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
Ìóñèåíêî Þðèé Âàñèëüåâè÷×241,119.01.2022Ñ
Ìóñèåíêî Þðèé Âàñèëüåâè÷, ðîä. 07.02.1962, ñíñ ËÔÝÑÂ ÎÔÂÝ
Ñóììàðíûé ÏÐÍÄ (çà 2020-2021 ãã.) = 241.136
Ñòàòüè:
1. M. Lucchini. Yu. Musienko, A. Heering "Experimental method to monitor temperature stability of SiPMs operating in conditions of extremely high dark count rate", Nucl.Instrum.Meth.A 977 (2020) 164300, ÏÐÍÄ = 1,455*30*0,51 = 22.262
2. Yu. Musienko, A. Heering, A. Karneyeu, M. Wayne, “Change of SiPM parameters after very high neutron irradiation” // JINST 15: 09, C09036, 2020. doi: 10.1088/1748-0221/15/09/C09036. ÏÐÍÄ = 1,415*30*0,430 = 18,254
3. Abbott R. et al. (CMS MTD Collaboration). Test beam characterization of sensor prototypes for the CMS Barrel MIP Timing Detector // JINST 16: 07, P07023, 2021. DOI: 10.1088/1748-0221/16/07/P07023. ÏÐÍÄ = 1,415*30*0,047 = 2,00
4. Acar B. et al. (CMS HGCAL Collaboration). The DAQ system of the 12,000 channel CMS high granularity calorimeter prototype // JINST 16: 04, T04001, 2021. DOI: 10.1088/1748-0221/16/04/T04001. ÏÐÍÄ = 1,415*30*0,028 = 1,19
Ñóììàðíûé ÏÐÍÄ ïî ñòàòüÿì/ïðåïðèíòàì íå CMS = 43.706

Äîêëàäû íà êîíôåðåíöèÿõ è òðóäû êîíôåðåíöèé:
1. Yu. Musienko, A. Heering, A. Karneyeu, M. Wayne, Change of SiPM parameters after very high neutron irradiation // The International Conference "Instrumentation for Colliding Beam Physics" (INSTR20), Budker INP, Novosibirsk, Russia, 24-28 February 2020, plenary talk. https://indico.inp.nsk.su/event/20/contributions , ÏÐÍÄ = 10 + 15*0,43 = 16,45
2. Heering A., Musienko Yu., Karneyeu A., Wayne M., Ruchti R., Gutierrez G.R. Integration of mini TECs on the CMS MTD barrel timing layer 16 ch SiPM array to reduce the DCR after very high irradiation // CPAD Instrumentation Frontier Workshop 2021, CFNS, Stony Brook University, USA, 18-22 March, 2021, óñòíûé. https://indico.fnal.gov/event/46746/. ÏÐÍÄ = 15*0,30 = 4,50
Ñóììàðíûé ÏÐÍÄ ïî äîêëàäàì = 20.95

Ñòàòüè CMS:
Ñòàòüè:
1. Tumasyan A. et al. (CMS Collaboration). Observation of tW production in the single-lepton channel in pp collisions at $ \sqrt{s} $ = 13 TeV // JHEP 11: 111, 2021. DOI: 10.1007/JHEP11(2021)111. ÏÐÍÄ = 5,810*30*0,007 = 1,22
2. Tumasyan A. et al. (CMS Collaboration). Measurement of differential $t \bar t$ production cross sections in the full kinematic range using lepton+jets events from proton-proton collisions at $\sqrt {s}$ = 13 TeV // Phys.Rev.D104: 9, 092013, 2021. DOI: 10.1103/PhysRevD.104.092013. ÏÐÍÄ = 5,296*30*0,007 = 1,11
3. Lee K. et al. (CMS Collaboration). Probing effective field theory operators in the associated production of top quarks with a Z boson in multilepton final states at $ \sqrt{s} $ = 13 TeV // JHEP 12: 83, 2021. DOI: 10.1007/JHEP12(2021)083. ÏÐÍÄ = 5,810*30*0,007 = 1,22
4. Tumasyan A. et al. (CMS Collaboration). Search for new particles in events with energetic jets and large missing transverse momentum in proton-proton collisions at $ \sqrt{s} $ = 13 TeV // JHEP 11: 153, 2021. DOI: 10.1007/JHEP11(2021)153. ÏÐÍÄ = 5,810*30*0,007 = 1,22
