In the Littlest Higgs model with $T$ parity (LHT), the $T$-odd heavy photon ($A_H$) is weakly interacting and can play the role of dark matter. We investigate the lower limit on the mass of $A_H$ dark matter under the constraints from Higgs data, EWPOs, $R_b$, Planck 2015 dark matter relic abundance, PandaX-II/LUX 2016 direct detections and LHC-8 TeV monojet results. We find that (1) Higgs data, EWPOs and $R_b$ can exclude the mass of $A_H$ up to 99 GeV. To produce the correct dark matter relic abundance, $A_H$ has to co-annihilate with $T$-odd quarks ($q_H$) or leptons ($\ell_H$); (2) the LUX (PandaX-II) 2016 data can further exclude $m_{A_H}<380 (270)$ GeV for $\ell_H$-$A_H$ co-annihilation and $m_{A_H}<350 (240)$ GeV for $q_H-A_H$ co-annihilation; (3) LHC-8 TeV monojet result can give a strong lower limit, $m_{A_H}>540$ GeV, for $q_H$-$A_H$ co-annihilation; (4) future XENON1T (2017) experiment can fully cover the parameter space of $\ell_H$-$A_H$ co-annihilation and will push the lower limit of $m_{A_H}$ up to about 640 GeV for $q_H$-$A_H$ co-annihilation.
Probing the MSSM explanation of the muon g-2 anomaly in dark matter experiments and at a 100 TeV $pp$ collider
我们探讨了当前和未来的暗物质和对撞机实验的能力，在探测异常磁矩的μ子，$(g-2)_μ$，在最小超对称标准模型（MSSM）。我们发现，最新的PandaX-II/LUX-2016数据对参数空间提供了强约束，使$(g-2)_μ$在$2σ$范围内，这将被即将到来的XENON-1 T（2017）实验进一步排除。我们还发现，100 TeV的$pp$对撞机可以覆盖我们的大多数幸存的样品，满足DM遗迹密度在$3σ$范围内通过$Z$或$h$共振效应，通过搜索从$\tildeχ^0_2\tildeχ^+_1$相关的产品的三轻子事件。而在100 TeV $pp$对撞机和DM直接探测中超出未来三轻子搜索灵敏度的样品要么是类higgsino/wino LSP，要么是与slepton共湮灭的类bino LSP。这样的压缩区域可以由在100 TeV $pp$对撞机上的单喷射（类）搜索覆盖。
Two experiments from the Fermilab, E989 and CDF II, have reported two anomalies for muon $g-2$ and $W$-boson mass that may indicate the new physics at the low energy scale. Here we examine the possibility of a common origin of these two anomalies in the Next-to-Minimal Supersymmetric Standard Model. Considering various experimental and astrophysical constraints such as the Higgs mass, collider data, flavor physics, dark matter relic density, and direct detection experiments, we find that lighter electroweakinos and sleptons can generate sufficient contributions to muon $g-2$ and $m_W$. Moreove…
We propose the family universal $U(1)_X$ models with three right-handed neutrinos by choosing the $U(1)_X$ gauge symmetry as a linear combination of $U(1)_Y\times U(1)_χ$ of $SO(10)$. To be consistent with the quantum gravity effects, we introduced a Dirac fermion $χ$ as a dark matter candidate, which is odd under the gauged $Z_2$ symmetry after $U(1)_X$ breaking. The isospin violation dark matter with $f_n/f_p = -0.7$ can be realized naturally, and thus the LUX, PANDAX, and XENON1T experimental constraints can be evaded. Moreover, we study the masses and mixings for Higgs and gauge bosons, co…
Testing light and heavy vector mediators with solar CE$ν$NS measurements
Instituto de Física Corpuscular (IFIC), CSIC‐Universitat de Valéncia（粒子物理研究所（IFIC），西班牙科学委员会-瓦伦西亚大学）；University of Hamburg（汉堡大学）；Istituto Nazionale di Fisica Nucleare (INFN), Laboratori Nazionali del Gran Sasso（意大利国家核物理研究所（INFN），格兰萨索国家实验室）；Universidad Nacional Autónoma de México（墨西哥国立自治大学）；Gran Sasso Science Institute（格兰萨索科学研究所）
The 331 model with right-handed neutrinos is re-assessed to investigate the CP violation in the quark sector. After the spontaneous symmetry breaking, the masses and physical fields of the particle content are obtained. The fermions content of the 331 model is enlarged to include exotic quarks with known electric charge and with masses defined at the TeV scale. The existence of these exotic quarks induces extra CP violations via couplings with quarks of the Standard Model mediated by charged gauge boson with mass fixed at the TeV scale. An extra discrete $\mathbb{Z}_{2}$ symmetry is introduced…
The $Z_3$-invariant next-to-minimal supersymmetric standard model (NMSSM) can provide a candidate for dark matter (DM). It can also be used to explain the hypothesis that the Higgs signal observed on the Large Hadron Collider (LHC) comes from the contribution of the two lightest CP-even Higgs bosons, whose masses are near 125 GeV. At present, XENON1T, LUX, and PandaX experiments have imposed very strict restrictions on direct collision cross sections of {dark matter}. In this paper, we consider a scenario that the observed Higgs signal is the superposition of two mass-degenerate Higgs in the $…
We explore the prospects for direct detection of dark energy by current and upcoming terrestrial dark matter direct detection experiments. If dark energy is driven by a new light degree of freedom coupled to matter and photons then dark energy quanta are predicted to be produced in the Sun. These quanta free-stream towards Earth where they can interact with Standard Model particles in the detection chambers of direct detection experiments, presenting the possibility that these experiments could be used to test dark energy. Screening mechanisms, which suppress fifth forces associated with new l…
Invisible decay of solar neutrinos at dark matter experiments
Gran Sasso Science Institute（格兰萨索科学研究所）；Istituto Nazionale di Fisica Nucleare (INFN), Laboratori Nazionali del Gran Sasso（意大利国家核物理研究所（INFN），格兰萨索国家实验室）；Instituto de Física Corpuscular (IFIC), CSIC‐Universitat de Valéncia（粒子物理研究所（IFIC），CSIC-巴伦西亚大学）；Institute of Experimental Physics, University of Hamburg（汉堡大学实验物理研究所）
Projected Sensitivity of Paleo-Detectors to Dark Matter Effective Interactions with Nuclei
The University of Texas at Austin（德克萨斯大学奥斯汀分校）；Stockholm University（斯德哥尔摩大学）；KTH Royal Institute of Technology（皇家理工学院）；University of North Florida（北佛罗里达大学）；Jožef Stefan Institute（约瑟夫·斯蒂芬研究所）
The observed Higgs mass indicates that the Standard Model can be valid up to near the Planck scale $M_\text{P}$. Within this framework, it is important to examine how little modification is necessary to fit the recent experimental results in particle physics and cosmology. As a minimal extension, we consider the possibility that the Higgs field plays the role of inflaton and that the dark matter is the Higgs-portal scalar field. We assume that the extended Standard Model is valid up to the string scale $10^{17}\,\text{GeV}$. (This translates to the assumption that all the non-minimal couplings…
