Ðåéòèíã (ÏÐÍÄ) ñîòðóäíèêîâ ÈßÈ ÐÀÍ ñåçîíà 2022 [312]
ïî ãðóïïàì: Òåîðåòè÷åñêàÿ ôèçèêà, ßäåðíàÿ ôèçèêà, Íåéòðèííàÿ ôèçèêà è ÊË, ôèçèêà ×àñòèö, Óñêîðèòåëüíàÿ ôèçèêà, Ìåæäèñöèïëèíàðíûå èññëåäîâàíèÿ
ïî äîëæíîñòÿì è ðåãèîíàì: Ìîñêâà, íàó÷íûå Ñîòðóäíèêè (ïî Óêàçó), íàó÷íûå Ðàáîòíèêè (âíå Óêàçà), Àñïèðàíòû, ñòóÄåíòû, âíåøíèå ñîâÌåñòèòåëè, Ñá...Ìá - òî æå äëÿ ÁÍÎ
| ÔÈÎ | ÃÐ | ÏÐÍÄ | äàòà | äîëæí |
| Ìåôîäüåâ Àëåêñàíäð Âëàäèìèðîâè÷ | × | 318,5 | 19.01.2022 | Ñ |
Ìåôîäüåâ Àëåêñàíäð Âëàäèìèðîâè÷
(ðîä. 25.10.1991)
Ìëàäøèé íàó÷íûé ñîòðóäíèê, ËÎÁÄ
Ñóììàðíûé ÏÐÍÄ (çà 2020 – 2021 ã.ã.) = 318,48108
ÏÐÍÄ ñêëàäûâàåòñÿ èç íèæåïåðå÷èñëåííûõ ôàêòîðîâ:
ÝËÅÊÒÐÎÍÍÛÅ ÏÐÅÏÐÈÍÒÛ:
1) A. Abed Abud,…, A. Mefodiev,… et al. (1177 àâò). Design, construction and operation of the ProtoDUNE-SP Liquid Argon TPC. arXiv:2108.01902 [physics.ins-det]. ÏÐÍÄ=3*0.012= 0.036;
2) B. Abi,…, A. Mefodiev,… et al. (973 àâò). Experiment simulation configurations approximating DUNE TDR. arXiv:2103.04797 [hep-ex]. ÏÐÍÄ=3*0.018= 0.054;
3) B. Abi,…, A. Mefodiev,… et al. (936 àâò). Deep Underground Neutrino Experiment (DUNE), Far Detector Technical Design Report, Volume II DUNE Physics. arXiv:2002.03005 [hep-ex]. ÏÐÍÄ=3*0.018= 0.054;
4) C. Ahdida, …, A. Mefodiev,… et al. (338 àâò). Track reconstruction and matching between emulsion and silicon pixel detectors for the SHiP-charm experiment. arXiv:2112.11754 [physics.ins-det]. ÏÐÍÄ=3*0.028= 0.084;
5) C. Ahdida, …, A. Mefodiev,… et al. (345 àâò). The SHiP experiment at the proposed CERN SPS Beam Dump Facility. arXiv: 2112.01487 [physics.ins-det]. ÏÐÍÄ=3*0.028= 0.084
6) A. Ajmi,…, A. Mefodiev,… et. Al (77 àâò). BabyMIND detector first physics run. arXiv:2004.05245 [physics.ins-det]. ÏÐÍÄ=3*0.07= 0.21;
7) C. Ahdida,…, A. Mefodiev,… et al. (343 àâò). SND@LHC. arXiv:2002.08722 [physics.ins-det]. ÏÐÍÄ=3*0.028= 0.084;
8) C. Ahdida,…, A. Mefodiev,… et al. (333 àâò). Measurement of the muon flux for the SHiP experiment. arXiv:2001.04784 [physics.ins-det]. ÏÐÍÄ=3*0.028= 0.084;
Ñóììà ïî ïðåïðèíòàì: 0,69
ÑÒÀÒÜÈ Â ÆÓÐÍÀËÀÕ:
1) A. Abed Abud,…, A. Mefodiev, … et al. (1181 àâò). Searching for solar KDAR with DUNE. JCAP 10 (2021) 065; DOI: 10.1088/1475-7516/2021/10/065 (arXiv:2107.09109 [hep-ex]). ÏÐÍÄ= 5.839*30*0.012= 2.10204;
2) A. Abed Abud,…, A. Mefodiev, … et al. (1086 àâò). Deep Underground Neutrino Experiment (DUNE) near detector conceptual design report. Instruments 5 (2021) 4, 31; DOI: 10.3390/instruments5040031 (arXiv: 2103.13910 [physics.ins-det]). ÏÐÍÄ= 8*0.012= 0.096;
3) K. Abe,…, A. Mefodiev, … et al. (311 àâò). First T2K measurement of transverse kinematic imbalance in the muon-neutrino charged-current single-?+ production channel containing at least one proton. Phys.Rev.D 103 (2021) 11, 112009; DOI: 10.1103/PhysRevD.103.112009 (arXiv:2102.03346 [hep-ex]). ÏÐÍÄ= 5.296*30*0.028= 4.44864;
