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
ÔÈÎÃÐÏÐÍÄäàòàäîëæí
Ñóâîðîâ Ñåðãåé Áîðèñîâè÷×763,219.01.2022Ñ
Ñóâîðîâ Ñåðãåé Áîðèñîâè÷ (ðîä. 21.08.1993) ÌÍÑ ËÔÝÑÂ ÎÔÂÝ
Ñóììàðíûé ÏÐÍÄ (çà 2020-2021 ã.ã.) = 763.172
ÏÐÍÄ ñêëàäûâàåòñÿ èç íèæåïåðå÷èñëåííûõ ôàêòîðîâ:
ÝËÅÊÒÐÎÍÍÛÅ ÏÐÅÏÐÈÍÒÛ:
1) K. Abe, ..., S. Suvorov, ... et al (389 authors) “The Hyper-Kamiokande Experiment - Snowmass LOI” e-Print: 2009.00794 ÏÐÍÄ=3*0.028=0.084 2) A. Ajmi, …, S. Suvorov et al (77 authors) “Baby MIND detector first physics run” e-Print: 2004.05245 ÏÐÍÄ=3*0.07=0.21 3) D. Gorbunov, … , S. Suvorov (3 authors) “Revisiting PS191 limits on sterile neutrinos” arXiv:2112.06800, 2021 ÏÐÍÄ=3*0.51=1.53 4) S. Dolan, …, S. Suvorov (18 authors) “Sensitivity of the Upgraded T2K Near Detector to constrain neutrino and anti-neutrino interactions with no mesons in the final state by exploiting nucleon-lepton correlations” e-Print: 2108.11779 ÏÐÍÄ=3*0.2=0.6
ÑÒÀÒÜÈ Â ÆÓÐÍÀËÀÕ: 5) D. Attie, … S. Suvorov, et al (61 authors) “Characterization of resistive Micromegas detectors for the upgrade of the T2K Near Detector Time Projection Chambers” Nucl.Instrum.Meth.A 1025 (2022) 166109 ÏÐÍÄ = 30*1.455*0.07 = 3.056 6) D. Gorbunov, … , S. Suvorov (3 authors) “Constraints on light scalars from PS191 results”
Phys.Lett.B 820 (2021) 136524 ÏÐÍÄ=30*4.036*0.51=61.751 7) D. Gorbunov, … , S. Suvorov (4 authors) “Double-hit signature of millicharged particles in 3D segmented neutrino detector” Phys.Lett.B 822 (2021) 136641 ÏÐÍÄ=30*4.036*0.51=61.751 8) K. Abe, ..., S. Suvorov, ... et al (311 authors) “First T2K measurement of transverse kinematic imbalance in the muon-neutrino chargedcurrent single-? production channel containing at least one proton” Phys.Rev.D 103 (2021) 11, 112009 ÏÐÍÄ=30*5.296*0.028=4.449 9) K. Abe, ..., S. Suvorov, ... et al (501 authors) “Supernova Model Discrimination with Hyper-Kamiokande” Astrophys.J. 916 (2021) 1, 15 ÏÐÍÄ=30*5.874*0.018=3.172 10) K. Abe, ..., S. Suvorov, ... et al (296 authors) “T2K measurements of muon neutrino and antineutrino disappearance using 3.13\times 10^{21} protons on target“ Phys. Rev. D 103, L011101 ÏÐÍÄ=30*5.296*0.028=4.449 11) K. Abe, ..., S. Suvorov, ... et al (369 authors) “Measurements of \bar{\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 ÏÐÍÄ=30*2.572*0.028=2.160 12) K. Abe, ..., S. Suvorov, ... et al (310 authors) “Improved constraints on neutrino mixing from the T2K experiment with 3.13?10^21 protons on target” Phys.Rev.D 103 (2021) 11, 112008 ÏÐÍÄ=30*5.296*0.028=4.449 13)A. Blondel, ..., S. Suvorov, ... et al (50 authors) “The SuperFGD Prototype Charged Particle Beam Tests” JINST 15 (2020) 12, P12003 ÏÐÍÄ = 30*1.415*0.07 = 2.971 14) D. Gorbunov, … , S. Suvorov (4 authors) “Heavy Neutral Leptons from kaon decays