Study of Ultra-High-Energy Gamma-Ray Source 1LHAASO J0056+6346u and Its Possible Origins

preprint2025arXivOpen access
Zhen CaoF. AharonianY. X. BaiY. W. BaoD. BastieriX. J. BiY. J. BiW. BianJ. BlunierA. V. BukevichC. M. CaiY. Y. CaiW. Y. CaoZhe CaoJ. ChangJ. F. ChangE. S. ChenG. H. ChenH. K. ChenL. F. ChenLiang ChenLong ChenM. J. ChenM. L. ChenQ. H. ChenS. ChenS. H. ChenS. Z. ChenT. L. ChenX. B. ChenX. J. ChenX. P. ChenY. ChenN. ChengQ. Y. ChengY. D. ChengM. Y. CuiS. W. CuiX. H. CuiY. D. CuiB. Z. DaiH. L. DaiZ. G. DaiDanzengluobuY. X. DiaoA. J. DongX. Q. DongK. K. DuanJ. H. FanY. Z. FanJ. FangJ. H. FangK. FangC. F. FengH. FengL. FengS. H. FengX. T. FengY. FengY. L. FengS. GabiciB. GaoQ. GaoW. GaoW. K. GaoM. M. GeT. T. GeL. S. GengG. GiacintiG. H. GongQ. B. GouM. H. GuF. L. GuoJ. GuoK. J. GuoX. L. GuoY. Q. GuoY. Y. GuoR. P. HanO. A. HannukselaM. HasanH. H. HeH. N. HeJ. Y. HeX. Y. HeY. HeS. Hernández-CadenaB. W. HouC. HouX. HouH. B. HuS. C. HuC. HuangD. H. HuangJ. J. HuangX. L. HuangX. T. HuangX. Y. HuangY. HuangY. Y. HuangA. InventarX. L. JiH. Y. JiaK. JiaH. B. JiangK. JiangX. W. JiangZ. J. JiangM. JinS. KaciM. M. KangI. KarpikovD. KhangulyanD. KuleshovK. KurinovCheng LiCong LiD. LiF. LiH. B. LiH. C. LiJian LiJie LiK. LiL. LiR. L. LiS. D. LiT. Y. LiW. L. LiX. R. LiXin LiY. LiZhe LiZhuo LiE. W. LiangY. F. LiangS. J. LinB. LiuC. LiuD. LiuD. B. LiuH. LiuJ. LiuJ. L. LiuJ. R. LiuM. Y. LiuR. Y. LiuS. M. LiuW. LiuX. LiuY. LiuY. N. LiuY. Q. LouQ. LuoY. LuoH. K. LvB. Q. MaL. L. MaX. H. MaI. O. MaliyJ. R. MaoZ. MinW. MitthumsiriY. MizunoG. B. MouA. NeronovK. C. Y. NgM. Y. NiL. NieL. J. OuZ. W. OuP. PattarakijwanichZ. Y. PeiD. Y. PengJ. C. QiM. Y. QiJ. J. QinD. QuA. RazaC. Y. RenD. RuffoloA. SáizD. SavchenkoD. SemikozL. ShaoO. ShchegolevY. Z. ShenX. D. ShengZ. D. ShiF. W. ShuH. C. SongYu. V. StenkinV. StepanovY. SuD. X. SunH. SunJ. X. SunQ. N. SunX. N. SunZ. B. SunN. H. TabasamJ. TakataP. H. T. TamH. B. TanQ. W. TangR. TangZ. B. TangW. W. TianC. N. TongL. H. WanC. WangD. H. WangG. W. WangH. G. WangJ. C. WangK. WangKai WangL. P. WangL. Y. WangR. WangW. WangX. G. WangX. J. WangX. Y. WangY. WangY. D. WangZ. H. WangZ. X. WangZheng WangD. M. WeiJ. J. WeiY. J. WeiT. WenS. S. WengC. Y. WuH. R. WuQ. W. WuS. WuX. F. WuY. S. WuS. Q. XiJ. XiaJ. J. XiaG. M. XiangD. X. XiaoG. XiaoY. F. XiaoY. L. XinH. D. XingY. XingD. R. XiongB. N. XuC. Y. XuD. L. XuR. F. XuR. X. XuS. S. XuW. L. XuL. XueD. H. YanT. YanC. W. YangC. Y. YangF. F. YangL. L. YangM. J. YangR. Z. YangW. X. YangZ. H. YangZ. G. YaoX. A. YeL. Q. YinN. YinX. H. YouZ. Y. YouQ. YuanH. YueH. D. ZengT. X. ZengW. ZengX. T. ZengM. ZhaB. B. ZhangB. T. ZhangC. ZhangH. ZhangH. M. ZhangH. Y. ZhangJ. L. ZhangJ. Y. ZhangLi ZhangP. F. ZhangR. ZhangS. R. ZhangS. S. ZhangS. Y. ZhangW. ZhangW. Y. ZhangX. ZhangX. P. ZhangYi ZhangYong ZhangZ. P. ZhangJ. ZhaoL. ZhaoL. Z. ZhaoS. P. ZhaoX. H. ZhaoZ. H. ZhaoF. ZhengT. C. ZhengB. ZhouH. ZhouJ. N. ZhouM. ZhouP. ZhouR. ZhouX. X. ZhouB. Y. ZhuC. G. ZhuF. R. ZhuH. ZhuK. J. ZhuY. C. ZouX. Zuo

