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Constraints on heavy decaying dark matter from 570 days of LHAASO observations

The LHAASO Collaboration, Zhen Cao, F. Aharonian, Q. An, Axikegu, L. X. Bai, Y. X. Bai, Y. W. Bao, D. Bastieri, X. J. Bi, Y. J. Bi, J. T. Cai, Zhe Cao, J. Chang, J. F. Chang, E. S. Chen, Liang Chen, Liang Chen, Long Chen, M. J. Chen, M. L. Chen, Q. H. Chen, S. H. Chen, S. Z. Chen, T. L. Chen, Y. Chen, H. L. Cheng, N. Cheng, Y. D. Cheng, S. W. Cui, X. H. Cui, Y. D. Cui, B. D Ettorre Piazzoli, B. Z. Dai, H. L. Dai, Z. G. Dai, Danzengluobu, D. della Volpe, K. K. Duan, J. H. Fan, Y. Z. Fan, Z. X. Fan, J. Fang, K. Fang, C. F. Feng, L. Feng, S. H. Feng, X. T. Feng, Y. L. Feng, B. Gao, C. D. Gao, L. Q. Gao, Q. Gao, W. Gao, W. K. Gao, M. M. Ge, L. S. Geng, G. H. Gong, Q. B. Gou, M. H. Gu, F. L. Guo, J. G. Guo, X. L. Guo, Y. Q. Guo, Y. Y. Guo, Y. A. Han, H. H. He, H. N. He, S. L. He, X. B. He, Y. He, M. Heller, Y. K. Hor, C. Hou, X. Hou, H. B. Hu, Q. Hu, S. Hu, S. C. Hu, X. J. Hu, D. H. Huang, W. H. Huang, X. T. Huang, X. Y. Huang, Y. Huang, Z. C. Huang, X. L. Ji, H. Y. Jia, K. Jia, K. Jiang, Z. J. Jiang, M. Jin, M. M. Kang, T. Ke, D. Kuleshov, K. Levochkin, B. B. Li, Cheng Li, Cong Li, F. Li, H. B. Li, H. C. Li, H. Y. Li, J. Li, Jian Li, Jie Li, K. Li, W. L. Li, X. R. Li, Xin Li, Xin Li, Y. Z. Li, Zhe Li, Zhuo Li, E. W. Liang, Y. F. Liang, S. J. Lin, B. Liu, C. Liu, D. Liu, H. Liu, H. D. Liu, J. Liu, J. L. Liu, J. S. Liu, J. Y. Liu, M. Y. Liu, R. Y. Liu, S. M. Liu, W. Liu, Y. Liu, Y. N. Liu, W. J. Long, R. Lu, Q. Luo, H. K. Lv, B. Q. Ma, L. L. Ma, X. H. Ma, J. R. Mao, A. Masood, Z. Min, W. Mitthumsiri, Y. C. Nan, Z. W. Ou, B. Y. Pang, P. Pattarakijwanich, Z. Y. Pei, M. Y. Qi, Y. Q. Qi, B. Q. Qiao, J. J. Qin, D. Ruffolo, A. Saiz, C. Y. Shao, L. Shao, O. Shchegolev, X. D. Sheng, J. Y. Shi, H. C. Song, Yu. V. Stenkin, V. Stepanov, Y. Su, Q. N. Sun, X. N. Sun, Z. B. Sun, P. H. T. Tam, Z. B. Tang, W. W. Tian, B. D. Wang, C. Wang, H. Wang, H. G. Wang, J. C. Wang, J. S. Wang, L. P. Wang, L. Y. Wang, R. Wang, R. N. Wang, W. Wang, X. G. Wang, X. Y. Wang, Y. Wang, Y. D. Wang, Y. J. Wang, Y. P. Wang, Z. H. Wang, Z. X. Wang, Zhen Wang, Zheng Wang, D. M. Wei, J. J. Wei, Y. J. Wei, T. Wen, C. Y. Wu, H. R. Wu, S. Wu, X. F. Wu, Y. S. Wu, S. Q. Xi, J. Xia, J. J. Xia, G. M. Xiang, D. X. Xiao, G. Xiao, G. G. Xin, Y. L. Xin, Y. Xing, Z. Xiong, D. L. Xu, R. X. Xu, L. Xue, D. H. Yan, J. Z. Yan, C. W. Yang, F. F. Yang, H. W. Yang, J. Y. Yang, L. L. Yang, M. J. Yang, R. Z. Yang, S. B. Yang, Y. H. Yao, Z. G. Yao, Y. M. Ye, L. Q. Yin, N. Yin, X. H. You, Z. Y. You, Y. H. Yu, Q. Yuan, H. Yue, H. D. Zeng, T. X. Zeng, W. Zeng, Z. K. Zeng, M. Zha, X. X. Zhai, B. B. Zhang, F. Zhang, H. M. Zhang, H. Y. Zhang, J. L. Zhang, L. X. Zhang, Li Zhang, Lu Zhang, P. F. Zhang, P. P. Zhang, R. Zhang, S. B. Zhang, S. R. Zhang, S. S. Zhang, X. Zhang, X. P. Zhang, Y. F. Zhang, Y. L. Zhang, Yi Zhang, Yong Zhang, B. Zhao, J. Zhao, L. Zhao, L. Z. Zhao, S. P. Zhao, F. Zheng, Y. Zheng, B. Zhou, H. Zhou, J. N. Zhou, P. Zhou, R. Zhou, X. X. Zhou, C. G. Zhu, F. R. Zhu, H. Zhu, K. J. Zhu, X. Zuo, S. Ando, M. Chianese, D. F. G. Fiorillo, G. Miele, K. C. Y. Ng

