Abstract:We analyze the LHC prospects for measurements of the tt pair produced exclusively in photon-photon or semiexclusively in photon-Pomeron and Pomeron-Pomeron processes using protons tagged in forward proton detectors on both sides of the interaction point. These processes are interesting from the point of view of a possible measurement of the top quark mass and constraining models used in beyond the Standard Model physics. Focusing on the semileptonic channel, tt → jjblν lb , making use of the exclusive nature o… Show more
“…The predictions of forward proton scattering arise in a diverse range of physics, including the hard [1,2] and nonperturbative QCD [3], interactions at electroweak scale [4][5][6][7], and searches for physics beyond Standard Model [8][9][10][11][12][13]. Such events, usually called diffractive, involve an exchange of a colourless object between interacting protons, one or both of which may remain intact.…”
Section: Studies Of Diffractive Physics With Afpmentioning
The performance of the ATLAS Forward Proton (AFP) Silicon Tracker detector is studied using the dedicated low-luminosity ATLAS LHC data collected in the 2017 running period of LHC Run 2. A brief description of the AFP spectrometer is given, followed by the discussion of unique opportunities of diffractive physics studies in low pile-up conditions. Additionally, some features of 2017 data are explored, including trigger efficiency and creation of particle showers within the detectors.
“…The predictions of forward proton scattering arise in a diverse range of physics, including the hard [1,2] and nonperturbative QCD [3], interactions at electroweak scale [4][5][6][7], and searches for physics beyond Standard Model [8][9][10][11][12][13]. Such events, usually called diffractive, involve an exchange of a colourless object between interacting protons, one or both of which may remain intact.…”
Section: Studies Of Diffractive Physics With Afpmentioning
The performance of the ATLAS Forward Proton (AFP) Silicon Tracker detector is studied using the dedicated low-luminosity ATLAS LHC data collected in the 2017 running period of LHC Run 2. A brief description of the AFP spectrometer is given, followed by the discussion of unique opportunities of diffractive physics studies in low pile-up conditions. Additionally, some features of 2017 data are explored, including trigger efficiency and creation of particle showers within the detectors.
“…An alternative, recently proposed in Ref. [1] (see also Ref. [10]), is the study of top quark production in pp collisions characterized by intact protons in the final state.…”
Section: Introductionmentioning
confidence: 99%
“…In our previous article [1], we have performed the first comprehensive study of the elastic top quark for all luminosity scenarios considered, although a good separation between the two is observed for rather low amounts of pile-up, typically lower than 50. In particular in Ref.…”
Section: Introductionmentioning
confidence: 99%
“…Rev. D102, 074014 (2020) [1] which has demonstrated that the sum of two semi-exclusive t t production modes, namely in photon-Pomeron (γP) and Pomeron-Pomeron (PP) interactions, can be experimentally measured when the t t system decays semi-leptonically, t t → jjblν l b, both forward protons are tagged and a low amount of pile-up is present. In this study we focus on separating individual channels and a special attention is paid to the situation at high-luminosity LHC environment.…”
The elastic production of top quark pairs in pp collisions at low and high luminosity regimes is investigated in detail. We extend the study performed in Phys. Rev. D102, 074014 (2020) [1] which has demonstrated that the sum of two semi-exclusive t t production modes, namely in photon-Pomeron (γP) and Pomeron-Pomeron (PP) interactions, can be experimentally measured when the t t system decays semi-leptonically, t t → jjblν l b, both forward protons are tagged and a low amount of pile-up is present. In this study we focus on separating individual channels and a special attention is paid to the situation at high-luminosity LHC environment. We observe that the separation of the PP and γγ events is a challenging task, especially at high amounts of pile-up even with an optimistic 10 ps resolution of timing detectors. In contrast, the γP signal is relatively well separable from all backgrounds at low levels of pile-up, allowing us to discover the elastic t t production and probe, for the first time, the production of a top quark pair in the γP interactions. The diffractive photoproduction of such a complex system as the t t pair hence can be used not only to study diffractive properties of the scattering amplitude but also to search for new physics beyond the Standard Model, and consequently to be a solid part of the physics programme of forward proton detectors at LHC.
“…Previous phenomenology studies based on the use of the proton tagging technique to study two-photon fusion interactions can be found in refs. [12][13][14][15][16][17][18][19][20][21][22][23][24][25][26][27][28]. Other interesting studies that aim also to describe photon fluxes in processes with proton dissociation, treated in the k T factorization framework, are presented in refs.…”
We present a phenomenology study on central exclusive production of W+W− boson pairs in proton-proton collisions at the Large Hadron Collider at 14 TeV using the forward proton detectors, such as the ATLAS Forward Proton or the CMS-TOTEM Precision Proton Spectrometer detectors. Final states where at least one of the W bosons decay hadronically in a large-radius jet are considered. The latter extends previous efforts that consider solely leptonic final states. A measurement of exclusive W+W− also allows us to further constrain anomalous quartic gauge boson interactions between photons and W bosons. Expected limits on anomalous quartic gauge couplings $$ {a}_{0,C}^W $$
a
0
,
C
W
associated to dimension-six effective operators are derived for the hadronic, semi-leptonic, and leptonic final states. It is found that the couplings can be probed down to one-dimensional values of $$ {a}_0^W=3.7\times {10}^{-7}{\mathrm{GeV}}^{-2} $$
a
0
W
=
3.7
×
10
−
7
GeV
−
2
and $$ {a}_C^W=9.2\times {10}^{-7}{\mathrm{GeV}}^{-7} $$
a
C
W
=
9.2
×
10
−
7
GeV
−
7
at 95% CL at an integrated luminosity of 300 fb−1 by combining all final states, compared to values of about $$ {a}_0^W=4\times {10}^{-6}{\mathrm{GeV}}^{-2} $$
a
0
W
=
4
×
10
−
6
GeV
−
2
and $$ {a}_C^W=1\times {10}^{-5}{\mathrm{GeV}}^{-2} $$
a
C
W
=
1
×
10
−
5
GeV
−
2
at 95% CL expected for the leptonic channel alone.
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