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我们讨论了超对称希格斯轻子膨胀模型和BICEP2实验最近的CMB B模式观测所产生的物理学。 CMB B模式极化表示的原始波动的张量与标量比r =0.20â0.05+0.07与该膨胀模型对自然参数值的预测一致。 该模型的一个显着特征是,它根据张量模式波动的幅度预测了跷跷板的质量比例M。 从BICEP2实验发现68%(95%)的置信度(CL)约束为50个电子折叠和391GeV <M给出927 GeV <M <1.62 TeV(751 GeV <M <2.37 TeV) <795 GeV(355 GeV <M <1.10 TeV)60个电子折叠。 在I型跷跷板上,由于混合角小,在这种质量范围内的右旋中微子在对撞机实验中难以捉摸。 相比之下,在III型跷跷板中,重的轻子将在未来的实验范围之内。 我们指出,对应于BICEP2实验的68%CL的参数区域的很大一部分将被14 TeV的大型强子对撞机实验覆盖。
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Physics Letters B 735 (2014) 186–190
Contents lists available at ScienceDirect
Physics Letters B
www.elsevier.com/locate/physletb
TeV scale seesaw from supersymmetric Higgs-lepton inflation
and BICEP2
Shinsuke Kawai
a,∗
, Nobuchika Okada
b
a
Department of Physics, Sungkyunkwan University, Suwon 440-746, Republic of Korea
b
Department of Physics and Astronomy, University of Alabama, Tuscaloosa, AL 35487, USA
a r t i c l e i n f o a b s t r a c t
Article history:
Received
16 May 2014
Accepted
13 June 2014
Available
online 18 June 2014
Editor:
J. Hisano
Keywords:
Supergravity
Right-handed
neutrinos
Inflation
Cosmic
microwave background
We discuss the physics resulting from the supersymmetric Higgs-lepton inflation model and the recent
CMB B-mode observation by the BICEP2 experiment. The tensor-to-scalar ratio r = 0.20
+0.07
−0.05
of the
primordial fluctuations indicated by the CMB B-mode polarization is consistent with the prediction of
this inflationary model for natural parameter values. A salient feature of the model is that it predicts
the seesaw mass scale M from the amplitude of the tensor mode fluctuations. It is found that the
68% (95%) confidence level (CL) constraints from the BICEP2 experiment give 927 GeV < M < 1.62 TeV
(751 GeV
< M < 2.37 TeV) for 50 e-foldings and 391 GeV < M < 795 GeV (355 GeV < M < 1.10 TeV)
for 60 e-foldings. In the type I seesaw case, the right-handed neutrinos in this mass range are elusive
in collider experiments due to the small mixing angle. In the type III seesaw, in contrast, the heavy
leptons will be within the reach of future experiments. We point out that a significant portion of the
parameter region corresponding to the 68% CL of the BICEP2 experiment will be covered by the Large
Hadron Collider experiments at 14 TeV.
© 2014 The Authors. Published by Elsevier B.V. This is an open access article under the CC BY license
(http://creativecommons.org/licenses/by/3.0/). Funded by SCOAP
3
.
1. Introduction
The discovery of the cosmic microwave background (CMB)
B-mode polarization by the BICEP2 experiment [1] is truly re-
markable
as the existence of the tensor mode in the primordial
fluctuations provides a direct evidence for inflation in the early
Universe.
1
It has a significant impact on inflation model building.
In the past decade models producing small tensor mode fluctu-
ations
were considered favourable since, for example, the Planck
data in 2013 [2] constrained the tensor-to-scalar ratio r < 0.11 at
95% confidence level (CL). The models of inflation producing such
small r include the Higgs inflation model [3,4], supersymmetric
Higgs inflation-type models [5–9], the hill-top inflation model [10],
and the R
2
inflation model [11]. Among these, the Higgs inflation
model is a particularly simple and concrete particle physics real-
ization
of inflation that also provides predictions in low-energy
particle physics. These models are in tension with the finding of
*
Corresponding author.
E-mail
addresses: kawai@skku.edu (S. Kawai), okadan@ua.edu (N. Okada).
1
The BICEP2 experiment uses 150 GHz single wavelength bolometers. In order
to conclude that the gravitational waves causing the polarization are undeniably of
inflationary origin, the results need to be confirmed also at other wavelengths.
the BICEP2 experiment. See Refs. [12–14] for the updated status of
various models.
In
the present paper we point out that the prediction of the in-
flationary
scenario which we call the Higgs-lepton inflation (HLI)
[15,16] fits extremely well with the new data for natural choice
of parameters. The HLI scenario is realized in the supersymmetric
seesaw model, which is the simplest extension of the minimal su-
persymmetric
Standard Model (MSSM) to include the right-handed
neutrinos. The model incorporates the type I [17] or type III see-
saw
mechanism [18] by which the small nonzero neutrino masses
that are evidenced by the neutrino oscillations are naturally ex-
plained.
It also includes possibility for generating baryon asym-
metry
through leptogenesis or the Affleck–Dine mechanism. As a
feature of the model, HLI directly associates the spectrum of the
CMB with the mass scale of the right-handed neutrinos. We will
see that the new data from the BICEP2 experiments constrains this
mass scale to be between a few hundred GeV and a few TeV. These
constraints are potentially useful since the right-handed (s)neutri-
nos
may also be searched in colliders.
2. Higgs-lepton inflation in the supersymmetric seesaw model
The HLI model [15,16] is an “all-in” phenomenological model
of inflation that includes the seesaw mechanism [17], the origin of
the baryon asymmetry, the origin of the dark matter, as well as
http://dx.doi.org/10.1016/j.physletb.2014.06.042
0370-2693/
© 2014 The Authors. Published by Elsevier B.V. This is an open access article under the CC BY license (http://creativecommons.org/licenses/by/3.0/). Funded by
SCOAP
3
.
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