P. Atri, S. E. Motta, J. van den Eijnden, J. H. Matthews, J. C. A. Miller-Jones, R. Fender, D. Williams-Baldwin, I. Heywood, P. Woudt
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Jet–interstellar medium (ISM) interaction sites near black hole X-ray binaries provide unique laboratories that provide insights into the energetics of the jets launched from stellar-mass black holes.<i>Aims.<i/> This work aims to detect and characterise the bow shock near one black hole X-ray binary, Cyg X-1, and then use this bow shock structure to parametrise the properties of the jet launched by Cyg X-1 over its lifetime.<i>Methods.<i/> We used the MeerKAT radio telescope to investigate the bow shock structure formed by the interaction between the jets of Cyg X-1 and the ISM. Using new <i>L<i/>- and <i>S<i/>-band detections of the bow shock, we constrained the density of the unshocked ISM and mapped the bow shock’s spectral index. These values were applied to self-similar models developed initially for FR II galaxies to estimate the energy transport rate and the age of Cyg X-1 jets.<i>Results.<i/> We successfully detect the bow shock north of Cyg X-1 in the <i>L<i/> and <i>S<i/> bands and report its size and brightness. We present the spectral index distribution across the bow shock, which is in the range −0.9 ≤ <i>α<i/> ≤ 0.4, with an error distribution (0.6 ≤ Δ<i>α<i/> ≤ 1.5) that peaks at unity. We determine that the unshocked ISM density is 6–7 cm<sup>−3<sup/> for a temperature range of 10<sup>4<sup/>–3 × 10<sup>6<sup/> K. This temperature range suggests that the velocity of the bow shock is 21 km s km s<sup>−1<sup/>. The age of the Cyg X-1 jet responsible for the bow shock is 0.04–0.3 Myr, and the power of the jet is constrained to 2 × 10<sup>31<sup/> ergs s ergs s<sup>−1<sup/> for the case of opening angles of 0.3°–2.0°. We also detect new morphological features of the bow shock in the <i>S<i/>-band image. The comparison of archival H<sub><i>α<i/><sub/> maps with the new radio observations hints at different regions of emission, different temperature ranges, and different ISM densities.<i>Conclusions.<i/> MeerKAT’s sensitivity and resolution effectively reveal low surface brightness features of the Cyg X-1 bow shock. The spectral index suggests a consistent emission origin across the structure. The ISM density around Cyg X-1 is on the higher end for Galactic environments, and our results indicate a lower jet energy transport rate than prior estimates. Further searches with MeerKAT will help build a statistically significant sample, advancing our understanding of black hole X-ray binary jets and their impact on their local environments.","PeriodicalId":8571,"journal":{"name":"Astronomy & Astrophysics","volume":"108 1","pages":""},"PeriodicalIF":5.4000,"publicationDate":"2025-04-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Quantifying jet–interstellar medium interactions in Cyg X-1: Insights from dual-frequency bow shock detection with MeerKAT\",\"authors\":\"P. Atri, S. E. Motta, J. van den Eijnden, J. H. Matthews, J. C. A. Miller-Jones, R. Fender, D. Williams-Baldwin, I. Heywood, P. Woudt\",\"doi\":\"10.1051/0004-6361/202452837\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<i>Context.<i/> Accretion and outflows are astrophysical phenomena observed across a wide range of objects, from white dwarfs to supermassive black holes. Developing a complete picture of these processes requires complementary studies across this full spectrum of jet-launching sources. Jet–interstellar medium (ISM) interaction sites near black hole X-ray binaries provide unique laboratories that provide insights into the energetics of the jets launched from stellar-mass black holes.<i>Aims.<i/> This work aims to detect and characterise the bow shock near one black hole X-ray binary, Cyg X-1, and then use this bow shock structure to parametrise the properties of the jet launched by Cyg X-1 over its lifetime.<i>Methods.<i/> We used the MeerKAT radio telescope to investigate the bow shock structure formed by the interaction between the jets of Cyg X-1 and the ISM. Using new <i>L<i/>- and <i>S<i/>-band detections of the bow shock, we constrained the density of the unshocked ISM and mapped the bow shock’s spectral index. These values were applied to self-similar models developed initially for FR II galaxies to estimate the energy transport rate and the age of Cyg X-1 jets.<i>Results.