scholarly journals ASSOCIATED TOP-HIGGS PRODUCTION AT FUTURE COLLIDERS

2001 ◽  
Vol 16 (supp01a) ◽  
pp. 375-378 ◽  
Author(s):  
Sally Dawson ◽  
Laura Reina

We discuss the relevance of the associated production of a Higgs boson with a pair of top antitop quarks at both the LHC and a future high energy e+e- collider.

1999 ◽  
Vol 14 (30) ◽  
pp. 2093-2107 ◽  
Author(s):  
A. G. AKEROYD ◽  
A. ARHRIB ◽  
M. CAPDEQUI PEYRANÉRE

We study the associated production of a CP-odd Higgs boson A0 with a neutral gauge boson (Z or photon) in high-energy e+e- collisions at the one-loop level in the framework of two Higgs doublet models (THDM). We find that in the small tan β regime, the top quark loop contribution is enhanced leading to significant cross-sections (about a few fb), while in the large tan β regime the cross-section does not attain observable rates.


2020 ◽  
Vol 2020 (12) ◽  
Author(s):  
Amit Adhikary ◽  
Rahool Kumar Barman ◽  
Biplob Bhattacherjee

Abstract The prospects of observing the non-resonant di-Higgs production in the Standard Model at the proposed high energy upgrade of the LHC, viz. the HE-LHC ($$ \sqrt{s} $$ s = 27 TeV and ℒ = 15 ab−1) is studied. Various di-Higgs final states are considered based on their cleanliness and production rates. The search for the non-resonant double Higgs production at the HE-LHC is performed in the $$ b\overline{b}\gamma \gamma $$ b b ¯ γγ , $$ b\overline{b}{\tau}^{+}{\tau}^{-} $$ b b ¯ τ + τ − , $$ b\overline{b}{WW}^{\ast } $$ b b ¯ WW ∗ , WW∗γγ, $$ b\overline{b}{ZZ}^{\ast } $$ b b ¯ ZZ ∗ and $$ b\overline{b}{\mu}^{+}{\mu}^{-} $$ b b ¯ μ + μ − channels. The signal-background discrimination is performed through multivariate analyses using the Boosted Decision Tree Decorrelated (BDTD) algorithm in the TMVA framework, the XGBoost toolkit and Deep Neural Network (DNN). The variation in the kinematics of Higgs pair production as a function of the self-coupling of the Higgs boson, λh, is also studied. The ramifications of varying λh on the $$ b\overline{b}\gamma \gamma $$ b b ¯ γγ , $$ b\overline{b}{\tau}^{+}{\tau}^{-} $$ b b ¯ τ + τ − and $$ b\overline{b}{WW}^{\ast } $$ b b ¯ WW ∗ search analyses optimized for the SM hypothesis is also explored.


2005 ◽  
Vol 20 (36) ◽  
pp. 2819-2825
Author(s):  
YONG JIA ◽  
YANMING ZHANG

We have studied a top-Higgs production process [Formula: see text] in the topcolor assisted technicolor (TC2) model. The studies show that the production cross-section of [Formula: see text] is at the order of magnitude 10 fb in reasonable parameters space of TC2 model. A few hundred events of top-Higgs can be produced each year at the high energy linear e+e- colliders (LC). The top-Higgs may be directly observed via this process.


2021 ◽  
Vol 81 (10) ◽  
Author(s):  
F. Arco ◽  
S. Heinemeyer ◽  
M. J. Herrero

AbstractAn important task at future colliders is the investigation of the Higgs-boson sector. Here the measurement of the triple Higgs coupling(s) plays a special role. Based on previous analyses, within the framework of Two Higgs Doublet Models (2HDM) type I and II, we define and analyze several two-dimensional benchmark planes, that are over large parts in agreement with all theoretical and experimental constraints. For these planes we evaluate di-Higgs production cross sections at future high-energy $$e^+e^-$$ e + e - colliders, such as ILC or CLIC. We consider two different channels for the neutral di-Higgs pairs $$h_i h_j=hh,hH,HH,AA$$ h i h j = h h , h H , H H , A A : $$e^+e^- \rightarrow h_i h_j Z$$ e + e - → h i h j Z and $$e^+e^- \rightarrow h_i h_j \nu {{\bar{\nu }}}$$ e + e - → h i h j ν ν ¯ . In both channels the various triple Higgs-boson couplings contribute substantially. We find regions with a strong enhancement of the production channel of two SM-like light Higgs bosons and/or with very large production cross sections involving one light and one heavy or two heavy 2HDM Higgs bosons, offering interesting prospects for the ILC or CLIC. The mechanisms leading to these enhanced production cross sections are analyzed in detail. We propose the use of cross section distributions with the invariant mass of the two final Higgs bosons where the contributions from intermediate resonant and non-resonant BSM Higgs bosons play a crucial role. We outline which process at which center-of-mass energy would be best suited to probe the corresponding triple Higgs-boson couplings.


2012 ◽  
Vol 85 (7) ◽  
Author(s):  
Shou-Shan Bao ◽  
Xue Gong ◽  
Hong-Lei Li ◽  
Shi-Yuan Li ◽  
Zong-Guo Si

2021 ◽  
Vol 2021 (4) ◽  
Author(s):  
Marco Niggetiedt

Abstract We follow up on our discussion of the exact quark-mass dependence of the Higgs-gluon form factor at three loops in QCD [1] and turn our attention to the closely related Higgs-photon form factor. Similarly to our previous work, we intend to examine the form factor for the decay of a Higgs-boson with variable mass into two photons at the three-loop level in QCD. The set of master integrals is known numerically due to prior work on the Higgs-gluon form factor and is exploited to obtain expansions around the threshold as well as in the high-energy limit. Our results may be utilised to derive the photonic decay rate of the Higgs-boson through next-to-next-to-leading order.


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