5. Tumasyan A. et al. (CMS Collaboration). Search for chargino-neutralino production in events with Higgs and W bosons using 137 fb$^{-1}$ of proton-proton collisions at $\sqrt{s} =$ 13 TeV // JHEP 10: 45, 2021. DOI: 10.1007/JHEP10(2021)045. ÏÐÍÄ = 5,810*30*0,007 = 1,22
6. Tumasyan A. et al. (CMS Collaboration). Combined searches for the production of supersymmetric top quark partners in proton–proton collisions at $\sqrt{s} = 13\,\text {Te}\text {V} $ // Eur.Phys.J.C81: 11, 970, 2021. DOI: 10.1140/epjc/s10052-021-09721-5. ÏÐÍÄ = 4,590*30*0,007 = 0,96
7. Tumasyan A. et al. (CMS Collaboration). Measurement of prompt open-charm production cross sections in proton-proton collisions at $ \sqrt{s} $ = 13 TeV // JHEP 11: 225, 2021. DOI: 10.1007/JHEP11(2021)225. ÏÐÍÄ = 5,810*30*0,007 = 1,22
8. Tumasyan A. et al. (CMS Collaboration). Measurements of the Electroweak Diboson Production Cross Sections in Proton-Proton Collisions at s=5.02 TeV Using Leptonic Decays // Phys.Rev.Lett. 127: 19, 191801, 2021. DOI: 10.1103/PhysRevLett.127.191801. ÏÐÍÄ = 9,161*30*0,007 = 1,92
9. Tumasyan A. et al. (CMS Collaboration). Measurement of the electroweak production of Z$\gamma$ and two jets in proton-proton collisions at $\sqrt{s} =$ 13 TeV and constraints on anomalous quartic gauge couplings // Phys.Rev.D104: 72001, 2021. DOI: 10.1103/PhysRevD.104.072001. ÏÐÍÄ = 5,296*30*0,007 = 1,11
10. Tumasyan A. et al. (CMS Collaboration). Search for a heavy Higgs boson decaying into two lighter Higgs bosons in the $\tau\tau$bb final state at 13 TeV // JHEP 11: 57, 2021. DOI: 10.1007/JHEP11(2021)057. ÏÐÍÄ = 5,810*30*0,007 = 1,22
11. Tumasyan A. et al. (CMS Collaboration). Study of Z boson plus jets events using variables sensitive to double-parton scattering in pp collisions at 13 TeV // JHEP 10: 176, 2021. DOI: 10.1007/JHEP10(2021)176. ÏÐÍÄ = 5,810*30*0,007 = 1,22
12. Tumasyan A. et al. (CMS Collaboration). Measurements of the pp $\to$ W$^\pm\gamma\gamma$ and pp $\to$ Z$\gamma\gamma$ cross sections at $\sqrt{s} =$ 13 TeV and limits on anomalous quartic gauge couplings // JHEP 10: 174, 2021. DOI: 10.1007/JHEP10(2021)174. ÏÐÍÄ = 5,810*30*0,007 = 1,22
13. Sirunyan A. et al. (CMS Collaboration). Search for lepton-flavor violating decays of the Higgs boson in the $\mu\tau$ and e$\tau$ final states in proton-proton collisions at $\sqrt{s}$ = 13 TeV // Phys.Rev.D104: 3, 032013, 2021. DOI: 10.1103/PhysRevD.104.032013. ÏÐÍÄ = 5,296*30*0,007 = 1,11
14. Sirunyan A. et al. (CMS Collaboration). Search for long-lived particles decaying to jets with displaced vertices in proton-proton collisions at $\sqrt{s}=$ 13 TeV // Phys.Rev.D104: 5, 052011, 2021. DOI: 10.1103/PhysRevD.104.052011. ÏÐÍÄ = 5,296*30*0,007 = 1,11
15. Sirunyan A. et al. (CMS Collaboration). Search for a heavy resonance decaying to a top quark and a W boson at $\sqrt{s} =$ 13 TeV in the fully hadronic final state // JHEP 12: 106, 2021. DOI: 10.1007/JHEP12(2021)106. ÏÐÍÄ = 5,810*30*0,007 = 1,22
