Constraining graviton non-Gaussianity through the CMB bispectra

被引:6
作者
De Luca, Valerio [1 ,2 ]
Franciolini, Gabriele [1 ,2 ]
Kehagias, Alex [3 ]
Riotto, Antonio [1 ,2 ,4 ]
Shiraishi, Maresuke [5 ]
机构
[1] Univ Geneva, Dept phys Theor, 24 Quai Ansermet, CH-1211 Geneva, Switzerland
[2] Univ Geneva, CAP, 24 Quai Ansermet, CH-1211 Geneva, Switzerland
[3] Natl Tech Univ Athens, Phys Div, Zografou Campus, Athens 15780, Greece
[4] CERN, Dept TH, CH-1211 Geneva 23, Switzerland
[5] Kagawa Coll, Natl Inst Technol, Dept Gen Educ, 355 Chokushi Cho, Takamatsu, Kagawa 7618058, Japan
基金
瑞士国家科学基金会;
关键词
MASSLESS FIELDS; EQUATIONS; SPINS;
D O I
10.1103/PhysRevD.100.063535
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Tensor non-Gaussianities are a key ingredient to test the symmetries and the presence of higher spin fields during the inflationary epoch. Indeed, the shape of the three point correlator of the graviton is totally fixed by the symmetries of the de Sitter stage and, in the case of parity conservation, gets contributions only from the ordinary gravity action plus a higher derivative term called the (Weyl)(3) action. We discuss current and future bounds on the three point tensor contribution from the (Weyl)(3) term using cosmic microwave background (CMB) bispectra. Our results indicate that forthcoming experiments, such as LiteBIRD, CMB-S4, and CORE, will detect the presence of the (Weyl)(3) term if (MpL4)-L-4 similar to 10(17)r(-4), where L parametrizes the strength of the (Weyl)(3) term and r is the tensor-to-scalar ratio, which corresponds to L greater than or similar to 3.2 x 10(5)M(p)(-1), while the current upper limit is (MpL4)-L-4 = (1.1 +/- 4.0) x 10(19)r(-4) (68% CL).
引用
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页数:8
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