scholarly journals Multiple production of neutral Higgs bosons at high-energy e+e− colliders

1996 ◽  
Vol 375 (1-4) ◽  
pp. 203-212 ◽  
Author(s):  
A Djouadi ◽  
H.E Haber ◽  
P.M Zerwas
1989 ◽  
Vol 04 (15) ◽  
pp. 1485-1494 ◽  
Author(s):  
J.A. GRIFOLS ◽  
A. MÉNDEZ ◽  
G.A. SCHULER

Higgs bosons with two units of electric charge are an essential ingredient of Left-Right Symmetric Models. We discuss their production and decay at high energy colliders.


1976 ◽  
Vol 13 (7) ◽  
pp. 2013-2027 ◽  
Author(s):  
Richard C. Arnold ◽  
Gerald H. Thomas

2010 ◽  
Vol 19 (10) ◽  
pp. 2023-2031 ◽  
Author(s):  
B. G. SIDHARTH

We consider p–p collisions at very high energy. This becomes relevant in view of the LHC which has just resumed operation. Such collisions will take place in it and indeed already have taken place. Though recent results at the Tevatron in the U.S. seem to rule out the Higgs bosons, there are other results which are eagerly expected, some of these are surveyed here.


2001 ◽  
Vol 16 (supp01a) ◽  
pp. 92-103 ◽  
Author(s):  
R. L. Culbertson

The search for physics beyond the Standard Model includes Technicolor particles, Higgs Bosons, compositeness, many variations of Supersymmetry, large extra dimensions, model-independent searches for anomalies, and other topics. This article reports a subset of these ongoing searches at the high-energy colliders, Tevatron, HERA and LEP.


2010 ◽  
Vol 25 (40) ◽  
pp. 3335-3346
Author(s):  
D. V. NANOPOULOS

In supercritical string cosmology (SSC), a time-dependent dilaton leads to a smoothly evolving dark energy and modifies the regions of the mSUGRA parameter space where the observed value of the dark matter relic density may be obtained. In particular, the dilaton dilutes the supersymmetric dark matter density (of neutralinos) by a factor [Formula: see text] and consequently relaxes the allowed parameter mSUGRA parameter space. The final states expected at the LHC in this scenario, consist of Z bosons, Higgs bosons, and/or high energy taus. From this, it is possible to characterize these final states and determine the model parameters. Using these parameters, we determine the dark matter content and the neutralino–proton cross section. All these techniques can also be applied to determine model parameters in SSC models with different SUSY breaking scenarios.


2001 ◽  
Vol 16 (supp01b) ◽  
pp. 839-842
Author(s):  
◽  
G. Gómez-Ceballos

A search for pair produced charged Higgs bosons was performed in the high energy data collected by the DELPHI detector at LEP II at centre-of-mass energies from 183 GeV to 208 GeV. The three different final states, τντν, [Formula: see text] and [Formula: see text] were considered. No excess of data compared to the expected Standard Model processes was observed and the existence of a charged Higgs boson with mass lower than 75.0 GeV / c 2 is excluded at 95% confidence level.


2020 ◽  
Vol 80 (9) ◽  
Author(s):  
F. Arco ◽  
S. Heinemeyer ◽  
M. J. Herrero

AbstractAn important task at future colliders is the measurement of the triple Higgs coupling. Depending on its size relative to the Standard Model (SM) value, certain collider options result in a higher experimental accuracy. Within the framework of Two Higgs Doublet Models (2HDM) types I and II we investigate the allowed ranges for all triple Higgs couplings involving at least one light, SM-like Higgs boson. We take into account theoretical constraints (unitarity, stability), experimental constraints from direct Higgs-boson searches, measurements of the SM-like Higgs-boson properties, flavor observables and electroweak precision data. We find that the SM-type triple Higgs coupling w.r.t. its SM value, $$\lambda _{hhh}/\lambda _{\mathrm {SM}}$$ λ hhh / λ SM , can range between $$\sim -0.5$$ ∼ - 0.5 and $$\sim 1.5$$ ∼ 1.5 . Depending on which value is realized, the HL-LHC can compete with, or is clearly inferior to the ILC. We find the coupling $$\lambda _{hhH}$$ λ hhH between $$\sim -1.5$$ ∼ - 1.5 and $$\sim 1.5$$ ∼ 1.5 . Triple Higgs couplings involving two heavy Higgs bosons, $$\lambda _{hHH}$$ λ hHH , $$\lambda _{hAA}$$ λ hAA and $$\lambda _{hH^+H^-}$$ λ h H + H - can reach values up to $${{\mathcal {O}}}(10)$$ O ( 10 ) , roughly independent of the 2HDM type. This can lead to potentially strongly enhanced production of two Higgs-bosons at the HL-LHC or high-energy $$e^+e^-$$ e + e - colliders.


Sign in / Sign up

Export Citation Format

Share Document