TL;DR

The study targets heavy decaying dark matter in the mass range $10^{5}$–$10^{9}$ GeV by exploiting LHAASO-KM2A data from partial instrument operation. It employs a five-region, joint likelihood analysis that leverages the DM angular distribution across ROIs and includes both prompt and secondary Galactic IC gamma components, with a detailed treatment of detector response and backgrounds. The analysis yields 95% CL lower limits on the DM lifetime $ au_ ext{DM}$ that surpass previous gamma-ray constraints by factors of several, thereby challenging DM explanations for IceCube's diffuse high-energy neutrino flux in non-neutrino channels. The results demonstrate LHAASO-KM2A's strong DM indirect-detection capability with partial data and portend substantial improvements with full KM2A, additional detectors, and refined astrophysical modeling.

Abstract

The Kilometer Square Array~(KM2A) of the Large High Altitude Air Shower Observatory (LHAASO) aims at surveying the northern gamma-ray sky at energies above 10 TeV with unprecedented sensitivity. Gamma-ray observations have long been one of the most powerful tools for dark matter searches, as e.g., high-energy gamma-rays could be produced by the decays of heavy dark matter particles. In this letter, we present the first dark matter analysis with LHAASO-KM2A, using the first 340~days of data from 1/2-KM2A and 230~days of data from 3/4-KM2A. Several regions of interest are used to search for a signal and account for the residual cosmic-ray background after gamma/hadron separation. We find no excess of dark matter signals, and thus place some of the strongest gamma-ray constraints on the lifetime of heavy dark matter particles with mass between 10^5 and 10^9~GeV. Our results with LHAASO are robust, and have important implications for dark matter interpretations of the diffuse astrophysical high-energy neutrino emission.

Constraints on heavy decaying dark matter from 570 days of LHAASO observations

TL;DR

The study targets heavy decaying dark matter in the mass range GeV by exploiting LHAASO-KM2A data from partial instrument operation. It employs a five-region, joint likelihood analysis that leverages the DM angular distribution across ROIs and includes both prompt and secondary Galactic IC gamma components, with a detailed treatment of detector response and backgrounds. The analysis yields 95% CL lower limits on the DM lifetime that surpass previous gamma-ray constraints by factors of several, thereby challenging DM explanations for IceCube's diffuse high-energy neutrino flux in non-neutrino channels. The results demonstrate LHAASO-KM2A's strong DM indirect-detection capability with partial data and portend substantial improvements with full KM2A, additional detectors, and refined astrophysical modeling.

Abstract

The Kilometer Square Array~(KM2A) of the Large High Altitude Air Shower Observatory (LHAASO) aims at surveying the northern gamma-ray sky at energies above 10 TeV with unprecedented sensitivity. Gamma-ray observations have long been one of the most powerful tools for dark matter searches, as e.g., high-energy gamma-rays could be produced by the decays of heavy dark matter particles. In this letter, we present the first dark matter analysis with LHAASO-KM2A, using the first 340~days of data from 1/2-KM2A and 230~days of data from 3/4-KM2A. Several regions of interest are used to search for a signal and account for the residual cosmic-ray background after gamma/hadron separation. We find no excess of dark matter signals, and thus place some of the strongest gamma-ray constraints on the lifetime of heavy dark matter particles with mass between 10^5 and 10^9~GeV. Our results with LHAASO are robust, and have important implications for dark matter interpretations of the diffuse astrophysical high-energy neutrino emission.
Paper Structure (6 sections, 16 equations, 8 figures, 2 tables)

This paper contains 6 sections, 16 equations, 8 figures, 2 tables.

Figures (8)

  • Figure 1: 95% one-sided lower limits on DM lifetime obtained with the profile likelihood analysis (thick black lines), for DM decaying into $b$ quarks (left) or $\tau$ leptons (right). The black dashed line shows the limit obtained if we only consider prompt DM contribution. The green and yellow bands correspond to the expected 68% and 95% limit ranges from Monte Carlo simulations with the background-only hypothesis. Previous limits Cohen:2016uygIshiwata:2019aetChianese:2021jke and those from HAWC Abeysekara:2017jxs are shown with gray and blue lines
  • Figure S1: Pixelated sky map highlighting the selected ROIs, labeled with indices from 0 to 4, in Galactic (left panel) and equatorial (right panel) coordinates. The dark band shows 10 degrees around the Galactic plane.
  • Figure S2: The $\gamma$-ray and cosmic-ray survival fractions after $\gamma$/hadron separation. $\gamma$-ray events are obtained via simulation, while the cosmic-ray events are the actual 1/2-KM2A and 3/4-KM2A data.
  • Figure S3: Total DM $\gamma$-ray intensity (solid lines) from ROI$_0$ for the benchmark case of DM particles with $10^7$ GeV mass and $10^{28}$ s lifetime. The dashed lines show the prompt Galactic component, while the shaded regions highlight the additional contribution due to the secondary Galactic IC component. Different colors correspond to different decay channels.
  • Figure S4: Total $\gamma$-ray intensity from DM decays in ROI$_0$ obtained with (solid black lines) and without (dashed red lines) the SL+IR Galactic photon background, for $b\bar{b}$ and $\tau^{+}\tau{-}$ channels and with same parameters as Fig. \ref{['fig:DMfluxes']}. The lower panels show the ratio of the flux without SL+IR over the that with SL+IR.
  • ...and 3 more figures