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From Transition Electromagnetic Form Factors $\gamma^* \gamma^* \eta_c(1S,2S)$ to the Production of $\eta_c(1S,2S)$ at the LHC

We review our recent results for production of $\eta_c(1S)$ and $\eta_c(2S)$ in the $\gamma^* \gamma^* \to \eta_c(1S,2S)$ fusion and in proton-proton collisions via gluon-gluon fusion. The quarkonium wave functions are calculated by solving Schr\"odinger equation for different $c \bar c$ potent...

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Detalles Bibliográficos
Autor principal: Szczurek, Antoni
Lenguaje:eng
Publicado: 2020
Materias:
Acceso en línea:https://dx.doi.org/10.5506/APhysPolB.51.1559
http://cds.cern.ch/record/2741026
Descripción
Sumario:We review our recent results for production of $\eta_c(1S)$ and $\eta_c(2S)$ in the $\gamma^* \gamma^* \to \eta_c(1S,2S)$ fusion and in proton-proton collisions via gluon-gluon fusion. The quarkonium wave functions are calculated by solving Schr\"odinger equation for different $c \bar c$ potentials. Using Terentev prescription the light-cone wave functions are obtained. The light-cone wave functions are used then to calculate $\gamma^* \gamma^* \to \eta_c$ transition form factors. The theoretical results are compared to the Belle experimental data for $\eta_c(1S)$. In addition we discuss our results for two-photon decay width. We present also results of our calculations for proton-proton collisions obtained within $k_T$-factorization approach for different unintegrated gluon distributions. The results for hadroproduction of $\eta_c(1S)$ are compared to the LHCb experimental data.