16. Sirunyan A. et al. (CMS Collaboration). Constraints on anomalous Higgs boson couplings to vector bosons and fermions in its production and decay using the four-lepton final state // Phys.Rev.D104: 5, 052004, 2021. DOI: 10.1103/PhysRevD.104.052004. ÏÐÍÄ = 5,296*30*0,007 = 1,11
17. Sirunyan A. et al. (CMS Collaboration). Search for W' bosons decaying to a top and a bottom quark at s=13TeV in the hadronic final state // Phys.Lett.B820: 136535, 2021. DOI: 10.1016/j.physletb.2021.136535. ÏÐÍÄ = 4,771*30*0,007 = 1,00
18. Sirunyan A. et al. (CMS Collaboration). Search for charged Higgs bosons produced in vector boson fusion processes and decaying into vector boson pairs in proton–proton collisions at $\sqrt{s} = 13\,{\text {TeV}} $ // Eur.Phys.J.C81: 8, 723, 2021. DOI: 10.1140/epjc/s10052-021-09472-3. ÏÐÍÄ = 4,590*30*0,007 = 0,96
19. Sirunyan A. et al. (CMS Collaboration). Precision luminosity measurement in proton-proton collisions at $\sqrt{s} =$ 13 TeV in 2015 and 2016 at CMS // Eur.Phys.J.C81: 9, 800, 2021. DOI: 10.1140/epjc/s10052-021-09538-2. ÏÐÍÄ = 4,590*30*0,007 = 0,96
20. Sirunyan A. et al. (CMS Collaboration). Constraints on the Initial State of Pb-Pb Collisions via Measurements of $Z$-Boson Yields and Azimuthal Anisotropy at $\sqrt {s_{NN}}$=5.02 TeV // Phys.Rev.Lett. 127: 10, 102002, 2021. DOI: 10.1103/PhysRevLett.127.102002. ÏÐÍÄ = 9,161*30*0,007 = 1,92
21. Sirunyan A. et al. (CMS Collaboration). Measurements of Higgs boson production cross sections and couplings in the diphoton decay channel at $ \sqrt{\mathrm{s}} $ = 13 TeV // JHEP 7: 27, 2021. DOI: 10.1007/JHEP07(2021)027. ÏÐÍÄ = 5,810*30*0,007 = 1,22
22. Sirunyan A. et al. (CMS Collaboration). Measurements of production cross sections of the Higgs boson in the four-lepton final state in proton–proton collisions at $\sqrt{s} = 13\,\text {Te}\text {V} $ // Eur.Phys.J.C81: 6, 488, 2021. DOI: 10.1140/epjc/s10052-021-09200-x. ÏÐÍÄ = 4,590*30*0,007 = 0,96
23. Sirunyan A. et al. (CMS Collaboration). Search for resonant and nonresonant new phenomena in high-mass dilepton final states at $ \sqrt{s} $ = 13 TeV // JHEP 7: 208, 2021. DOI: 10.1007/JHEP07(2021)208. ÏÐÍÄ = 5,810*30*0,007 = 1,22
24. Sirunyan A. et al. (CMS Collaboration). Search for top squark production in fully-hadronic final states in proton-proton collisions at $\sqrt{s} =$ 13 TeV // Phys.Rev.D104: 5, 052001, 2021. DOI: 10.1103/PhysRevD.104.052001. ÏÐÍÄ = 5,296*30*0,007 = 1,11
25. Sirunyan A. et al. (CMS Collaboration). Study of Drell-Yan dimuon production in proton-lead collisions at $\sqrt{s_\mathrm{NN}} =$ 8.16 TeV // JHEP 5: 182, 2021. DOI: 10.1007/JHEP05(2021)182. ÏÐÍÄ = 5,810*30*0,007 = 1,22
26. Sirunyan A. et al. (CMS Collaboration). First measurement of large area jet transverse momentum spectra in heavy-ion collisions // JHEP 5: 284, 2021. DOI: 10.1007/JHEP05(2021)284. ÏÐÍÄ = 5,810*30*0,007 = 1,22
