scholarly journals Refined mass estimate for bilepton gauge boson

2021 ◽  
pp. 2150118
Author(s):  
Claudio Corianò ◽  
Paul H. Frampton

Using the most recent experimental data on parameters of the standard electroweak theory, as well as renormalization group equations with a boundary matching condition, we derive a refined and more accurate value for the mass of the doubly-charged bilepton [Formula: see text] occurring in the spontaneous breaking of the gauge group [Formula: see text] to the standard electroweak gauge group [Formula: see text]. Our result is [Formula: see text] TeV.

1996 ◽  
Vol 11 (19) ◽  
pp. 3509-3522 ◽  
Author(s):  
DAE SUNG HWANG ◽  
CHANG-YEONG LEE ◽  
YUVAL NE’EMAN

A superconnection, in which a scalar field enters as a zero-form in the odd part of the superalgebra, is used in the BRST quantization of the SU (2/1) “internally superunified” electroweak theory. A quantum action is obtained, by applying symmetric BRST/anti-BRST invariance. Evaluating the mass of the Higgs field, we exhibit the consistency between two approaches: (a) applying the supergroup’s (gauge) value for λ, the coupling of the scalar field’s quartic potential, to the conventional (spontaneous symmetry breakdown) evaluation; (b) dealing with the superconnection components as a supermultiplet of an (global) internal supersymmetry. This result thus provides a general foundation for the use of “internal” supergauges. With SU (2/1) broken by the negative squared mass term for the Higgs field and with the matter supermultiplets involving added “effective” ghost states, there is no reason to expect the symmetry’s couplings not to be renormalized. This explains the small difference between predicted and measured values for sin2θw, namely the other coupling fixed by SU (2/1) beyond the Standard Model’s SU(2)×U(1), and where the experimental results are very precise. Using the renormalization group equations and those experimental data, we thus evaluate the energy E8 at which the SU (2/1) predicted value of 0.25 is expected to correspond to the experimental values. With SU (2/1) precise at that energy Es=5 TeV , we then apply the renormalization group equations again, this time to evaluate the corrections to the above λ, the quartic coupling of the scalar fields; as a result we obtain corrections to the prediction for the Higgs meson’s mass. Our result predicts the Higgs’ mass [170 GeV, according to unrenormalized SU (2/1)] to be as low as 130±6 GeV , using for the top quark mass the recently measured value of 174 GeV .


1990 ◽  
Vol 05 (20) ◽  
pp. 1599-1604 ◽  
Author(s):  
I.L. BUCHBINDER ◽  
I.L. SHAPIRO ◽  
E.G. YAGUNOV

GUT’s in curved space-time is considered. The set of asymptotically free and asymptotically conformally invariant models based on the SU (N) gauge group is constructed. The general solutions of renormalization group equations are considered as the special ones. Several SU (2N) models, which are finite in flat space-time (on the one-loop level) and asymptotically conformally invariant in external gravitational field are also presented.


2021 ◽  
Vol 2021 (11) ◽  
Author(s):  
Shun Zhou

Abstract As is well known, the smallest neutrino mass turns out to be vanishing in the minimal seesaw model, since the effective neutrino mass matrix Mν is of rank two due to the fact that only two heavy right-handed neutrinos are introduced. In this paper, we point out that the one-loop matching condition for the effective dimension-five neutrino mass operator can make an important contribution to the smallest neutrino mass. By using the available one-loop matching condition and two-loop renormalization group equations in the supersymmetric version of the minimal seesaw model, we explicitly calculate the smallest neutrino mass in the case of normal neutrino mass ordering and find m1 ∈ [10−8, 10−10] eV at the Fermi scale ΛF = 91.2 GeV, where the range of m1 results from the uncertainties on the choice of the seesaw scale ΛSS and on the input values of relevant parameters at ΛSS.


2012 ◽  
Vol 22 (1) ◽  
pp. 1-6
Author(s):  
Hoang Ngoc Long ◽  
Nguyen Thi Kim Ngan

Renormalization group equations of the 3-3-1 models with A4 and S4 flavor symmetries as the only intermediate gauge group between the standard model and the scale of unification of the three coupling constants are presented. We shall assume that there is no necessarily a group of grand unification at the scale of convergence of the couplings.


2015 ◽  
Vol 11 (2) ◽  
pp. 2972-2978
Author(s):  
Fouad A. Majeed ◽  
Yousif A. Abdul-Hussien

In this study the calculations of the total fusion reaction cross section have been performed for fusion reaction systems 17F + 208Pb and 15C + 232Th which involving halo nuclei by using a semiclassical approach.The semiclassical treatment is comprising the WKB approximation to describe the relative motion between target and projectile nuclei, and Continuum Discretized Coupled Channel (CDCC) method to describe the intrinsic motion for both target and projectile nuclei. For the same of comparsion a full quantum mechanical clacualtions have been preforemd using the (CCFULL) code. Our theorticalrestuls are compared with the full quantum mechaincialcalcuations and with the recent experimental data for the total fusion reaction  checking the stability of the distancesThe coupled channel calculations of the total fusion cross section σfus, and the fusion barrier distribution Dfus. The comparsion with experiment proves that the semiclassiacl approach adopted in the present work reproduce the experimental data better that the full quantal mechanical calcautions. 


2021 ◽  
Vol 2021 (2) ◽  
Author(s):  
Yohei Ema ◽  
Kyohei Mukaida ◽  
Jorinde van de Vis

Abstract We derive one- and two-loop renormalization group equations (RGEs) of Higgs-R2 inflation. This model has a non-minimal coupling between the Higgs and the Ricci scalar and a Ricci scalar squared term on top of the standard model. The RGEs derived in this paper are valid as long as the energy scale of interest (in the Einstein frame) is below the Planck scale. We also discuss implications to the inflationary predictions and the electroweak vacuum metastability.


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