Evidence for particle acceleration approaching PeV energies in the W51 complex

preprint2026arXivOpen access
The LHAASO CollaborationZhen CaoF. AharonianAxikeguY. X. BaiY. W. BaoD. BastieriX. J. BiY. J. BiW. BianA. V. BukevichQ. CaoW. Y. CaoZhe CaoJ. ChangJ. F. ChangM. ChenE. S. ChenH. X. ChenLiang ChenLin ChenLong ChenM. J. ChenM. L. ChenQ. H. ChenS. ChenS. H. ChenS. Z. ChenT. L. ChenY. ChenN. ChengY. D. ChengM. Y. CuiS. W. CuiX. H. CuiY. D. CuiB. Z. DaiH. L. DaiZ. G. DaiDanzengluobuX. Q. DongK. K. DuanJ. H. FanY. Z. FanJ. FangJ. H. FangK. FangC. F. FengH. FengL. FengS. H. FengX. T. FengY. FengY. L. FengS. GabiciB. GaoC. D. GaoQ. GaoW. GaoW. K. GaoM. M. GeL. S. GengG. GiacintiG. H. GongQ. B. GouM. H. GuF. L. GuoX. L. GuoY. Q. GuoY. Y. GuoY. A. HanM. HasanH. H. HeH. N. HeJ. Y. HeY. HeY. K. HorB. W. HouC. HouX. HouH. B. HuQ. HuS. C. HuD. H. HuangT. Q. HuangW. J. HuangX. T. HuangX. Y. HuangY. HuangX. L. JiH. Y. JiaK. JiaK. JiangX. W. JiangZ. J. JiangM. JinM. M. KangI. KarpikovD. KuleshovK. KurinovB. B. LiC. M. LiCheng LiCong LiD. LiF. LiH. B. LiH. C. LiJian LiJie LiK. LiS. D. LiW. L. LiX. R. LiXin LiY. Z. LiZhe LiZhuo LiE. W. LiangY. F. LiangS. J. LinB. LiuC. LiuD. LiuD. B. LiuH. LiuH. D. LiuJ. LiuJ. L. LiuM. Y. LiuR. Y. LiuS. M. LiuW. LiuY. LiuY. N. LiuQ. LuoY. LuoH. K. LvB. Q. MaL. L. MaX. H. MaJ. R. MaoZ. MinW. MitthumsiriH. J. MuY. C. NanA. NeronovL. J. OuP. PattarakijwanichZ. Y. PeiJ. C. QiM. Y. QiB. Q. QiaoJ. J. QinA. RazaD. RuffoloA. SáizM. SaeedD. SemikozL. ShaoO. ShchegolevX. D. ShengF. W. ShuH. C. SongYu. V. StenkinV. StepanovY. SuD. X. SunQ. N. SunX. N. SunZ. B. SunJ. TakataP. H. T. TamQ. W. TangR. TangZ. B. TangW. W. TianC. WangC. B. WangG. W. WangH. G. WangH. H. WangJ. C. WangKai WangL. P. WangL. Y. WangP. H. WangR. WangW. WangX. G. WangX. Y. WangY. WangY. D. WangY. J. WangZ. H. WangZ. X. WangZhen WangZheng WangD. M. WeiJ. J. WeiY. J. WeiT. WenC. Y. WuH. R. WuQ. W. WuS. WuX. F. WuY. S. WuS. Q. XiJ. XiaG. M. XiangD. X. XiaoG. XiaoY. L. XinY. XingD. R. XiongZ. XiongD. L. XuR. F. XuR. X. XuW. L. XuL. XueD. H. YanJ. Z. YanT. YanC. W. YangC. Y. YangF. YangF. F. YangL. L. YangM. J. YangR. Z. YangW. X. YangY. H. YaoZ. G. YaoL. Q. YinN. YinX. H. YouZ. Y. YouY. H. YuQ. YuanH. YueH. D. ZengT. X. ZengW. ZengM. ZhaB. B. ZhangF. ZhangH. ZhangH. M. ZhangH. Y. ZhangJ. L. ZhangLi ZhangP. F. ZhangP. P. ZhangR. ZhangS. B. ZhangS. R. ZhangS. S. ZhangX. ZhangX. P. ZhangY. F. ZhangYi ZhangYong ZhangB. ZhaoJ. ZhaoL. ZhaoL. Z. ZhaoS. P. ZhaoX. H. ZhaoF. ZhengW. J. ZhongB. ZhouH. ZhouJ. N. ZhouM. ZhouP. ZhouR. ZhouX. X. ZhouB. Y. ZhuC. G. ZhuF. R. ZhuH. ZhuK. J. ZhuY. C. ZouX. ZuoS. Celli

Abstract

The γγ-ray emission from the W51 complex is widely acknowledged to be attributed to the interaction between the cosmic rays (CRs) accelerated by the shock of supernova remnant (SNR) W51C and the dense molecular clouds in the adjacent star-forming region, W51B. However, the maximum acceleration capability of W51C for CRs remains elusive. Based on observations conducted with the Large High Altitude Air Shower Observatory (LHAASO), we report a significant detection of γγ rays emanating from the W51 complex, with energies from 2 TeV to 200 TeV. The LHAASO measurements, for the first time, extend the γγ-ray emission from the W51 complex beyond 100 TeV and reveal a significant spectrum bending at tens of TeV. By combining the ``π0π^0-decay bump" featured data from Fermi-LAT, the broadband γγ-ray spectrum of the W51 region can be well-characterized by a simple pp-collision model. The observed spectral bending feature suggests an exponential cutoff at ∼400\sim400~TeV or a power-law break at ∼200\sim200~TeV in the CR proton spectrum, most likely providing the first evidence of SNRs serving as CR accelerators approaching the PeV regime. Additionally, two young star clusters within W51B could also be theoretically viable to produce the most energetic γγ rays observed by LHAASO. Our findings strongly support the presence of extreme CR accelerators within the W51 complex and provide new insights into the origin of Galactic CRs.

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