ÏÐÍÄ çà 2017-2018 ãã.
Ìóøêàðåíêîâ Àëåêñàíäð Íèêîëàåâè÷ 19.12.1980, êôìí, cíñ, ËÔßÐ
Ñòàòüè â ðåôåðèðóåìûõ çàðóáåæíûõ æóðíàëàõ:
[1] C. S. Akondi, ..., A. Mushkarenkov et al. [A2 Collaboration], “Experimental study of the ?p > K0?+, ?n > K0?, and ?n > K0?0 reactions at the Mainz Microtron,” arXiv:1811.05547 [nucl-ex]. 3*0.075 = 0.225 [2] A. Ka?ser, ..., A. Mushkarenkov et al., “First measurement of helicity-dependent cross sections in ?0? photoproduction from quasi-free nucleons,” Phys. Lett. B 786, 305 (2018) doi:10.1016/j.physletb.2018.10.006 [arXiv:1810.02778 [nucl-ex]]. 4.254*30*0.075 = 9.571 [3] M.Dieterle,...,A.Mushkarenkovet al.[A2Collaboration],“Photoproductionof ?0 Mesons o? Protons and Neutrons in the Second and Third Nucleon Resonance Region,” Phys. Rev. C, 065205 (2018) doi:10.1103/PhysRevC.97.065205 [arXiv:1805.10504 [nucl-ex]]. 3.304*30*0.075 = 7.434 [4] S. Prakhov, ..., A. Mushkarenkov et al. [A2 Collaboration], “High-statistics measurement of the ? > 3?0 decay at the Mainz Microtron,” Phys. Rev. C 97, no. 6, 065203 (2018) doi:10.1103/PhysRevC.97.065203 [arXiv:1803.02502 [hep-ex]]. 3.304*30*0.075 = 7.434 [5] V. Sokhoyan, ..., A. Mushkarenkov et al. [A2 Collaboration], “Experimental study of the ?p > ?0?p reaction with the A2 setup at the Mainz Microtron,” Phys. Rev. C 97, no. 5, 055212 (2018) doi:10.1103/PhysRevC.97.055212 [arXiv:1803.00727 [nucl-ex]]. 3.304*30*0.075 = 7.434 [6] T. Jude, ..., A. Mushkarenkov et al., “Strangeness photoproduction at the BGO-OD experiment,” PoS Hadron 2017, 054 (2018). doi:10.22323/1.310.0054 8*0.075 = 0.6 [7] P.Adlarson,...,A.Mushkarenkovet al.,“Measurementofthedecay ?0 > ?0?0? atMAMI,” Phys. Rev. D 98, no.1, 012001(2018) doi:10.1103/PhysRevD.98.012001 [arXiv:1709.04230 [hep-ex]]. 4.394*30*0.075 = 9.887 [8] M. Dieterle, ..., A. Mushkarenkov et al., “First measurement of the polarization observable E and helicity-dependent cross sections in single ?0 photoproduction from quasi-free nucleons,” Phys. Lett. B 770, 523 (2017) doi:10.1016/j.physletb.2017.04.079 [arXiv:1705.07342 [nucl-ex]]. 4.254*30*0.075 = 9.571
1
[9] L. Witthauer, ..., A. Mushkarenkov et al. [A2 Collaboration], “Helicity-dependent cross sections and double-polarization observable E in ? photoproduction from quasifree protons and neutrons,” Phys. Rev. C 95, no. 5, 055201 (2017) doi:10.1103/PhysRevC.95.055201 [arXiv:1704.00649 [nucl-ex]]. 3.304*30*0.075 = 7.434
[10] A. A. Turinge, A. M. Lapik, A. N. Mushkarenkov, V. G. Nedorezov and N. V. Rudnev, “Emission of d, t, 3He and ?-particles from 12C nuclei excited by intermediate energy photons,” EPJ Web Conf. 138, 01005 (2017). doi:10.1051/epjconf/201713801005 8/5 = 1.6
[11] A. A. Turinge, A. M. Lapik, A. N. Mushkarenkov, V. G. Nedorezov and N. V. Rudnev, “Fragmentation of light nuclei by intermediate energy photons,” Phys. Part. Nucl. 48, no. 1, 95 (2017). doi:10.1134/S1063779617010166 8/5 = 1.6
[12] V. L. Kashevarov, ..., A. Mushkarenkov et al. [A2 Collaboration], “Study of ? and ?0 Photoproduction at MAMI,” Phys. Rev. Lett. 118, no. 21, 212001 (2017) doi:10.1103/PhysRevLett.118.212001 [arXiv:1701.04809 [nucl-ex]]. 8.839*30*0.075 = 19.888 [13] P. Adlarson, ..., A. Mushkarenkov et al. [A2 Collaboration], “Measurement of the ?0 > e+e?? Dalitz decay at the Mainz Microtron,” Phys. Rev. C 95, no. 2, 025202 (2017) doi:10.1103/PhysRevC.95.025202 [arXiv:1611.04739 [hep-ex]]. 3.304*30*0.075 = 7.434
[14] V. Sokhoyan, ..., A. Mushkarenkov et al. [A2 Collaboration], “Determination of the scalar polarizabilitiesoftheprotonusingbeamasymmetry ?3 inComptonscattering,” Eur.Phys. J. A 53, no. 1, 14 (2017) doi:10.1140/epja/i2017-12203-0 [arXiv:1611.03769 [nucl-ex]]. 2.799*30*0.075 = 6.298 [15] P. Adlarson, ..., A. Mushkarenkov et al., “Measurement of the ? > ?0e+e? and ? > e+e?? Dalitz decays with the A2 setup at MAMI,” Phys. Rev. C 95, no. 3, 035208 (2017) doi:10.1103/PhysRevC.95.035208 [arXiv:1609.04503 [hep-ex]]. 3.304*30*0.075 = 7.434
ÈÒÎÃÎ: ÏÐÍÄ = 103.844