27. Sirunyan A. et al. (CMS Collaboration). Measurements of angular distance and momentum ratio distributions in three-jet and Z + two-jet final states in pp collisions // Eur.Phys.J.C81: 852, 2021. DOI: 10.1140/epjc/s10052-021-09570-2. ÏÐÍÄ = 4,590*30*0,007 = 0,96
28. Sirunyan A. et al. (CMS Collaboration). Search for a heavy vector resonance decaying to a ${\mathrm{Z}}_{\mathrm{}}^{\mathrm{}}$ boson and a Higgs boson in proton-proton collisions at $\sqrt{s} = 13\,\text {Te}\text {V} $ // Eur.Phys.J.C81: 8, 688, 2021. DOI: 10.1140/epjc/s10052-021-09348-6. ÏÐÍÄ = 4,590*30*0,007 = 0,96
29. Sirunyan A. et al. (CMS Collaboration). Search for top squarks in final states with two top quarks and several light-flavor jets in proton-proton collisions at $\sqrt {s}$ = 13 TeV // Phys.Rev.D104: 3, 032006, 2021. DOI: 10.1103/PhysRevD.104.032006. ÏÐÍÄ = 5,296*30*0,007 = 1,11
30. Sirunyan A. et al. (TOTEM and CMS Collaborations). Hard color-singlet exchange in dijet events in proton-proton collisions at $\sqrt{s} =$ 13 TeV // Phys.Rev.D104: 32009, 2021. DOI: 10.1103/PhysRevD.104.032009. ÏÐÍÄ = 5,296*30*0,007 = 1,11
31. Sirunyan A. et al. (CMS Collaboration). Performance of the CMS muon trigger system in proton-proton collisions at $\sqrt{s} =$ 13 TeV // JINST 16: P07001, 2021. DOI: 10.1088/1748-0221/16/07/P07001. ÏÐÍÄ = 1,415*30*0,007 = 0,30
32. Sirunyan A. et al. (CMS Collaboration). Observation of a New Excited Beauty Strange Baryon Decaying to$\Xi^-_\mathrm{b} \pi^+ \pi^-$ // Phys.Rev.Lett. 126: 25, 252003, 2021. DOI: 10.1103/PhysRevLett.126.252003. ÏÐÍÄ = 9,161*30*0,007 = 1,92
33. Sirunyan A. et al. (CMS Collaboration). Measurement of the W$\gamma$ Production Cross Section in Proton-Proton Collisions at $\sqrt {s}$=13 TeV and Constraints on Effective Field Theory Coefficients // Phys.Rev.Lett. 126: 25, 252002, 2021. DOI: 10.1103/PhysRevLett.126.252002. ÏÐÍÄ = 9,161*30*0,007 = 1,92
34. Sirunyan A. et al. (CMS Collaboration). Measurements of the differential cross sections of the production of Z + jets and $\gamma$ + jets and of Z boson emission collinear with a jet in pp collisions at $ \sqrt{s} $ = 13 TeV // JHEP 5: 285, 2021. DOI: 10.1007/JHEP05(2021)285. ÏÐÍÄ = 5,810*30*0,007 = 1,22
35. Sirunyan A. et al. (CMS Collaboration). In-medium modification of dijets in PbPb collisions at $ \sqrt{s_{\mathrm{NN}}} $ = 5.02 TeV // JHEP 5: 116, 2021. DOI: 10.1007/JHEP05(2021)116. ÏÐÍÄ = 5,810*30*0,007 = 1,22
36. Sirunyan A. et al. (CMS Collaboration). Measurement of the Z boson differential production cross section using its invisible decay mode (Z$\nu\bar{\nu}$) in proton-proton collisions at $\sqrt{s}=$ 13 TeV // JHEP 5: 205, 2021. DOI: 10.1007/JHEP05(2021)205. ÏÐÍÄ = 5,810*30*0,007 = 1,22
37. Sirunyan A. et al. (CMS Collaboration). First measurement of the cross section for top quark pair production with additional charm jets using dileptonic final states in pp collisions at s=13TeV // Phys.Lett.B820: 136565, 2021. DOI: 10.1016/j.physletb.2021.136565. ÏÐÍÄ = 4,771*30*0,007 = 1,00
