综合研究
IF 10.2 4区 物理与天体物理 Q1 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-10-16 DOI: 10.1016/j.jheap.2024.10.009
J. Praveen, S.K. Narasimhamurthy
In this study, we explore the dynamics of matter bounce cosmology within the framework of Finsler-Randers geometry, focusing on the role of the Finslerian correction term η(t). By integrating Finsler geometry into cosmological models, we introduce anisotropic effects that significantly impact the evolution of the universe, particularly during the bounce phase. The research examines various cosmological parameters, including the deceleration (qη(t)), jerk (jη(t)), and snap (sη(t)) parameters, highlighting the influence of the Finsler correction on these key indicators. Our results demonstrate that the Finslerian framework leads to more complex and abrupt transitions in the universe's expansion dynamics compared to traditional Riemannian models. The study also reveals that the Finslerian correction intensifies the violations of energy conditions, such as the null energy condition (NEC), which are crucial for the occurrence of a successful bounce. Furthermore, the analysis of the squared sound speed vs2 indicates that the model's stability is highly sensitive to the choice of the Finslerian parameters, with certain configurations leading to instability during the bounce. Our findings underscore the unique contributions of Finsler geometry to cosmological models, offering deeper insights into the behavior of the universe under anisotropic influences and providing a potential avenue for addressing longstanding challenges in cosmology.
在这项研究中,我们在芬斯勒-兰德斯几何框架内探索了物质反弹宇宙学的动力学,重点研究了芬斯勒修正项η(t)的作用。通过将芬斯勒几何整合到宇宙学模型中,我们引入了各向异性效应,这些效应对宇宙的演化产生了重大影响,尤其是在反弹阶段。研究考察了各种宇宙学参数,包括减速(qη(t))、突变(jη(t))和弹跳(sη(t))参数,强调了芬斯勒修正对这些关键指标的影响。我们的研究结果表明,与传统的黎曼模型相比,芬斯勒框架会导致宇宙膨胀动力学发生更加复杂和突然的转变。研究还发现,芬斯勒修正加剧了对能量条件的违反,如零能量条件(NEC),这对成功反弹的发生至关重要。此外,对声速平方 vs2 的分析表明,模型的稳定性对芬斯勒参数的选择高度敏感,某些配置会导致反弹过程中的不稳定性。我们的发现强调了芬斯勒几何对宇宙学模型的独特贡献,为各向异性影响下的宇宙行为提供了更深入的见解,并为解决宇宙学中长期存在的挑战提供了潜在的途径。
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引用次数: 0
A universal energy relation between synchrotron and synchrotron self-Compton radiation in GRBs and blazars 同步辐射与同步辐射自康普顿辐射在全球热射线暴和炽星中的普遍能量关系
IF 10.2 4区 物理与天体物理 Q1 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-10-16 DOI: 10.1016/j.jheap.2024.10.007
Tao Wen , Yu-Hua Yao , Song-Zhan Chen , Ben-Zhong Dai , Yi-Qing Guo
The recent and brightest GRB 221009A observed by LHAASO marked the first detection of the onset of TeV afterglow, with a total of 7 GRBs exhibiting very high energy (VHE) afterglow radiation. However, consensus on VHE radiation of GRBs is still lacking. Multi-wavelength studies are currently a primary research method for investigating high-energy γ-ray astronomy. The limited sample of VHE GRBs, combined with their transient nature, hinders the progress of physical studies of GRBs. This paper aims to obtain useful information for GRB research through the properties of blazars, which share significant similarities with GRBs. By fitting high-quality and simultaneous multiwavelength spectral energy distributions with a one-zone leptonic model, the study explores the similarity of radiation properties of blazars and GRBs. A tight correlation between synchrotron and synchrotron self-Compton (SSC) emission luminosities suggests that blazars and GRBs share similar radiation mechanisms, to be specific, synchrotron radiation produces the observed X-ray photons, which also serve as targets for electrons in the SSC process. We hope that ground-based experiments can observe more GRBs in sub-TeV to confirm these findings.
