Physics Letters B 770 (2017) 335–341
Contents lists available at ScienceDirect
Physics Letters B
www.elsevier.com/locate/physletb
Measuring CP nature of top-Higgs couplings at the future
Large Hadron electron Collider
Baradhwaj Coleppa
a
, Mukesh Kumar
b,∗
, Satendra Kumar
a
, Bruce Mellado
c
a
Department of Physics, Indian Institute of Technology Gandhinagar, Gandhinagar 382 355, India
b
National Institute for Theoretical Physics, School of Physics and Mandelstam Institute for Theoretical Physics, University of the Witwatersrand, Johannesburg,
Wits 2050, South Africa
c
University of the Witwatersrand, School of Physics, Private Bag 3, Wits 2050, South Africa
a r t i c l e i n f o a b s t r a c t
Article history:
Received
25 February 2017
Received
in revised form 27 April 2017
Accepted
1 May 2017
Available
online 4 May 2017
Editor:
G.F. Giudice
Keywords:
Electron–proton
collision
Top-Higgs
coupling
Top
polarisation
We investigate the sensitivity of top-Higgs coupling by considering the associated vertex as CP phase
(ζ
t
) dependent through the process p e
−
→
¯
th ν
e
in the future Large Hadron electron Collider. In par-
ticular
the decay modes are taken to be h → b
¯
b and
¯
t → leptonic mode. Several distinct ζ
t
dependent
features are demonstrated by considering observables like cross sections, top-quark polarisation, rapidity
difference between h and
¯
t and different angular asymmetries. Luminosity (L) dependent exclusion limits
are obtained for ζ
t
by considering significance based on fiducial cross sections at different σ -levels. For
electron and proton beam-energies of 60 GeV and 7TeV respectively, at L = 100 fb
−1
, the regions above
π/5 <ζ
t
≤ π are excluded at 2σ confidence level, which reflects better sensitivity expected at the Large
Hadron Collider. With appropriate error fitting methodology we find that the accuracy of SM top-Higgs
coupling could be measured to be κ = 1.00 ±0.17(0.08) at
√
s = 1.3(1.8) TeV for an ultimate L = 1 ab
−1
.
© 2017 The Author(s). 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 recent discovery of the Higgs boson at the Large Hadron
Collider (LHC) serves as the last step in establishing the particle
content of the Standard Model (SM). The next step that has been
undertaken is the characterisation of its properties regarding spin,
CP-nature and the nature of interaction with other particles. While
the spin-0 nature of the Higgs boson has been established by the
experiments [1–5] and a complete CP-odd nature excluded at a
99.98% confidence limit (C.L.) [6,7], the possibility remains that the
Higgs boson could still be an admixture of CP-odd and even states.
Investigation of this possibility in a future Large Hadron electron
Collider (LHeC) is the goal of this article via a detailed analysis
of the associated production of the Higgs boson with an anti-top
quark.
Since
in the SM the Higgs boson coupling to fermions is directly
proportional to the mass of the fermions, the Yukawa coupling as-
sociated
with the third generation is important in the context of
*
Corresponding author.
E-mail
addresses: baradhwaj@iitgn.ac.in (B. Coleppa), mukesh.kumar@cern.ch
(M. Kumar),
satendrak@iitgn.ac.in (S. Kumar), bruce.mellado@wits.ac.za
(B. Mellado).
investigating the properties of the Higgs boson. Deviations in the
top-Higgs coupling directly affect the production cross section of
Higgs boson at the colliders, while changes in the bottom-Higgs
coupling affect the total branching ratios.
Here we study the associated production of the Higgs boson
with an anti-top quark at the future e
−
p collider which employs a
7TeV proton beam from a circular pp collider, and electrons from
an Energy Recovery Linac (ERL) being developed for the LHeC [8,9].
The choice of an ERL energy of electron of E
e
= 60 to 120 GeV,
with available proton beam energy E
p
= 7TeV provides centre
of mass energy of
√
s ≈ 1.3to1.8TeV. While the LHC is clearly
energetically superior, the LHeC configuration is advantageous for
the following reasons: (i) since initial states are asymmetric, back-
ward
and forward scattering can be disentangled, (ii) it provides
a clean environment with suppressed backgrounds from strong
interaction processes and free from issues like pile-ups, multiple
interactions etc. (iii) such machines are known for high precision
measurements of the dynamical properties of the proton allowing
simultaneous tests of electroweak and QCD effects. A detailed re-
port
on the physics and detector design concepts of the LHeC can
be found in the Ref. [8]. A distinguishing feature of the e
−
p col-
lider
is that the production of the Higgs is only due to electroweak
processes [10,11] and as noted above, since the e
−
and p energies
are different, the machine can also produce interesting patterns of
http://dx.doi.org/10.1016/j.physletb.2017.05.006
0370-2693/
© 2017 The Author(s). 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
.