19–23 Dec 2024
Asia/Shanghai timezone

Contribution List

90 out of 90 displayed
  1. Jianxin Lu (USTC)
    20/12/2024, 08:30
  2. Lailin Xu (USTC), Nan Lu (University of Science and Technology of China)
    20/12/2024, 08:35
  3. Jiayin Gu (Fudan University)
    20/12/2024, 08:40
  4. Shuo Han
    20/12/2024, 09:05
  5. Huan-Yu Bi (Peking University)
    20/12/2024, 09:30
  6. Jeffrey Davis Raymond(remote)
    20/12/2024, 09:50
  7. Hongtao Yang (USTC)
    20/12/2024, 10:40
  8. Xu-Xiang Li (U. Utah)
    20/12/2024, 11:05
  9. Fangyi Guo
    20/12/2024, 11:25
  10. Qiuping Shen
    20/12/2024, 11:45
  11. Zhijun Liang
    20/12/2024, 14:00
  12. Wei Su (SYSU)
    20/12/2024, 14:25
  13. 刘康 (TDLI/SJTU)
    20/12/2024, 14:45
  14. Zi-Qiang Chen (Guangzhou U.)
    20/12/2024, 15:10
  15. Tahir Javaid
    20/12/2024, 16:05
  16. Yang Zhang (USTC)
    20/12/2024, 16:25
  17. Yanhui Ma
    20/12/2024, 16:45
  18. Xiao-Feng Wang (USTC)
    20/12/2024, 17:05
  19. 曹庆宏
    20/12/2024, 19:00
  20. Li-Lin Yang (Zhejiang University)
    21/12/2024, 08:30
  21. 立诚 章
    21/12/2024, 08:55
  22. Jian Wang (Shandong University)
    21/12/2024, 09:15
  23. Chengjun Yu (USTC)
    21/12/2024, 09:35
  24. Hao Zhang (Remote) (IHEP)
    21/12/2024, 10:30
  25. Sijing Zhang (Laboratoire des deux Infinis – Toulouse)
    21/12/2024, 10:55
  26. Hao-Lin Li (UC Louven)
    21/12/2024, 11:15
  27. Chu Wang (IHEP)
    21/12/2024, 11:40
  28. Yanping Huang (IHEP)
    21/12/2024, 14:00
  29. Ling-Xiao Xu (ICTP, Triest)
    21/12/2024, 14:25
  30. 王震 (USTC/TDLI-SJTU)
    21/12/2024, 14:45
  31. Wenxing Zhang (Hebei University)
    21/12/2024, 15:05
  32. 周辰
    21/12/2024, 15:55
  33. Shao-Jiang Wang (ITP)
    21/12/2024, 16:20
  34. Liangliang Han (Nanjing University)
    21/12/2024, 16:40
  35. Zhe Li (Shandong University)
    21/12/2024, 17:00
  36. Congqiao Li (Peking University)
    21/12/2024, 17:15
  37. Hengkui Wu
    21/12/2024, 17:40
  38. 王子瑞 (University of Michigan)
    22/12/2024, 08:30
  39. 蔡岳霖 (紫金山天文台)
    22/12/2024, 08:55
  40. Jing Chen (上海交通大学)
    22/12/2024, 09:20
  41. 周也铃 (杭州高研院)
    22/12/2024, 09:40
  42. Yikun Wang(remote) (Johns Hopkins University)
    22/12/2024, 10:35
  43. yizhou cai (Nanjing University)
    22/12/2024, 11:00
  44. 郭怀珂 (University of CAS)
    22/12/2024, 11:20
  45. 刘齐斌 (TDLI/SJTU)
    22/12/2024, 11:45
  46. 王志伟 (电子科技大学)
    22/12/2024, 12:05
  47. 杨天一 (北京大学)
    22/12/2024, 14:00
  48. 张阳
    22/12/2024, 14:25
  49. 黄发朋
    22/12/2024, 14:50
  50. 张永超
    22/12/2024, 15:15
  51. Antonio De Maria(remote)
    22/12/2024, 16:10
  52. Ning Chen
    22/12/2024, 16:35
  53. 李家琳 (SJTU)
    22/12/2024, 16:55
  54. Cheng Li
    22/12/2024, 17:15
  55. Shuxiang Li
    22/12/2024, 17:30
  56. Lailin Xu (USTC), Nan Lu (University of Science and Technology of China)
    22/12/2024, 17:45
  57. Yanqi Wang
  58. Yanqi Wang
  59. 王延祺
  60. ning chen (Nankai University)

    Three-generational SM quark/lepton masses are known to be hierarchical, and the latest LHC measurements of the SM Higgs boson Yukawa couplings match well with the SM prediction. We propose a unified SU(8) framework, which can non-trivially and minimally embed three-generational SM fermions. There is only one unique SM Higgs doublet according to the origin of the non-anomalous B-L symmetry....

