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我们使用有效场论框架考虑了希格斯玻色子异常FCNC与u,c,d,s和b夸克的相互作用。 异常耦合的约束来自希格斯玻色子产生的实验结果,随后在s = 13 TeV的LHC下衰减成bb对。 通过执行逼真的检测器模拟并在s = 13 TeV的四轻子最终状态下准确再现CMS希格斯玻色子测量的分析选择,可以设置H→bs和H→bd的分支分数的上限。 搜索被预测为HL-LHC的运行条件。 基于具有H→γγ衰变通道的希格斯玻色子产生,研究了FCC-hh对FCNC异常相互作用的敏感性。 结果表明,在FCC-hh机上,可以期望将B(H→bs)和B(H→bd)的10-2的上限设置为95%CL。
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Available online at www.sciencedirect.com
ScienceDirect
Nuclear Physics B 952 (2020) 114921
www.elsevier.com/locate/nuclphysb
Constraints on the Higgs boson anomalous FCNC
interactions with light quarks
M. Ilyushin
a
, P. Mandrik
a,b,∗
, S. Slabospitskii
a,b
a
NRC “Kurchatov Institute” -IHEP, Protvino, Moscow Region, Russia
b
Moscow Institute of Physics and Technology, Dolgoprudny, Moscow Region, Russia
Received 13
May 2019; received in revised form 27 November 2019; accepted 6 January 2020
Available
online 9 January 2020
Editor: Hong-Jian
He
Abstract
We consider the Higgs boson anomalous FCNC interactions with u, c, d, s and b quarks using the
effective field theory framework. Constraints on anomalous couplings are derived from experimental results
on Higgs boson production with subsequent decay into b
¯
b pair at LHC with
√
s = 13 TeV. Upper limits
on the branching fractions of H → b¯s and H → b
¯
d are set by performing a realistic detector simulation
and accurately reproducing analysis selections of the CMS Higgs boson measurement in the four-lepton
final state at
√
s = 13 TeV. The searches are projected into operation conditions of HL-LHC. Sensitivity at
FCC-hh to anomalous FCNC interactions is studied based on Higgs boson production with H → γγ decay
channel. It is shown that at FCC-hh machine one can expect to set the upper limits of the order of 10
−2
at
95% CL for B(H →b¯s) and B(H → b
¯
d).
© 2020 The Authors. Published by Elsevier B.V. This is an open access article under the CC BY license
(http://creativecommons.org/licenses/by/4.0/). Funded by SCOAP
3
.
1. Introduction
The discovery of Higgs boson by the Large Hadron Collider (LHC) [1,2] experiments has
opened up new area of direct searches for physics Beyond Standard Model (BSM). One of the
possible anomalous interaction is the Higgs-mediated flavor-changing neutral currents (FCNC).
These processes are forbidden in Standard Model (SM) at tree le
vel and are strongly suppressed
in loop corrections by the Glashow-Iliopoulos-Maiani mechanism [3].
*
Corresponding author.
E-mail
address: petr.mandrik@ihep.ru (P. Mandrik).
https://doi.org/10.1016/j.nuclphysb.2020.114921
0550-3213/© 2020
The Authors. Published by Elsevier B.V. This is an open access article under the CC BY license
(http://creativecommons.org/licenses/by/4.0/). Funded by SCOAP
3
.
2 M. Ilyushin et al. / Nuclear Physics B 952 (2020) 114921
Table 1
The
current experimental upper limits on FCNC decays of top-quark at 95% CL.
Detector B(t →uH ) B(t →cH ) Ref.
ATLAS, 13 TeV, 36.1 fb
−1
1.2 ×10
−3
1.1 ×10
−3
[7]
CMS, 13 TeV, 35.9 fb
−1
4.7 ×10
−3
4.7 ×10
−3
[9]
Table 2
The
upper limits on FCNC decays of Higgs boson to the
light quarks at 95% CL from experiments with mesons
(see [10]for details).
Observable Constraint
D
0
oscillations B(H → u ¯c) 2 ×10
−5
B
0
d
oscillations B(H → d
¯
b) 8 ×10
−5
K
0
oscillations B(H → d ¯s) 2 × 10
−6
B
0
s
oscillations B(H → s
¯
b) 7 ×10
−3
The Higgs mediated FCNC in top-quark sector is actively investigated at LHC [4–9]. The
main analyses strategy is to search for t
¯
t production with one top quark decay through a FCNC
channel and other follow the dominant SM decay t → bW . In [9] production of single top quark
through a FCNC in association with the Higgs boson is considered in additional. The results of
the searches are summarized in T
able 1.
