Constraining the Cosmic-ray Energy Based on Observations of Nearby Galaxy Clusters by LHAASO

preprint2026arXivOpen access
The LHAASO CollaborationZhen 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

Galaxy clusters act as reservoirs of high-energy cosmic rays (CRs). As CRs propagate through the intracluster medium, they generate diffuse γγ-rays detectable by arrays such as LHAASO. These γγ-rays result from proton-proton (pppp) collisions of very high-energy cosmic rays (VHECRs) or inverse Compton (IC) scattering of positron-electron pairs created by pγpγ interactions of ultra-high-energy cosmic rays (UHECRs). We analyzed diffuse γγ-ray emission from the Coma, Perseus, and Virgo clusters using LHAASO data. Diffuse emission was modeled as a disk of radius R500R_{500} for each cluster while accounting for point sources. No significant diffuse emission was detected, yielding 95\% confidence level (C.L.) upper limits on the γγ-ray flux: for WCDA (1-25~TeV) and KM2A (>25>25~TeV), less than (49.4,13.7,54.0)(49.4, 13.7, 54.0) and (1.34,1.14,0.40)×10−14(1.34, 1.14, 0.40) \times 10^{-14}~ph~cm−2^{-2}~s−1^{-1} for Coma, Perseus, and Virgo, respectively. The γγ-ray upper limits can be used to derive model-independent constraints on the integral energy of CRp above 10~TeV (corresponding to the LHAASO observational range >1>1~TeV under the pppp scenario) to be less than (1.96,0.59,0.08)×1061(1.96, 0.59, 0.08) \times 10^{61}~erg. The absence of detectable annuli/ring-like structures, indicative of cluster accretion or merging shocks, imposes further constraints on models in which the UHECRs are accelerated in the merging shocks of galaxy clusters.

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.