in the SHiP experiment” Physics Letters B Volume 810 ÏÐÍÄ = 30*5.296*0.25 = 35.783 15)K. Abe, ..., S. Suvorov, ... et al (333 authors) “Simultaneous measurement of the muon neutrino charged-current cross section on oxygen and carbon without pions in the final state at T2K” Phys. Rev. D 101, 112004 ÏÐÍÄ = 30*5.296*0.028 = 4.449 16)K. Abe, ..., S. Suvorov, ... et al (333 authors) “Measurement of the charged-current electron (anti-)neutrino inclusive cross-sections at the
T2K off-axis near detector ND280” JHEP 10 (2020) 114 ÏÐÍÄ = 30*5.810*0.028 = 4.880 17) K. Abe, ..., S. Suvorov, ... et al (352 authors) “First combined measurement of the muon neutrino and antineutrino charged-current cross section without pions in the final state at T2K” Phys.Rev.D 101 (2020) 11, 112001 ÏÐÍÄ = 30*5.296*0.028 = 4.449 18)L. Munteanu, S. Suvorov, et al (10 authors) “New method for an improved antineutrino energy reconstruction with charged-current interactions in next-generation detectors” Phys.Rev.D 101 (2020) 9, 092003 ÏÐÍÄ = 30*5.296*0.20 = 31.776 19)K. Abe, ..., S. Suvorov, ... et al (344 authors) “Search for Electron Antineutrino Appearance in a Long-baseline Muon Antineutrino Beam” Phys.Rev.Lett. 124 (2020) 16, 161802 ÏÐÍÄ = 30*9.161*0.028 = 7.695 20) K. Abe, ..., S. Suvorov, ... et al (335 authors) “Constraint on the matter–antimatter symmetry-violating phase in neutrino oscillations" Nature 580 (2020) 7803, 339-344, Nature 583 (2020) 7814, E16 (erratum) ÏÐÍÄ = 30*49.962*0.028 = 41.968 21)K. Abe, ..., S. Suvorov, ... et al (376 authors) “Measurement of the muon neutrino charged-current single \pi^+ production on hydrocarbon using the T2K off-axis near detector ND280” Phys.Rev.D 101 (2020) 1, 012007 ÏÐÍÄ = 30*5.296*0.028 = 4.449 22)K. Abe, ..., S. Suvorov, ... et al (325 authors) “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.D 102 (2020) 1, 012007 ÏÐÍÄ = 30*5.296*0.028 = 4.449 23)D. Attie, … S. Suvorov, et al (56 authors) “Performances of a resistive Micromegas module for the Time Projection Chambers of the T2K Near Detector upgrade” Nucl.Instrum.Meth.A 957 (2020) 163286 ÏÐÍÄ = 30*1.455*0.07 = 3.056

ÄÎÊËÀÄÛ ÍÀ ÊÎÍÔÅÐÅÍÖÈßÕ è ÒÐÓÄÛ ÊÎÍÔÅÐÅÍÖÈÉ:
1. S. Suvorov! "Performance of the Time Projection Chambers with resistive MicroMegas of the T2K near
detector upgrade” XIX International Workshop on Neutrino Telescopes 18–26 Feb 2021 ÏÐÍÄ = 25 2. “The T2K near detector upgrade” Blois 2021: 32nd Rencontres de Blois on "Particle Physics and Cosmology” 17–22 Oct 2021 Blois, France ÏÐÍÄ = 25
ÍÀÓ×ÍÎ-ÎÁÐÀÇÎÂÀÒÅËÜÍÛÉ ÊÓÐÑΠ1. Ðàçðàáîòêà êóðñà “Ââåäåíèå â ôèçèêó íåéòðèíî” ÏÐÍÄ = 30 2. ×òåíèå êóðñà “Ââåäåíèå â ôèçèêó íåéòðèíî” ÏÐÍÄ = 8
Ïîâûøàþùèé êîýôôèöèåíò 2 ïîñëå çàùèòû êàíäèäàòñêîé äèññåðòàöèè. Èòîãî çà 2020-2021 ã.ã.: ÏÐÍÄ=381.586* 2 =763.172