4) K. Abe,…, A. Mefodiev, … et al. (501 àâò). Supernova model discrimination with Hyper-Kamiokande. Astrophys.J. 916 (2021) 1, 15; DOI: 10.3847/1538-4357/abf7c4 (arXiv:2101.05269 [astro-ph.IM]). ÏÐÍÄ= 5.874*30*0.018= 3.17196;
5) K. Abe,…, A. Mefodiev, … et al. (310 àâò). Improved constraints on neutrino mixing from the T2K experiment with 3.13?10^21 protons on target. Phys.Rev.D 103 (2021) 11, 112008; DOI: 10.1103/PhysRevD.103.112008 (arXiv:2101.03779 [hep-ex]). ÏÐÍÄ= 5.296**30*0.028= 4.44864;
6) B. Abi,…, A. Mefodiev,… et al. (975 àâò). Prospects for Beyond the Standard Model Physics Searches at the Deep Underground Neutrino Experiment. Eur.Phys.J.C 81 (2021) 4, 322; DOI: 10.1140/epjc/s10052-021-09007-w (arXiv:2008.12769 [hep-ex]). 4.590*30*0.018 = 2.4786;
7) A. Blondel,…, A. Mefodiev,… et al. (50 àâò). The SuperFGD charged particle beam tests. JINST 15 (2020) 12, P12003; DOI: 10.1088/1748-0221/15/12/P12003 (arXiv:2008.08861 [physics.ins-det]). ÏÐÍÄ= 1.415*30*0.07 = 2.9715;
8) K. Abe,…, A. Mefodiev,… et al. (297 àâò). T2K measurements of muon neutrino and antineutrino disappearance using 3.13 x 10^21 protons on target. Phys.Rev.D 103 (2021) 1, L011101; DOI: 10.1103/PhysRevD.103.L011101 (arXiv:2008.07921 [hep-ex]). ÏÐÍÄ= 5.296**30*0.028= 4.44864;
9) B. Abi,…, A. Mefodiev,… et al. (973 àâò). Supernova neutrino burst detection with the Deep Underground Neutrino Experiment. Eur.Phys.J.C 81 (2021) 5, 423; DOI: 10.1140/epjc/s10052-021-09166-w (arXiv: 2008.06647 [hep-ex]). ÏÐÍÄ= 4.590*30*0.018 = 2.4786;
10) B. Abi,…, A. Mefodiev,… et al. (992 àâò). First results on ProtoDUNE-SP liquid argon time projection chamber performance from a beam test at the CERN Neutrino Platform. JINST 15 (2020) 12, P12004; DOI: 10.1088/1748-0221/15/08/T08008 (arXiv:2007.06722 [physics.ins-det]). ÏÐÍÄ= 1.415*30*0.018 = 0.7641;
11) B. Abi,…, A. Mefodiev,… et al. (975 àâò). Neutrino interaction classification with a convolutional neural network in the DUNE far detector. Phys.Rev. D102 (2020) 9, 092003; DOI: 10.1103/PhysRevD.102.092003 (arXiv:2006.15052 [physics.ins-det]). ÏÐÍÄ= 5.296*30*0.018 = 2.85984;
12) B. Abi,…, A. Mefodiev,… et al. (973 àâò). Long-baseline neutrino oscillation physics potential of the DUNE experiment. Eur.Phys.J.C80 (2020) 10, 978; DOI: 10.1140/epjc/s10052-020-08456-z (arXiv:2006.16043 [hep-ex]). ÏÐÍÄ= 4.590*30*0.018 = 2.4786;
13) K. Abe,…, A. Mefodiev,… et al. (371 àâò). Measurements of $\bar\nu_mu$ and $\bar\nu_mu + \nu_mu$ charged-current cross sections without detected pions nor protons on water and hydrocarbon at mean antineutrino energy of 0.86 GeV. PTEP 2021 (2021) 4, 043C01; DOI: 10.1093/ptep/ptab014 (arXiv:2004.13989 [hep-ex]). ÏÐÍÄ= 2.572*30*0.028= 2.16048;
14) K. Abe,…, A. Mefodiev,… et al. (333 àâò). Simultaneous measurement of the muon neutrino charged-current cross section on oxygen and carbon without pions in the final state at T2K. Phys.Rev. D101 (2020) 11, 112004; DOI: 10.1103/PhysRevD.101.112004 (arXiv:2004.05434 [hep-ex]). ÏÐÍÄ= 5.296*30*0.028 = 4.44864;