The FCNC couplings of the Higgs to the rest SM quarks can af
fect various low-energy preci-
sion measurements. The strongest indirect bounds on FCNC quark-quark-Higgs couplings came
from measurement of B
d,s
−
¯
B
d,s
, K
0
−
¯
K
0
and D
0
−
¯
D
0
oscillations [10]. The corresponding
constraints on FCNC couplings translated into upper limits on branching fractions of the FCNC
decays of Higgs boson to u, d, s, c, b quarks are summarized in the Table 2. Due to huge QCD
background the experiments at LHC are less sensitive to searching for FCNC decays of the Higgs
boson. On the other hand the direct probes of such processes could complement the indirect lim-
its. In addition in possible BSM scenarios the branching ratio of H → qq
can be enhanced with
keeping other low-energy flavor observables approximately at their SM values [11,12]. Therefor,
the searches for FCNC Higgs boson interactions are very important and could be considered as
a complementary probe of new physics.
At the moment there is no an
y experimental evidence of the FCNC process. Future research
and increase of the experimental sensitivity are related to the proposed energy-frontier colliders
[13–16] such as High Luminosity LHC (HL-LHC) [17] and Future Circular Collider (FCC-hh)
project, defined by the target of 100 TeV proton-proton collisions with a total inte
grated lumi-
nosity of 30 ab
−1
[18,19].
In this article we in
vested the contribution of FCNC interactions to the single Higgs boson
production (Fig. 1, left) and Higgs boson production in association with a light quark (Fig. 1,
center and right). The limits on Higgs boson FCNC interactions based on recent LHC data are
obtained and the searches are projected into operation conditions of HL-LHC [17]
and FCC-hh
projects.
2. The constraints from the current Higgs production cross-sections
The flavor-violating couplings may arise from different sources [20]. In this article we use the
effective field theory approach (EFT) [21–23]for describing the effects of BSM physics in Higgs
M. Ilyushin et al. / Nuclear Physics B 952 (2020) 114921 3
Fig. 1. Example of diagrams for Higgs boson production (left) and Higgs boson associated production with quark (center
and right) mediated by FCNC couplings.
interactions. The effective Lagrangian (up to dimension-six gauge-invariant effective operators)
has the form as follows [24,25]:
L
BSM
=−
1
√
2
¯q(κ
L
qq
H
P
L
+κ
R
qq
H
P
R
)q
H (1)
where P
L,R
=
1
2
(1 ±γ
5
), q, q
∈ (u, c, t) or q, q
∈ (d, s, b). The couplings κ
L
qq
H
and κ
R
qq
H
are
complex in general.
Note, that in our analysis these couplings are appeared in the combination
|κ
L
qq
|
2
+|κ
R
qq
|
2
= (Re κ
L
qq
)
2
+(Im κ
L
qq
)
2
+(Re κ
R
qq
)
2
+(Im κ
R
qq
)
2
Thus, in what follows we set
κ ≡|κ
L
qq
|=|κ
R
qq
|
λ ≡|Re κ
L
qq
|=|Im κ
L
qq
|=|Re κ
R
qq
|=|Im κ
R
qq
|
→ κ =
√
2λ
⎫
⎪
⎬
⎪
⎭
(2)
The Higgs decays width resulted from (1) equals:
(H → q ¯q
) =
3(|κ
L
qq
|
2
+|κ
R
qq
|
2
)M
H
32π
=
6|λ
qq
|
2
M
H
16π
=|λ
qq
|
2
×14.92 GeV (3)
The very rough estimate of the coupling λ
qq
(actually in order of magnitude) could be obtained
from the measurement of the Higgs boson total decay width. The CMS collaboration presents
the constraint of on the Higgs boson total width [26]:
H
= 3.2
+2.8
−2.2
MeV @ 68% CL (4)
H
=[0.08 ÷9.16] MeV @ 95% CL (5)
We use the value of 9.16 MeV from (5)as an upper limit on
H
. Then one gets:
SM
H
+2(H → q ¯q
) ≤ 9.16 MeV,
SM
H
= 4.1MeV
⇒|λ
qq
|≤0.013 (6)
The more realistic estimates of the coupling λ
qq
could be obtained from the Higgs production
in the pp-collisions at LHC [27,28]:
pp → HX, pp → HW/ZX, H→ b
¯
b (7)
We use the experimental results from ATLAS and CMS collaborations:
μ
b
=
σ
exp
(pp → HX,H→ b
¯
b)
σ
theor
(pp → HX,H→ b
¯
b)
(8)
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