38. Sirunyan A. et al. (CMS Collaboration). Search for supersymmetry in final states with two oppositely charged same-flavor leptons and missing transverse momentum in proton-proton collisions at $\sqrt{s} =$ 13 TeV // JHEP 4: 123, 2021. DOI: 10.1007/JHEP04(2021)123. ÏÐÍÄ = 5,810*30*0,007 = 1,22
39. Sirunyan A. et al. (CMS Collaboration). Electron and photon reconstruction and identification with the CMS experiment at the CERN LHC // JINST 16: 05, P05014, 2021. DOI: 10.1088/1748-0221/16/05/P05014. ÏÐÍÄ = 1,415*30*0,007 = 0,30
40. Sirunyan A. et al. (CMS Collaboration). Search for singly and pair-produced leptoquarks coupling to third-generation fermions in proton-proton collisions at s=13 TeV // Phys.Lett.B819: 136446, 2021. DOI: 10.1016/j.physletb.2021.136446. ÏÐÍÄ = 4,771*30*0,007 = 1,00
41. Sirunyan A. et al. (CMS Collaboration). Search for new physics in top quark production with additional leptons in proton-proton collisions at $\sqrt{s} = $ 13 TeV using effective field theory // JHEP 3: 95, 2021. DOI: 10.1007/JHEP03(2021)095. ÏÐÍÄ = 5,810*30*0,007 = 1,22
42. Sirunyan A. et al. (CMS Collaboration). Measurement of differential cross sections for Z bosons produced in association with charm jets in pp collisions at $\sqrt{s} =$ 13 TeV // JHEP 4: 109, 2021. DOI: 10.1007/JHEP04(2021)109. ÏÐÍÄ = 5,810*30*0,007 = 1,22
43. Sirunyan A. et al. (CMS Collaboration). Search for long-lived particles using displaced jets in proton-proton collisions at $\sqrt{s} = $ 13 TeV // Phys.Rev.D104: 1, 012015, 2021. DOI: 10.1103/PhysRevD.104.012015. ÏÐÍÄ = 5,296*30*0,007 = 1,11
44. Sirunyan A. et al. (CMS Collaboration). Search for nonresonant Higgs boson pair production in final states with two bottom quarks and two photons in proton-proton collisions at $ \sqrt{s} $ = 13 TeV // JHEP 3: 257, 2021. DOI: 10.1007/JHEP03(2021)257. ÏÐÍÄ = 5,810*30*0,007 = 1,22
45. Sirunyan A. et al. (CMS Collaboration). Search for the rare decay of the W boson into a pion and a photon in proton-proton collisions at s=13TeV // Phys.Lett.B819: 136409, 2021. DOI: 10.1016/j.physletb.2021.136409. ÏÐÍÄ = 4,771*30*0,007 = 1,00
46. Sirunyan A. et al. (CMS Collaboration). Observation of Forward Neutron Multiplicity Dependence of Dimuon Acoplanarity in Ultraperipheral Pb-Pb Collisions at $\sqrt{s_{NN}}$=5.02 TeV // Phys.Rev.Lett. 127: 12, 122001, 2021. DOI: 10.1103/PhysRevLett.127.122001. ÏÐÍÄ = 9,161*30*0,007 = 1,92
47. Sirunyan A. et al. (CMS Collaboration). Measurement of the Higgs boson production rate in association with top quarks in final states with electrons, muons, and hadronically decaying tau leptons at $\sqrt{s} =$ 13 TeV // Eur.Phys.J.C81: 4, 378, 2021. DOI: 10.1140/epjc/s10052-021-09014-x. ÏÐÍÄ = 4,590*30*0,007 = 0,96
48. Sirunyan A. et al. (CMS Collaboration). Development and validation of HERWIG 7 tunes from CMS underlying-event measurements // Eur.Phys.J.C81: 4, 312, 2021. DOI: 10.1140/epjc/s10052-021-08949-5. ÏÐÍÄ = 4,590*30*0,007 = 0,96