15) K. Abe,…, A. Mefodiev,… et al. (369 àâò). Measurement of the charged-current electron (anti-)neutrino inclusive cross-sections at the T2K off-axis near detector ND280. JHEP 10 (2020) 114; DOI: 10.1007/JHEP10(2020)114 (arXiv:2002.11986 [hep-ex]). ÏÐÍÄ= 5.810*30*0.028 = 4.8804;
16) K. Abe,…, A. Mefodiev,… et al. (352 àâò). First combined measurement of the muon neutrino and antineutrino charged-current cross section without pions in the final state at T2K. Phys.Rev. D101 (2020) 11, 112001; DOI: 10.1103/PhysRevD.101.112001 (arXiv:2002.09323 [hep-ex]). ÏÐÍÄ= 5.296*30*0.028 = 4.44864;
17) B. Abi,…, A. Mefodiev,… et al. (936 àâò). Volume III. DUNE far detector technical coordination. JINST 15 (2020) 08, T08009; DOI: 10.1088/1748-0221/15/08/T08009 (arXiv:2002.03008 [physics.ins-det]). ÏÐÍÄ= 1.415*30*0.018 = 0.7641;
18) B. Abi,…, A. Mefodiev,… et al. (936 àâò). Volume I. Introduction to DUNE. JINST 15 (2020) 08, T08008; DOI: 10.1088/1748-0221/15/08/T08008 (arXiv:2002.02967 [physics.ins-det]). ÏÐÍÄ= 1.415*30*0.018 = 0.7641;
19) B. Abi,…, A. Mefodiev,… et al. (936 àâò). Volume IV. DUNE far detector single-phase technology. JINST 15 (2020) 08, T08010; DOI: 10.1088/1748-0221/15/08/T08010 (arXiv:2002.03010 [physics.ins-det]). ÏÐÍÄ= 1.415*30*0.018 = 0.7641;
20) K. Abe,…, A. Mefodiev,… et al. (344 àâò). Search for electron antineutrino appearance in a long-baseline muon antineutrino beam. Phys.Rev.Lett. 124 (2020) 16, 161802; DOI: 10.1103/PhysRevLett.124.161802. (1911.07283 [hep-ex]). ÏÐÍÄ= 9.161*30*0.028= 7.69524;
21) K. Abe,…, A. Mefodiev,… et al. (335 àâò). Constraint on the matter–antimatter symmetry-violating phase in neutrino oscillations. Nature 580 (2020) 7803, 339-344, Nature 583 (2020) 7814, E16 (erratum). DOI: 10.1038/s41586-020-2177-0, 10.1038/s41586-020-2415-5 (erratum). (e-Print: 1910.03887 [hep-ex]). ÏÐÍÄ= 49.962*30*0.028 = 41.96808;
22) K. Abe,…, A. Mefodiev,… et al. (376 àâò). Measurement of the muon neutrino charged-current single ??+ production on hydrocarbon using the T2K. Phys.Rev.D101 (2020) no.1, 012007. DOI: 10.1103/PhysRevD.101.012007. ÏÐÍÄ= 5.296*30*0.028 = 4.44864;
23) K. Abe,…, A. Mefodiev,… et al. (325 àâò). First measurement of the charged current $\overline{\nu}_{\mu}$ double differential cross section on a water target without pions in the final state. Phys. Rev.D102 (2020), no. 1, 012007. DOI:10.1103/PhysRevD.102.012007. ÏÐÍÄ= 5.296*30*0.028 = 4.44864;
24) Eduardo Cortina Gil, …, A. Mefodiev,… et al. (325 àâò). Search for Lepton Number and Flavor Violation in K+ and ?0 Decays. Phys.Rev.Lett. 127 (2021) 13, 131802. DOI: 10.1103/PhysRevLett.127.131802 ÏÐÍÄ= 9.161*30*0.028= 7.69524;
25) Eduardo Cortina Gil, …, A. Mefodiev,… et al. (203 àâò). Measurement of the very rare K^{+} >{\pi}^{+}\nu \overline{\nu} decay. JHEP 06 (2021) 093. DOI: 10.1007/JHEP06(2021)093 (e-Print: 2103.15389 [hep-ex]) ÏÐÍÄ= 5.810*30*0.028= 4.8804
