43 research outputs found

    Isomeric pair 95m,gNb{^{95\rm m,g}\rm{Nb}} in photonuclear reactions on nat^{\rm nat}Mo at end-point bremsstrahlung energy of 35-95 MeV

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    The natMo(γ,xnp)95m,g{^{\rm nat}\rm{Mo}}(\gamma,x\rm np)^{95\rm m,g}Nb photonuclear reaction was studied using the electron beam from the NSC KIPT linear accelerator LUE-40. Experiment was performed using the activation and off-line γ\gamma-ray spectrometric technique. The experimental isomeric yield ratio d(Eγmax)=Ym(Eγmax)/Yg(Eγmax)d(E_{\rm{\gamma max}}) = Y_{\rm m}(E_{\rm{\gamma max}}) / Y_{\rm g}(E_{\rm{\gamma max}}) was determined for the reaction products 95m,gNb^{95\rm m,g}\rm{Nb} at the end-point bremsstrahlung energy EγmaxE_{\rm{\gamma max}} range of 35-95 MeV. The obtained values of d(Eγmax)d(E_{\rm{\gamma max}}) are in satisfactory agreement with the results of other authors and extend the range of previously known data. The theoretical values of the yields Ym,g(Eγmax)Y_{\rm m,g}(E_{\rm{\gamma max}}) and the isomeric yield ratio d(Eγmax)d(E_{\rm{\gamma max}}) for the isomeric pair 95m,gNb^{95\rm m,g}\rm{Nb} from the natMo(γ,xnp){^{\rm nat}\rm{Mo}}(\gamma,x\rm np) reaction were calculated using the partial cross-sections σ(E)\sigma(E) from the TALYS1.95 code for six different level density models LDLD. The comparison showed a noticeable excess (more than 3.85 times) of the experimental isomeric yield ratio over all theoretical estimates. At the investigated range of EγmaxE_{\rm{\gamma max}} the theoretical dependence of d(Eγmax)d(E_{\rm{\gamma max}}) on energy was confirmed - the isomeric yield ratio smoothly decreases with increasing energy.Comment: 9 pages, 9 figures, 1 tabl

    Photonuclear reactions cross-sections at energies up to 100 MeV for different experimental setups

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    In experiments on the electron linac LUE-40 of RDC "Accelerator" NSC KIPT, the flux-averaged cross-sections ⟨σ(Eγmax)⟩exp\langle{\sigma(E_{\rm{\gamma max}})}\rangle_{\rm{exp}} of photonuclear reactions 100Mo(γ,n)99Mo{^{100}\rm{Mo}}(\gamma,n)^{99}\rm{Mo}, 27Al(γ,x)24Na{^{27}\rm{Al}}(\gamma,x)^{24}\rm{Na}, 93Nb(γ,n)92mNb{^{93}\rm{Nb}}(\gamma,n)^{92m}\rm{Nb}, 93Nb(γ,3n)90Nb{^{93}\rm{Nb}}(\gamma,3n)^{90}\rm{Nb}, and 181Ta(γ,n)180gTa{^{181}\rm{Ta}}(\gamma,n)^{180g}\rm{Ta} were measured using the γ\gamma-activation technique. The theoretical flux-average cross-sections ⟨σ(Eγmax)⟩th\langle{\sigma(E_{\rm{\gamma max}})}\rangle_{\rm{th}} were computed using the partial cross-section σ(E)\sigma(E) values from the TALYS1.9-1.95 codes and bremsstrahlung γ\gamma-flux calculated using GEANT4.9.2. Two different experimental setups were used in the experiments: an aluminum electron absorber and a deflecting magnet to clean the bremsstrahlung γ\gamma-flux from electrons. A comparison of the flux-average cross-sections measured for two experimental setups was performed. The possibility of using the reactions 100Mo(γ,n)99Mo{^{100}\rm{Mo}}(\gamma,n)^{99}\rm{Mo}, 27Al(γ,x)24Na{^{27}\rm{Al}}(\gamma,x)^{24}\rm{Na}, 93Nb(γ,n)92mNb{^{93}\rm{Nb}}(\gamma,n)^{92m}\rm{Nb}, 93Nb(γ,3n)90Nb{^{93}\rm{Nb}}(\gamma,3n)^{90}\rm{Nb}, and 181Ta(γ,n)180gTa{^{181}\rm{Ta}}(\gamma,n)^{180g}\rm{Ta} as monitors of the bremsstrahlung γ\gamma-flux for the energy range 30-100 MeV was investigated.Comment: 8 pages, 6 figures, 1 tabl

    Production of 180m{^{180\rm{m}}}Hf in photoproton reaction 181{^{181}}Ta(γ,p)(\gamma,p) at energy EγmaxE_{\rm{\gamma max}} = 35-95 MeV