Abstract

We report a dedicated study of the newly discovered extended UHE γγ-ray source 1LHAASO J0056+6346u. Analyzing 979 days of LHAASO-WCDA data and 1389 days of LHAASO-KM2A data, we observed a significant excess of γγ-ray events with both WCDA and KM2A. Assuming a point power-law source with a fixed spectral index, the significance maps reveal excesses of ∼12.65 σ{\sim}12.65\,σ, ∼22.18 σ{\sim}22.18\,σ, and ∼10.24 σ{\sim}10.24\,σ in the energy ranges of 1--25 TeV, 25--100 TeV, and >100> 100 TeV, respectively. We use a 3D likelihood algorithm to derive the morphological and spectral parameters, and the source is detected with significances of 12.65 σ12.65\,σ by WCDA and 25.27 σ25.27\,σ by KM2A. The best-fit positions derived from WCDA and KM2A data are (R.A. = 13.96∘±0.09∘13.96^\circ\pm0.09^\circ, Decl. = 63.92∘±0.05∘63.92^\circ\pm0.05^\circ) and (R.A. = 14.00∘±0.05∘14.00^\circ\pm0.05^\circ, Decl. = 63.79∘±0.02∘63.79^\circ\pm0.02^\circ), respectively. The angular size (r39r_{39}) of 1LHAASO J0056+6346u is 0.34∘±0.04∘0.34^\circ\pm0.04^\circ at 1--25 TeV and 0.24∘±0.02∘0.24^\circ\pm0.02^\circ at >25> 25 TeV. The differential flux of this UHE γγ-ray source can be described by an exponential cutoff power-law function: (2.67±0.25)×10−15(E/20 TeV)−1.97±0.10e−E/(55.1±7.2) TeV TeV−1 cm−2 s−1(2.67\pm0.25) \times 10^{-15} (E/20\,\text{TeV})^{-1.97\pm0.10} e^{-E/(55.1\pm7.2)\,\text{TeV}} \,\text{TeV}^{-1}\,\text{cm}^{-2}\,\text{s}^{-1}. To explore potential sources of γγ-ray emission, we investigated the gas distribution around 1LHAASO J0056+6346u. 1LHAASO J0056+6346u is likely to be a TeV PWN powered by an unknown pulsar, which would naturally explain both its spatial and spectral properties. Another explanation is that this UHE γγ-ray source might be associated with gas content illuminated by a nearby CR accelerator, possibly the SNR candidate G124.0+1.4.

Explore this paper’s authors, topics and related work.

Building this map preview

BZPEER is loading the nearby papers, people, topics and institutions for this page.

Reviews 0

Write a reviewWrite

No reviews yet.

Discussion 0

Add a commentWrite

No comments yet.