26) Eduardo Cortina Gil, …, A. Mefodiev,… et al. (202 àâò). Search for K+ decays to a muon and invisible particles. Phys.Lett.B 816 (2021) 136259. DOI: 10.1016/j.physletb.2021.136259 (e-Print: 2101.12304 [hep-ex]). ÏÐÍÄ= 4.771 *30*0.028= 4.00764
27) Eduardo Cortina Gil, …, A. Mefodiev,… et al. (200 àâò). Search for a feebly interacting particle XX in the decay K^{+}\rightarrow\pi^{+}X. JHEP 03 (2021) 058. DOI: 10.1007/JHEP03(2021)058. (e-Print: 2011.11329 [hep-ex]). ]) ÏÐÍÄ=5.810*30*0.028=4.8804
28) C. Ahdida,…, A. Mefodiev,… et al. (333 àâò). Sensitivity of the SHiP experiment to dark photons decaying to a pair of charged particles. Eur.Phys.J.C 81 (2021) 5, 451; DOI: 10.1140/epjc/s10052-021-09224-3 (arXiv:2011.05115 [hep-ex]). ÏÐÍÄ= 4.590*30*0.028= 3.8556;
29) C. Ahdida,…, A. Mefodiev,… et al. (338 àâò). Sensitivity of the SHiP experiment to light dark matter. JHEP 04 (2021) 199; DOI: 10.1007/JHEP04(2021)199 (arXiv:2010.11057 [hep-ex]). ÏÐÍÄ= 5.810*30*0.028= 4.8804;
30) Eduardo Cortina Gil, …, A. Mefodiev,… et al. (200 àâò). Search for \pi^0 decays to invisible particles. JHEP 02 (2021) 201. DOI: 10.1007/JHEP02(2021)201. (e-Print: 2010.07644 [hep-ex]). ÏÐÍÄ= 5.810*30*0.028=4.8804
31) Eduardo Cortina Gil, …, A. Mefodiev,… et al. (200 àâò). An investigation of the very rare {K}^{+}\to {\pi}^{+}\nu \overline{\nu} decay. JHEP 11 (2020) 042. DOI:10.1007/JHEP11(2020)042. (e-Print: 2007.08218 [hep-ex]) ÏÐÍÄ= 5.810*30*0.028=4.8804
32) Eduardo Cortina Gil, …, A. Mefodiev,… et al. (202 àâò). Search for heavy neutral lepton production in K+ decays to positrons. Phys.Lett.B 807 (2020) 135599. DOI: 10.1016/j.physletb.2020.135599. (e-Print: 2005.09575 [hep-ex]). ÏÐÍÄ= 4.771 *30*0.028= 4.00764
33) C. Ahdida,…, A. Mefodiev,… et al. (332 àâò). Measurement of the muon flux from 400 GeV/c protons interacting in a thick molybdenum/tungsten target. Eur.Phys.J.C 80 (2020) 3, 284; DOI: 10.1140/epjc/s10052-020-7788-y. ÏÐÍÄ= 4.590*30*0.028 = 3.8556;
34) C. Ahdida,…, A. Mefodiev,… et al. (332 àâò). The magnet of the scattering and neutrino detector for the SHiP experiment at CERN. JINST 15 (2020) 01, P01027. DOI: 10.1088/1748-0221/15/01/P01027. (e-Print: 1910.02952 [physics.ins-det]). ]). ÏÐÍÄ= 1.415*30*0.028 =1,1886
Ñóììà ïî ñòàòüÿì â ðåôåðèðóåìûõ æóðíàëàõ: 158.55054
ÄÎÊËÀÄÛ ÍÀ ÊÎÍÔÅÐÅÍÖÈßÕ è ÒÐÓÄÛ ÊÎÍÔÅÐÅÍÖÈÉ:
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ÏÎÂÛØÀÞÙÈÉ ÁÀË ÇÀ ÇÀÙÈÒÓ ÊÀÍÄÈÄÀÒÑÊÎÉ ÄÈÑÑÅÐÒÀÖÈÈ
23.12.2021 â äèññåðòàöèîííîì ñîâåòå ÈßÈ ÐÀÍ çàùèòèë êàíäèäàòñêóþ äèññåðòàöèþ íà òåìó "Ðàçðàáîòêà è ñîçäàíèå ìàãíèòíîãî íåéòðèííîãî äåòåêòîðà Baby MIND" ïî ñïåöèàëüíîñòè 01.04.01 - "ïðèáîðû è ìåòîäû ýêñïåðèìåíòàëüíîé ôèçèêè" – ïîâûøàþùèé êîýôôèöèåíò 2.0 (äëÿ ñîòðóäíèêîâ äî 40 ëåò â ãîä ïîñëå çàùèòû êàíäèäàòñêîé äèññåðòàöèè)
Èòîãî çà 2020-2020 ã.ã.: ÏÐÍÄ= (158.55054 + 0.69)*2 = 318,48108