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Ivan V. Zaitsev

Publications and source records attributed to Ivan V. Zaitsev.

10 recordsLinked to original sources

On a possible effective four-boson interaction and its implications at the upgraded LHC

We consider a possibility of a spontaneous generation of fourfold effective interactions of electroweak gauge bosons $W^a$ and $B$. The conditions for the spontaneous generation are shown to lead to a set of compensation equations for parameters of the interaction. In case of a realization of a non-trivial solution of the set, important electro-weak parameter $\sin^2θ_W$ is defined. The existence of two non-trivial solutions is demonstrated, which provide a satisfactory value for the electromagnetic fine structure constant $α$ at scale $M_Z$: $α(M_Z) = 0.007756$. There is a solution with the high effective cut-off being close to the Planck mass by the order of magnitude. The most interesting solution corresponds to effective cut-off $\simeq 10^2\,TeV$. This solution gives quite definite prediction for non-perturbative effects in processes $p+p\to\bar t t (W^\pm, Z)$, which could be observed at the upgraded LHC.

hep-ph↗

On a possibility to calculate fundamental parameters of the Standard Model

The problem of a calculation of parameters of the Standard Model is considered in the framework of the compensation approach. Conditions for a spontaneous generation of effective interactions of fundamental fields are shown to lead to sets of equations for parameters of a theory. A principal possibility to calculate mass ratios of fundamental quarks and leptons is demonstrated, as well of mixing angles of quarks, e.g. of the Cabibbo angle. A possibility of a spontaneous generation of an effective interaction of electroweak gauge bosons $W^a$ and $B$ is demonstrated. In case of a realization of a non-trivial solution of a set of compensation equations, parameter $\sin^2θ_W$ is defined. The non-trivial solution is demonstrated to provide a satisfactory value for the electromagnetic fine structure constant $α$ at scale $M_Z$: $α(M_Z) = 0.00772$. The results being obtained may be considered as sound arguments on behalf of a possibility of a calculation of parameters of the Standard Model.

hep-ph↗

Elimination of the Landau pole in QCD with the spontaneously generated anomalous three-gluon interaction

We apply the Bogoliubov compensation principle to QCD. The non-trivial solution of compensation equations for a spontaneous generation of the anomalous three-gluon interaction leads to the determination of parameters of the theory, including behavior of the gauge coupling $α_s(Q^2)$ without the Landau singularity, the gluon condensate $V_2\,\simeq\,0.01\,GeV^4$, mass of the lightest glueball $M_G\,\simeq\,1500\,MeV$ in satisfactory agreement with the phenomenological knowledge. The results strongly support the applicability of N.N. Bogoliubov compensation approach to gauge theories of the Standard Model.

hep-th↗

Non-perturbative approach to the problem of anomalous FB asymmetry in top pair production at TEVATRON

We apply Bogoliubov compensation principle to the problem of forward-backward asymmetry in $t \bar t$ production at TEVATRON. The non-trivial solution of compensation equation for anomalous four-fermion interaction effective interaction of doublets of heavy and light quarks leads to possibility of existence of $\bar t u,\, \bar b d$ vector bound states (resonance). The coupling of the bound state to $\bar t,\,u$ pair is calculated. With this result we obtain satisfactory description of totality of data on the effect of FB asymmetry including slope of effect dependence on invariant $t \bar t$ mass. Predictions for the resonance mass and production cross-section at LHC are presented.

hep-ph↗

LHC would-be $γ\,γ$ excess as a non-perturbative effect of the electro-weak interaction

The recently reported would-be excess at $125\, GeV$ in invariant mass distribution of $γ\, γ$ and of $l^+\,l^+\,l^-\,l^-$ obtained in the course of the Higgs boson search at LHC is tentatively interpreted as a scalar bound state of two $W$. Non-perturbative effects of EW interaction obtained by application of Bogoliubov compensation approach lead to such bound state due to existence of anomalous three-boson gauge-invariant effective interaction. The application of this scheme gives satisfactory agreement with existing data without any adjusting parameter but the bound state mass $125\,GeV$, while $σ\,BR$ for $γ\,γ$ resonance is predicted to be twice more as the value for the SM Higgs. Decay channel $γ\,l^+\,l^-$ may serve as a decisive check of the interpretation.