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  61. Yanping Huang (IHEP)
  62. Liangliang Han (Nanjing University)
  63. Sijing Zhang (Laboratoire des deux Infinis – Toulouse)
  64. Congqiao Li (Peking University)
  65. Chengjun Yu
  66. Chu Wang (IHEP)
  67. 东东 魏 (中山大学)

    In the traditional view, a cosmic first-order phase transition cannot occur without the nucleation of a few bubbles within the entire Hubble volume. However, the presence of domain walls during the transition can significantly alter the dynamics of the process. Using lattice simulations, we demonstrate that thermal fluctuations can destabilize domain walls, which then transform into domain...

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  68. 东东 魏 (中山大学)
  69. Shuxiang Li (USTC)

    We investigate the discovery prospect of doubly-charged Higgs boson at future electron collider Compact Linear Collider (CLIC). After neutrino mass generation through the Type II seesaw mechanism, we examine the small vacuum expectation value (VEV) parameter region of the type-II seesaw model in four different collision modes. In this region, $\mathcal{O}(1)$ Yukawa couplings between Higgs...

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  70. Yongcheng Wu (Nanjing Normal U.)
  71. Prof. Jiayin Gu (Fudan University)
  72. 健 王 (山东大学)

    The precise determination of the Higgs boson self-couplings is essential for understanding the mechanism behind electroweak symmetry breaking. However, due to the limited number of Higgs boson pair events at the LHC, only loose constraints have been established so far.
    Current constraints are based on the assumption that the cross section is a quadratic function of the trilinear Higgs...

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  73. Chen Zhou
  74. Dr Zhe Li (Shandong University)

    After the discovery of the Higgs boson at LHC in 2012, the precision test of the SM and search for new physics beyond the SM have become two most important research areas in the field of high-energy particle physics. This presentation focuses on these two areas, providing an in-depth investigation of the NNLO mixed QCD-EW corrections to the production of the SM gauge boson pair and THDM...

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  75. Zhuoni Qian (Hangzhou Normal U.)
  76. Shao-Jiang Wang (中国科学院理论物理研究所Institute of Theoretical Physics, Chinese Academy of Sciences)

    The future space-borne gravitational wave (GW) detectors would provide a promising probe for the new physics beyond the standard model that admits the first-order phase transitions. The predictions for the GW background vary sensitively among different concrete particle physics models but also share a large degeneracy in the model buildings, which motivates an effective model description on...

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  77. Qibin Liu (Tsung-Dao Lee Institute, Shanghai Jiao Tong Univ. (CN))

    Ref. https://arxiv.org/abs/2406.01656
    JHEP 08 (2024) 153
    A combination of searches for Higgs boson decaying into a visible photon and a massless dark photon (H→γγ$_𝑑$) is presented using 139 fb$^{−1}$ of proton--proton collision data at a centre-of-mass energy of √s = 13 TeV recorded by the ATLAS detector at the Large Hadron Collider. The observed (expected) 95% confidence level upper limit...

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  78. 立诚 章 (University of Maryland)

    This study presents a search for a vector boson $V$ ($W$ or $Z$ boson) associated Higgs boson pair ($HH$) production process using proton-proton ($pp$) collision data at a center-of-mass energy of 13 TeV, collected by the CMS detector at the LHC, corresponding to an integrated luminosity of 138 fb$^{-1}$. The processes include $pp \rightarrow ZHH$ and $pp \rightarrow WHH$ production,...

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  79. Zhen Wang (University of Science and Technology of China (CN))

    Ref. Phys. Lett. B 858 (2024) 139007
    A search for Higgs boson pair production via vector-boson fusion is performed in the Lorentz-boosted regime, where a Higgs boson candidate is reconstructed as a single large-radius jet, using 140 fb−1 of proton-proton collision data at √s = 13 TeV recorded by the ATLAS detector at the Large Hadron Collider. Only Higgs boson decays into bottom quark pairs...

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  80. Dr Jing Chen (SJTU/TDLI)

    Ref. ATLAS-HIGP-2024-32
    A search for production of three Higgs bosons (HHH) in the 6b final state is presented. The search uses 126 fb−1 of pp collision data at √s = 13 TeV collected with the ATLAS detector at the Large Hadron Collider. The analysis targets both non-resonant and resonant production of HHH. The resonant interpretations primarily consider a cascade decay topology of X→SH→HHH...

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  81. Dr Xu-Xiang Li (U. Utah)
  82. Dr Huan-Yu Bi (Peking University)
  83. Prof. Zi-Qiang Chen (Guangzhou U.)
  84. Prof. Li-Lin Yang (Zhejiang University)
  85. Cheng Li (Sun Yat-sen University)

    The 2HDM+S is the singlet extension of Two-Higgs-Doublets Model (2HDM), where the additional singlet-like particles can accommodate more physics potential beyond the Standard Model (SM), e.g. the dark matter candidate, as well as match to the Higgs sector of Next-to Mnimal-supersymmetric Standard model (NMSSM). The BSM extension of the Higgs sector can contribute the self-energy of $W^\pm$ and...

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  86. Xiao-Feng Wang (USTC)

    We compute the two-loop master integrals in $ d = 4 - 2\epsilon $ spacetime dimensions using the differential equation method, specifically for QCD-EW corrections to the $ WWV $ ($ V = H, Z, \gamma $) vertex. This analysis includes integral families that incorporate massive $ t/b $ quarks within the quark loops, with the master integrals constructing to a canonical differential system....

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