最近由LHAASO观测到的最亮的GRB 221009A标志着首次探测到TeV余辉的开始,总共有7个GRB表现出极高能(VHE)余辉辐射。然而,人们对 GRB 的 VHE 辐射仍然缺乏共识。多波长研究是目前研究高能γ射线天文学的主要方法。VHE GRBs 样本有限,加之其瞬态性质,阻碍了 GRBs 物理研究的进展。本文旨在通过与 GRBs 有着显著相似性的类星体的特性来获取对 GRB 研究有用的信息。通过用单区轻子模型拟合高质量的多波长同步光谱能量分布,该研究探索了类星体和古雷暴暴的辐射特性的相似性。同步加速器和同步加速器自康普顿(SSC)发射光度之间的紧密相关性表明,蓝星和GRB具有相似的辐射机制,具体来说,同步加速器辐射产生了观测到的X射线光子,而X射线光子也是SSC过程中电子的目标。我们希望地面实验能够观测到更多的亚天文单位的GRB,以证实这些发现。
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引用次数: 0
Bouncing universe scenarios in an extended gravitational framework involving curvature-matter coupling 涉及曲率-物质耦合的扩展引力框架中的弹跳宇宙情景
IF 10.2 4区 物理与天体物理 Q1 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-10-10 DOI: 10.1016/j.jheap.2024.10.005
M. Zubair , Quratulien Muneer , Saira Waheed , G. Dilara Açan Yildiz , Ertan Gudekli
Exploration of bouncing cosmic models in modified theories has gained much popularity in modern cosmology. This paper explores the Lagrangian function of a new theory namely F(R,Lm,T) framework by taking four renowned cosmic bouncing models, i.e., the exponential bounce, oscillatory bounce scenario, power law, and matter bouncing. Our primary objective is to fix the form of F(R,Lm,T) function for each model and investigate which kinds of reconstructed Lagrangian function have potential of regenerating bouncing scenario in terms of analytical form. It is seen that except power law model, the analytical solutions are conceivable only for certain cases of these bouncing models. For power law bounce, different cases of Lagrangian function may be rebuilt analytically while for some other bouncing scenarios, it is found that particular solutions are not always attainable and hence only the complimentary solutions can be explored. Further, we examine the behavior of energy constraints and stability of these analytically formed bouncing solutions. Additionally, we determine that the dark energy phase in F(R,Lm,T) gravity is compatible with the experimental data of BAO+Sne-Ia+CMB+H(z) and it is shown that cosmic bounce can be produced with dark energy eras in this gravity. We also present some constraints on the model parameters with Hubble parameter values and ΛCDM to determine the best-fit values of model via least square and reduced chi-squares methods. It is concluded that matter bounce model is the best fitted with the observational data set as well as ΛCDM model because it has least value of χm2.
对修正理论中宇宙弹跳模型的探索在现代宇宙学中颇受欢迎。本文以指数反弹、振荡反弹、幂律反弹和物质反弹四种著名的宇宙反弹模型为研究对象,探讨了一种新理论即F(R,Lm,T)框架的拉格朗日函数。我们的主要目的是确定每种模型的 F(R,Lm,T)函数形式,并研究哪种重构的拉格朗日函数在解析形式上具有再生弹跳情景的潜力。结果表明,除幂律模型外,只有在这些弹跳模型的某些情况下才可能得到解析解。对于幂律反弹,拉格朗日函数的不同情况都可以通过分析重建,而对于其他一些反弹情况,我们发现并不总是可以获得特定的解,因此只能探索补充解。此外,我们还研究了能量约束的行为以及这些通过分析形成的弹跳解的稳定性。此外,我们确定 F(R,Lm,T)引力中的暗能量阶段与 BAO+Sne-Ia+CMB+H(z)的实验数据是兼容的,并证明在这种引力中暗能量时代可以产生宇宙反弹。我们还提出了哈勃参数值和ΛCDM对模型参数的一些约束,通过最小二乘法和缩小二乘法确定模型的最佳拟合值。结论是物质反弹模型与观测数据集以及ΛCDM模型拟合得最好,因为它的χm2值最小。
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引用次数: 0
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Journal of High Energy Astrophysics
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