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Search for dark photons from neutral meson decays in $$p+p$$ and $$d$$+Au collisions at $$sqrt{s_{NN}} = 200$$ GeV

$$sqrt{s_{NN}}$$=200GeVの陽子-陽子および重陽子-金衝突における中性中間子崩壊からのダークフォトン探索

Adare, A.*; 長谷川 勝一   ; 今井 憲一; 佐甲 博之   ; 佐藤 進  ; 谷田 聖   ; PHENIX Collaboration*; 他574名*

Adare, A.*; Hasegawa, Shoichi; Imai, Kenichi; Sako, Hiroyuki; Sato, Susumu; Tanida, Kiyoshi; PHENIX Collaboration*; 574 of others*

The standard model (SM) of particle physics is spectacularly successful, yet the measured value of the muon anomalous magnetic moment $$(g-2)_{mu}$$ deviates from SM calculations by $$3.6sigma$$. Several theoretical models attribute this to the existence of a "dark photon", an additional $$U(1)$$ gauge boson, which is weakly coupled to ordinary photons. The PHENIX experiment at the Relativistic Heavy Ion Collider has searched for a dark photon, $$U$$, in $$pi^0,;eta to gamma e^+e^-$$ decays and obtained upper limits of O(2$$times 10^{-6})$$ on $$U$$-$$gamma$$ mixing at 90% C.L. for the mass range $$30 < m_U < 90 {rm MeV}/c^2$$. Combined with other experimental limits, the remaining region in the $$U$$-$$gamma$$ mixing parameter space that can explain the $$(g-2)_{mu}$$ deviation from its SM value is nearly completely excluded at the 90% confidence level, with only a small region of $$29 < m_U < 32 {rm MeV}/c^2$$ remaining.

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パーセンタイル:92.41

分野:Physics, Nuclear

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