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    The production of the 180mHf^{180\rm{m}}\rm{Hf} nuclei in the photoproton reaction 181Ta(γ,p){^{181}\rm{Ta}}(\gamma,p) was studied at end-point bremsstrahlung energies EγmaxE_{\rm{\gamma max}} = 35-95 MeV. The experiment was performed at the electron linear accelerator LUE-40 NSC KIPT with the use of the γ\gamma activation and off-line γ\gamma-ray spectroscopy. The experimental values of the bremsstrahlung flux-averaged cross-sections ⟨σ(Eγmax)⟩m\langle{\sigma(E_{\rm{\gamma max}})}\rangle_{\rm{m}} for the 181Ta(γ,p)180mHf{^{181}\rm{Ta}}(\gamma,p)^{180\rm{m}}\rm{Hf} reaction were determined, and at Eγmax>55E_{\rm{\gamma max}} > 55 MeV obtained for the first time. The measured values, also as the literature data, are significantly exceed the theoretical flux-averaged cross-sections ⟨σ(Eγmax)⟩th\langle{\sigma(E_{\rm{\gamma max}})}\rangle_{\rm{th}}. The ⟨σ(Eγmax)⟩th\langle{\sigma(E_{\rm{\gamma max}})}\rangle_{\rm{th}} values were calculated using the cross-section σ(E)\sigma(E) computed with the TALYS1.95 code for six different level density models. A comparative analysis of the calculated total cross-sections for the reactions 181Ta(γ,p)180Hf{^{181}\rm{Ta}}(\gamma,p)^{180}\rm{Hf} and 181Ta(γ,n)180Ta{^{181}\rm{Ta}}(\gamma,n)^{180}\rm{Ta} was performed. It was shown that the photoproton (γ,p)(\gamma,p) to photoneutron (γ,n)(\gamma,n) strength ratio is consistent with the estimates based on the isospin selection rules and the value from the (e,e′p)(e,e'p) experiment.Comment: 9 pages, 4 figures, 2 table

    Population immunity to SARS-CoV-2 virus in residents of the Irkutsk Region in the dynamics of the epidemic

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    Background. Currently, the COVID-19 pandemic in the world and in Russia remains the main event. In this regard, the study of the manifestations of the epidemic process of the new coronavirus infection COVID-19 and the patterns of its development are an urgent area of research. In the fight against this viral disease, an important role is assigned to the study of the development of population immunity to the SARSCoV-2 virus, which will make it possible to assess the dynamics of seroprevalence and the formation of post-infectious humoral immunity, forecasting the development of the epidemiological situation, elucidating the characteristics of the epidemic process, and will also contribute to planning activities for specific and non-specific prevention of the disease.The aim: to determine the dynamics of population immunity to SARS-CoV-2 among the population of the Irkutsk region during the COVID-19 pandemic.Materials and methods. As a part of the Rospotrebnadzor project of assessing population immunity to SARS-CoV-2 in the population of the Russian Federation, the research has being conducted among the population of the Irkutsk region in the periods from June 23, 2020 to July 19, 2020 (Stage 1), from September 16, 2020 to September 25, 2020 (Stage 2), from December 7, 2020 to December 18, 2020 (Stage 3) and from March 8, 2021 to March 14, 2021(Stage 4), taking into account the reacted one recommended by the WHO. The content of antibodies to SARS-CoV-2 was determined by ELISA using a set of tests for human serum or plasma for specific immunoglobulins of class G to the proteins of the SARS-CoV-2 coronavirus.The results. The research of the humoral immunity of volunteers shows that during the period of an epidemic rise in the incidence of COVID-19 in the Irkutsk region, a low level of seroprevalence was formed (Stage 1 – 5.8 ± 0.5 %, Stage 2 – 12.1 ± 0.7 %), and in conditions of a long-term maximum increase in the incidence rate – 25.9 ± 1.0 % (Stage 3) and 46.2 ± 1.2 % (Stage 4). A significant proportion (Stage 1 – 82.2 ± 3.2 %, Stage 2 – 86.1 ± 2.3 %) of asymptomatic forms of infection characterizes the high intensity of the latently developing epidemic process in the first two stages. High levels of IgG in reconvalescents of COVID-19 persisted for an average of 3 to 5 months.Conclusion. The results of assessing the population immunity to the SARS-CoV-2 virus in the population of the Irkutsk region indicate that the seroprevalence level at Stage 4 of the research was 46.2 %. After the disease, on average, 49.5 % of persons did not detect antibodies. The results obtained should be taken into account when organizing preventive measures, including vaccination, and predicting morbidity

    ABOUT PAINLEVE PROPERTY OF A HYDRODYNAMIC SYSTEM

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    We represent conditions of hydrodynamic system when it passes the Painleve test. We use Kovaleskaya-Gambie method for fourth order ordinary differential system. We obtain Lorenz-like dynamic, hydrodynamic syste
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