Very High-energy Gamma-Ray Episodic Activity of Radio Galaxy NGC 1275 in 2022–2023 Measured with MACE

S. Godambe, N. Mankuzhiyil, C. Borwankar, B. Ghosal, A. Tolamatti, M. Pal, P. Chandra, M. Khurana, P. Pandey, Z. A. Dar, S. Godiyal, J. Hariharan, Keshav Anand, S. Norlha, D. Sarkar, R. Thubstan, K. Venugopal, A. Pathania, S. Kotwal, Raj Kumar, N. Bhatt, K. Chanchalani, M. Das, K. K. Singh, K. K. Gour, M. Kothari, Nandan Kumar, Naveen Kumar, P. Marandi, C. P. Kushwaha, M. K. Koul, P. Dorjey, N. Dorji, V. R. Chitnis, R. C. Rannot, S. Bhattacharyya, N. Chouhan, V. K. Dhar, M. Sharma and K. K. Yadav
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Abstract

The radio galaxy NGC 1275, located at the central region of Perseus cluster, is a well-known very high-energy (VHE) gamma-ray emitter. The Major Atmospheric Cherenkov Experiment Telescope has detected two distinct episodes of VHE (E > 80 GeV) gamma-ray emission from NGC 1275 during 2022 December and 2023 January. The second outburst, observed on 2023 January 10, was the more intense of the two, with flux reaching 58% of the Crab Nebula flux above 80 GeV. The differential energy spectrum measured between 80 GeV and can be described by a power law with a spectral index of Γ = −2.90 ± 0.16stat for both flaring events. The broadband spectral energy distribution derived from these flares, along with quasisimultaneous low-energy counterparts, suggests that the observed gamma-ray emission can be explained using a homogeneous single-zone synchrotron self-Compton model. The physical parameters derived from this model for both flaring states are similar. The intermediate state observed between two flaring episodes is explained by a lower Doppler factor or magnetic field, which subsequently returned to its previous value during the high-activity state observed on 2023 January 10.
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用 MACE 测量射电星系 NGC 1275 在 2022-2023 年的超高能量伽马射线外显活动
位于英仙座星系团中心区域的射电星系NGC 1275是一个著名的超高能量(VHE)伽马射线发射器。大大气切伦科夫实验望远镜在2022年12月和2023年1月期间探测到NGC 1275发出了两次不同的VHE(E > 80 GeV)伽马射线。2023年1月10日观测到的第二次爆发是两次爆发中强度最大的一次,80 GeV以上的通量达到蟹状星云通量的58%。在这两次爆发事件中,80 GeV 和 80 GeV 之间测量到的差能谱可以用幂律描述,光谱指数为 Γ = -2.90 ± 0.16stat。从这些耀斑得出的宽带光谱能量分布,以及准同步低能对应物,表明观测到的伽马射线发射可以用一个同质单区同步加速器自康普顿模型来解释。根据该模型得出的两种耀斑状态的物理参数是相似的。在两次耀斑之间观测到的中间状态可以用较低的多普勒因子或磁场来解释,而在 2023 年 1 月 10 日观测到的高活性状态期间,磁场又恢复到了先前的值。
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