49. Khachatryan V. et al. (CMS Collaboration). The very forward CASTOR calorimeter of the CMS experiment // JINST 16: 02, P02010, 2021. DOI: 10.1088/1748-0221/16/02/P02010. ÏÐÍÄ = 1,415*30*0,007 = 0,30
50. Sirunyan A. et al. (CMS Collaboration). Angular analysis of the decay B$^+$ $\to$ K$^*$(892)$^+\mu^+\mu^-$ in proton-proton collisions at $\sqrt{s} =$ 8 TeV // JHEP 4: 124, 2021. DOI: 10.1007/JHEP04(2021)124. ÏÐÍÄ = 5,810*30*0,007 = 1,22
51. Sirunyan A. et al. (CMS Collaboration). MUSiC: a model-unspecific search for new physics in proton–proton collisions at $\sqrt{s} = 13\,\text {TeV} $ // Eur.Phys.J.C81: 7, 629, 2021. DOI: 10.1140/epjc/s10052-021-09236-z. ÏÐÍÄ = 4,590*30*0,007 = 0,96
52. Sirunyan A. et al. (CMS Collaboration). Search for dark photons in Higgs boson production via vector boson fusion in proton-proton collisions at $ \sqrt{s} $ = 13 TeV // JHEP 3: 11, 2021. DOI: 10.1007/JHEP03(2021)011. ÏÐÍÄ = 5,810*30*0,007 = 1,22
53. Sirunyan A. et al. (CMS Collaboration). Measurement of prompt ${\mathrm{D^0}}$ and ${\mathrm{\overline{D}}{}^0}$ meson azimuthal anisotropy and search for strong electric fields in PbPb collisions at $\sqrt{s_\mathrm{NN}} =$ 5.02 TeV // Phys.Lett.B816: 136253, 2021. DOI: 10.1016/j.physletb.2021.136253. ÏÐÍÄ = 4,771*30*0,007 = 1,00
54. Sirunyan A. et al. (CMS Collaboration). Measurements of production cross sections of polarized same-sign W boson pairs in association with two jets in proton-proton collisions at $\sqrt{s} =$ 13 TeV // Phys.Lett.B812: 136018, 2021. DOI: 10.1016/j.physletb.2020.136018. ÏÐÍÄ = 4,771*30*0,007 = 1,00
55. Sirunyan A. et al. (CMS Collaboration). Measurement of the top quark Yukawa coupling from $\mathrm{t\bar{t}}$ kinematic distributions in the dilepton final state in proton-proton collisions at $\sqrt{s}=$ 13 TeV // Phys.Rev.D102: 9, 092013, 2020. DOI: 10.1103/PhysRevD.102.092013. ÏÐÍÄ = 5,296*30*0,007 = 1,11
56. Sirunyan A. et al. (CMS Collaboration). Studies of charm and beauty hadron long-range correlations in pp and pPb collisions at LHC energies // Phys.Lett.B813: 136036, 2021. DOI: 10.1016/j.physletb.2020.136036. ÏÐÍÄ = 4,771*30*0,007 = 1,00
57. Sirunyan A. et al. (CMS Collaboration). Evidence for Higgs boson decay to a pair of muons // JHEP 1: 148, 2021. DOI: 10.1007/JHEP01(2021)148. ÏÐÍÄ = 5,810*30*0,007 = 1,22
58. Sirunyan A. et al. (CMS Collaboration). Measurements of ${\mathrm{p}} {\mathrm{p}} \rightarrow {\mathrm{Z}} {\mathrm{Z}} $ production cross sections and constraints on anomalous triple gauge couplings at $\sqrt{s} = 13\,\text {TeV} $ // Eur.Phys.J.C81: 3, 200, 2021. DOI: 10.1140/epjc/s10052-020-08817-8. ÏÐÍÄ = 4,590*30*0,007 = 0,96
59. Sirunyan A. et al. (CMS Collaboration). W$^+$W$^-$ boson pair production in proton-proton collisions at $\sqrt{s} =$ 13 TeV // Phys.Rev.D102: 9, 092001, 2020. DOI: 10.1103/PhysRevD.102.092001. ÏÐÍÄ = 5,296*30*0,007 = 1,11
60. Sirunyan A. et al. (CMS Collaboration). Observation of electroweak production of W$\gamma$ with two jets in proton-proton collisions at $\sqrt {s}$ = 13 TeV // Phys.Lett.B811: 135988, 2020. DOI: 10.1016/j.physletb.2020.135988. ÏÐÍÄ = 4,771*30*0,007 = 1,00
