Strongly-interacting massive particle and dark photon in the era of the intensity frontier

被引:0
作者
Kamada, Ayuki [1 ]
Yamada, Masaki [2 ,3 ,4 ,5 ]
Yanagida, Tsutomu T. [6 ,7 ,8 ]
机构
[1] Inst Basic Sci IBS, Ctr Theoret Phys Universe, 55 Expo Ro, Daejeon 34126, South Korea
[2] Tohoku Univ, Frontier Res Inst Interdisciplinary Sci, Sendai, Miyagi 9808578, Japan
[3] Tohoku Univ, Dept Phys, Sendai, Miyagi 9808578, Japan
[4] MIT, Ctr Theoret Phys, Nucl Sci Lab, Cambridge, MA 02139 USA
[5] MIT, Dept Phys, Cambridge, MA 02139 USA
[6] Shanghai Jiao Tong Univ, TD Lee Inst, 800 Dongchuan Rd, Shanghai 200240, Peoples R China
[7] Shanghai Jiao Tong Univ, Sch Phys & Astron, 800 Dongchuan Rd, Shanghai 200240, Peoples R China
[8] Univ Tokyo, Kavli IPMU WPI, UTIAS, 5-1-5 Kashiwanoha, Kashiwa, Chiba 2778583, Japan
关键词
INTERACTION CROSS-SECTION; MATTER SELF-INTERACTIONS; QUANTUM-FIELD THEORY; COSMOLOGICAL SIMULATIONS; CONSTRAINTS; MONOPOLES; DUALITY; MILKY;
D O I
10.1103/PhysRevD.102.075001
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
A strongly interacting massive particle (SIMP) is an interesting candidate for dark matter (DM) because its self-interaction cross section can be naturally strong enough to address the astrophysical problem of small-scale structure formation. A simple model was proposed by assuming a monopole condensation, where composite SIMP comes from a "strongly interacting" U(1)(d) gauge theory. In the original model, the DM relic abundance is determined by the 3 -> 2 annihilation process via the Wess-Zumino-Witten term. In this paper, we discuss that the DM relic abundance is naturally determined also by a semiannihilation process via a kinetic mixing between the hypercharge gauge boson and the dark U(1)(d) gauge boson (dark photon). The dark photon can be discovered by LDMX-style missing momentum experiments in the near future.
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页数:8
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