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A. N. Tabachenko

Publications and source records attributed to A. N. Tabachenko.

6 recordsLinked to original sources

Isobar configurations: $ΔN$ correlations versus the independent particle model

We present a comparative analysis of two models for the $A( {γ,\,πN})B$ reaction, which take into account the isobar configurations in the ground state of the nuclei: the $ΔN$ correlation model and the quasifree pion photoproduction model. The considered models differ in their descriptions of the nucleus states. The $ΔN$ correlation model takes into account the dynamic correlations of the nucleon and isobar formed in the virtual transition $NN \to ΔN$, and in the quasifree pion photoproduction model, isobars and nucleons in the nucleus are considered as independent constituents. The predictions of the models are considered for two reactions ${}^{16}$O$( {γ,\,π^{ +} p} ){}^{15}$C and ${}^{16}$O$( {γ,\,π^{ -} p} ){}^{15}$O. It is shown, that the two models predict the differential cross section significantly differing both in absolute values, and in the shape of the angular dependence. We compare the results of the $ΔN$ correlation model for the $( {γ,\,πN} )$ and $( {γ,\,πNN})$ reactions with the ${}^{16}$O$( {γ,\, π^{ -} p})$ reaction data measured at BNL. Our results give support to the $ΔN$ correlation model.

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Pion photoproduction on nucleus with two-nucleon emission

A model for the pion photoproduction on nuclei in the $A\left({γ,\, πNN} \right)B$ reaction is presented. This is an extension of our recent model for the $A\left({γ,\, πN} \right)B$ reaction. In this approach we have moved beyond the standard shell-model considering $Δ$\textit{N} correlations in the nuclear wave functions, which are caused by the virtual transitions $NN \to ΔN \to NN$ in the ground state of the nucleus. The main ingredients of the model are the two- and three-particle density matrices and the transition operators $γΔ\to Nπ$ and $γN \to Nπ$. The direct and exchange reaction mechanisms, which follow from the structure of the density matrices, are examined. The model is used to investigate the $^{12}$C$\left({γ,\, π^{+} p} \right)$ and $^{12}$C$\left({γ,\, π^{-} p} \right)$ reactions in the kinematic region of the large momentum transfers to the residual nuclear system, where the pion production occurs with the emission of two nucleons.

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Photoproduction of the $πN$ pair on nuclei and isobar configurations

A model of $πN$ pair photoproduction on nuclei at high momentum transfer is presented. The $A(γ,πN)B$ reaction amplitude is obtained by means of an extended impulse approximation, according to which the nuclear wavefunction includes delta-isobar components in addition to nucleon components. A one-particle transition operator is defined in terms of the two-body $γN\toπN$ and $γΔ\toπN$ photoproduction amplitudes. Direct and exchange mechanisms of the nuclear photoproduction reaction are studied, and numerical estimates are made and presented of $^{12}{\rm C}(γ,π^- p){^{11}{\rm C}}$ and $^{12}{\rm C}(γ,π^+ p){^{11}{\rm Be}}$ differential cross sections at photon incident energies in the $Δ(1232)$ resonance region.

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Momentum distribution of Delta- isobar in closed shell nuclei

One Delta- isobar components of the wave function in closed shell nuclei are considered within the framework of the harmonic oscillator model. Conventional transition potential is the pi- and rho- exchange potential. On the basis of the Delta- isobar configuration wave function, the momentum distribution of the Delta- isobar is calculated for the light nuclei $^4 He$,$^{16}O$,$^{12}C$

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Search for Delta^++ component in 12^C ground state using 12^C(gamma, pi^+ p) reaction

The differential cross section for the $^{12}$C$(γ,π^{+}p)$ reaction has been measured in the $Δ$(1232) resonance region at high recoil momenta of the residual nuclear system. The data are analyzed under the assumption that the formation of the $π^+p$ pairs may be interpreted as a $γΔ^{++}\toπ^+p$ process which takes place on a $Δ^{++}$ preexisting in the target nucleus. Estimates of the $Δ^{++}$ momentum distribution $ρ_{Δ^{++}}(\bar{p})$=0.17 fm$^3$ for a mean momentum $\bar{p}=300\pm49$ MeV/c as well as the number of $Δ$ isobars per nucleon $N_Δ=0.017$ were obtained for $^{12}$C.

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Search for the $Δ^{++}$ component in $^{12}C$ ground state using $^{12}C(γ, π^{+}p)$ reaction

The differential cross section for the reaction $^{12}$C$(γ,π^{+}p)$ has been measured in the $Δ$ resonance region at high recoil momenta of the residual nuclear system. The data are analysed under the assumption that the formation of $π^+p$ pairs may be interpreted as $γΔ^{++}\toπ^+p$ process, proceeding on the $Δ^{++}$ constituent in a target nucleus. As a result, the estimation $N_Δ=0.028\pm 0.008$ deltas per nucleon in $^{12}$C was obtained.

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