hep-ph↗

CDF Wjj anomaly as a non-perturbative effect of the electro-weak interaction

The recently reported CDF excess at $120\,-\, 160\,GeV$ in invariant mass distribution of jet pairs accompanying $W$-boson is tentatively interpreted as a bound state of two $W$ decaying to quark-anti-quark pair. Non-perturbative effects of EW interaction obtained by application of Bogoliubov compensation approach lead to such bound state due to existence of anomalous three-boson gauge-invariant effective interaction. The application of this scheme gives satisfactory agreement with existing data without any adjusting parameter but the bound state mass $145\,GeV$.

hep-ph↗

Non-perturbative solutions in the electro-weak theory with $\bar t t$ condensate and the $t$-quark mass

We apply Bogoliubov compensation principle to the gauge electro-weak interaction to demonstrate a spontaneous generation of anomalous three-boson gauge invariant effective interaction. The non-trivial solution of compensation equations uniquely defines the form-factor of the anomalous interaction and parameters of the theory including value of gauge electro-weak coupling $g(M_W^2)$ in satisfactory agreement with its experimental value. A possibility of spontaneous generation of effective four-fermion interaction of heavy quarks is also demonstrated. This interaction defines an equation for a scalar bound state of heavy quarks which serve as a substitute for the elementary scalar Higgs doublet. As a result we calculate the $t$-quark mass $m_t\,=\,177\,GeV$ in satisfactory agreement with the experimental value. The results strongly support idea of $\bar t\,t$ condensate as a source of the electro-weak symmetry breaking.

hep-ph↗

Non-perturbative solutions in the electro-weak theory and the Higgs boson mass

We apply Bogoliubov compensation principle to the gauge electro-weak interaction to demonstrate a spontaneous generation of anomalous three-boson gauge invariant effective interaction. The non-trivial solution of compensation equations uniquely defines the form-factor of the anomalous interaction and parameters of the theory including value of gauge electro-weak coupling $g(M_W^2)\simeq 0.62$ in satisfactory agreement to the experimental value. A possibility of spontaneous generation of effective four-fermion interaction of heavy quarks is also demonstrated. This interaction defines an equation for a scalar bound state of heavy quarks which serve as a substitute for the elementary scalar Higgs doublet. As a result we obtain two possible solutions for the observable Higgs boson mass: $M_1\,=\,(306\,\pm\,14)GeV$ and $M_2\,=\,(253\,\pm\,10)\,GeV$. Values for other parameters e.g. anomalous three-boson coupling $\,G$, Higgs boson width $Γ_H$, its branching ratios and estimates for cross-section of Higgs production at LHC are also obtained.

hep-ph↗

NJL interaction derived from QCD: vector and axial-vector mesons

In previous works effective non-local $SU(2)\times SU(2)$ NJL model was derived in the framework of the fundamental QCD. All the parameters of the model are expressed through QCD parameters: current light quark mass $m_0$ and average non-perturbative $α_s$. The results for scalar and pseudo-scalar mesons are in satisfactory agreement to existing data. In the present work the same model without introduction of any additional parameters is applied for a description of masses and strong decay widths of $ρ$- and $a_1$-mesons. The results for both scalar and vector sectors agree with data with only one adjusted parameter $m_0$, with account of average $α_s \simeq 0.415$, which is obtained in a previous work as well.

hep-ph↗

NJL model derived from QCD

We apply Bogolubov approach to QCD with two light quarks to demonstrate a spontaneous generation of an effective interaction, leading to the Nambu -- Jona-Lasinio model. The resulting theory contains two parameters: average low-energy value of $α_s$ and current light quark mass $m_0$. All other low-energy parameters: the pion decay constant, mass of the $π$-meson, mass of the $σ$-meson and its width, the constituent quark mass, the quark condensate are expressed in terms of the two input parameters in satisfactory correspondence to experimental data and chiral phenomenology. {\it E.g.} in the approximation being used we have for $α_s = 0.67$ and $m_0 = 20 MeV$: $f_π= 93 MeV, m_π= 135 MeV, m_σ= 492 MeV, Γ_σ= 574 MeV, m_q = 295 MeV, <\bar q q> = -(222 MeV)^3$.

hep-ph↗