<i/> We successfully detect the bow shock north of Cyg X-1 in the <i>L<i/> and <i>S<i/> bands and report its size and brightness. We present the spectral index distribution across the bow shock, which is in the range −0.9 ≤ <i>α<i/> ≤ 0.4, with an error distribution (0.6 ≤ Δ<i>α<i/> ≤ 1.5) that peaks at unity. We determine that the unshocked ISM density is 6–7 cm<sup>−3<sup/> for a temperature range of 10<sup>4<sup/>–3 × 10<sup>6<sup/> K. This temperature range suggests that the velocity of the bow shock is 21 km s km s<sup>−1<sup/>. The age of the Cyg X-1 jet responsible for the bow shock is 0.04–0.3 Myr, and the power of the jet is constrained to 2 × 10<sup>31<sup/> ergs s ergs s<sup>−1<sup/> for the case of opening angles of 0.3°–2.0°. We also detect new morphological features of the bow shock in the <i>S<i/>-band image. The comparison of archival H<sub><i>α<i/><sub/> maps with the new radio observations hints at different regions of emission, different temperature ranges, and different ISM densities.<i>Conclusions.<i/> MeerKAT’s sensitivity and resolution effectively reveal low surface brightness features of the Cyg X-1 bow shock. The spectral index suggests a consistent emission origin across the structure. The ISM density around Cyg X-1 is on the higher end for Galactic environments, and our results indicate a lower jet energy transport rate than prior estimates. 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引用次数: 0
摘要
上下文。吸积和喷流是一种天体物理现象,从白矮星到超大质量黑洞,在各种各样的物体上都能观察到。要想对这些过程有一个完整的了解,就需要对整个喷射源进行补充研究。黑洞x射线双星附近的喷流-星际介质(ISM)相互作用点提供了独特的实验室,可以深入了解从恒星质量黑洞发射的喷流的能量学。这项工作的目的是探测和表征一个黑洞x射线双星Cyg X-1附近的弓形激波,然后使用这种弓形激波结构来参数化Cyg X-1在其生命周期内发射的射流的特性。我们使用MeerKAT射电望远镜研究了Cyg X-1喷流与ISM相互作用形成的弓形激波结构。利用新的弓形激波的L和s波段探测,我们限制了未受激波的ISM的密度,并绘制了弓形激波的谱指数。这些值被应用到最初为FR II星系开发的自相似模型中,以估计Cyg X-1喷流的能量传输速率和年龄。我们成功地在L和S波段探测到Cyg X-1北部的弓形激波,并报告了它的大小和亮度。我们给出了整个弓形激波的谱指数分布,其范围为−0.9≤α≤0.4,误差分布(0.6≤Δα≤1.5)在单位处达到峰值。我们确定在104-3 × 106 K的温度范围内,未受冲击的ISM密度为6-7 cm−3。这个温度范围表明弓形激波的速度为21 km s km s−1。产生弓形激波的Cyg X-1射流的年龄为0.04-0.3 Myr,在开口角为0.3°-2.0°的情况下,射流的功率限制为2 × 1031 ergs s−1。我们还在s波段图像中发现了弓形激波的新的形态学特征。档案的Hα图与新的射电观测结果的比较暗示了不同的发射区域、不同的温度范围和不同的ISM密度。MeerKAT的灵敏度和分辨率有效地揭示了Cyg X-1弓形激波的低表面亮度特征。光谱指数表明整个结构具有一致的发射源。Cyg X-1周围的ISM密度在银河系环境中处于较高的一端,我们的结果表明射流能量传输率比先前估计的要低。MeerKAT的进一步搜索将有助于建立一个具有统计意义的样本,提高我们对黑洞x射线双星射流及其对当地环境的影响的理解。
Quantifying jet–interstellar medium interactions in Cyg X-1: Insights from dual-frequency bow shock detection with MeerKAT
Context. Accretion and outflows are astrophysical phenomena observed across a wide range of objects, from white dwarfs to supermassive black holes. Developing a complete picture of these processes requires complementary studies across this full spectrum of jet-launching sources. Jet–interstellar medium (ISM) interaction sites near black hole X-ray binaries provide unique laboratories that provide insights into the energetics of the jets launched from stellar-mass black holes.Aims. This work aims to detect and characterise the bow shock near one black hole X-ray binary, Cyg X-1, and then use this bow shock structure to parametrise the properties of the jet launched by Cyg X-1 over its lifetime.Methods. We used the MeerKAT radio telescope to investigate the bow shock structure formed by the interaction between the jets of Cyg X-1 and the ISM. Using new L- and S-band detections of the bow shock, we constrained the density of the unshocked ISM and mapped the bow shock’s spectral index. These values were applied to self-similar models developed initially for FR II galaxies to estimate the energy transport rate and the age of Cyg X-1 jets.Results. We successfully detect the bow shock north of Cyg X-1 in the L and S bands and report its size and brightness. We present the spectral index distribution across the bow shock, which is in the range −0.9 ≤ α ≤ 0.4, with an error distribution (0.6 ≤ Δα ≤ 1.5) that peaks at unity. We determine that the unshocked ISM density is 6–7 cm−3 for a temperature range of 104–3 × 106 K. This temperature range suggests that the velocity of the bow shock is 21 km s km s−1. The age of the Cyg X-1 jet responsible for the bow shock is 0.04–0.3 Myr, and the power of the jet is constrained to 2 × 1031 ergs s ergs s−1 for the case of opening angles of 0.3°–2.0°. We also detect new morphological features of the bow shock in the S-band image. The comparison of archival Hα maps with the new radio observations hints at different regions of emission, different temperature ranges, and different ISM densities.Conclusions. MeerKAT’s sensitivity and resolution effectively reveal low surface brightness features of the Cyg X-1 bow shock. The spectral index suggests a consistent emission origin across the structure. The ISM density around Cyg X-1 is on the higher end for Galactic environments, and our results indicate a lower jet energy transport rate than prior estimates. Further searches with MeerKAT will help build a statistically significant sample, advancing our understanding of black hole X-ray binary jets and their impact on their local environments.
期刊介绍:
Astronomy & Astrophysics is an international Journal that publishes papers on all aspects of astronomy and astrophysics (theoretical, observational, and instrumental) independently of the techniques used to obtain the results.