61. Sirunyan A. et al. (CMS Collaboration). A search for bottom-type, vector-like quark pair production in a fully hadronic final state in proton-proton collisions at $\sqrt{s} =$ 13 TeV // Phys.Rev.D102: 112004, 2020. DOI: 10.1103/PhysRevD.102.112004. ÏÐÍÄ = 5,296*30*0,007 = 1,11
62. Sirunyan A. et al. (CMS Collaboration). Measurement of B$_\mathrm{c}$(2S)$^+$ and B$_\mathrm{c}^*$(2S)$^+$ cross section ratios in proton-proton collisions at $\sqrt{s} =$ 13 TeV // Phys.Rev.D102: 9, 092007, 2020. DOI: 10.1103/PhysRevD.102.092007. ÏÐÍÄ = 5,296*30*0,007 = 1,11
63. Sirunyan A. et al. (CMS Collaboration). Measurement of differential $\mathrm{t\bar{t}}$ production cross sections using top quarks at large transverse momenta in $pp$ collisions at $\sqrt{s} =$ 13 TeV // Phys.Rev.D103: 5, 052008, 2021. DOI: 10.1103/PhysRevD.103.052008. ÏÐÍÄ = 5,296*30*0,007 = 1,11
64. Sirunyan A. et al. (CMS Collaboration). Evidence for electroweak production of four charged leptons and two jets in proton-proton collisions at $\sqrt {s}$ = 13 TeV // Phys.Lett.B812: 135992, 2021. DOI: 10.1016/j.physletb.2020.135992. ÏÐÍÄ = 4,771*30*0,007 = 1,00
65. Sirunyan A. et al. (CMS Collaboration). Search for top squark pair production using dilepton final states in ${\text {p}}{\text {p}}$ collision data collected at $\sqrt{s}=13\,\text {TeV} $ // Eur.Phys.J.C81: 1, 3, 2021. DOI: 10.1140/epjc/s10052-020-08701-5. ÏÐÍÄ = 4,590*30*0,007 = 0,96
66. Sirunyan A. et al. (CMS Collaboration). Search for dark matter produced in association with a leptonically decaying Z boson in proton-proton collisions at $\sqrt{s} =$ 13 TeV // Eur.Phys.J.C81: 1, 13, 2021. DOI: 10.1140/epjc/s10052-020-08739-5. ÏÐÍÄ = 4,590*30*0,007 = 0,96
67. Sirunyan A. et al. (CMS Collaboration). Search for supersymmetry in proton-proton collisions at $\sqrt{s} =$ 13 TeV in events with high-momentum Z bosons and missing transverse momentum // JHEP 9: 149, 2020. DOI: 10.1007/JHEP09(2020)149. ÏÐÍÄ = 5,810*30*0,007 = 1,22
68. Sirunyan A. et al. (CMS Collaboration). Measurements of the $W$ boson rapidity, helicity, double-differential cross sections, and charge asymmetry in $pp$ collisions at $\sqrt {s}$ = 13 TeV // Phys.Rev.D102: 9, 092012, 2020. DOI: 10.1103/PhysRevD.102.092012. ÏÐÍÄ = 5,296*30*0,007 = 1,11
69. Sirunyan A. et al. (CMS Collaboration). Search for the lepton flavor violating decay $\tau$ $\to$ 3$\mu$ in proton-proton collisions at $\sqrt{s} =$ 13 TeV // JHEP 1: 163, 2021. DOI: 10.1007/JHEP01(2021)163. ÏÐÍÄ = 5,810*30*0,007 = 1,22
70. Sirunyan A. et al. (CMS Collaboration). Search for decays of the 125 GeV Higgs boson into a Z boson and a $\rho$ or $\phi$ meson // JHEP 11: 39, 2020. DOI: 10.1007/JHEP11(2020)039. ÏÐÍÄ = 5,810*30*0,007 = 1,22
71. Sirunyan A. et al. (CMS Collaboration). Investigation into the event-activity dependence of $\Upsilon$(nS) relative production in proton-proton collisions at $ \sqrt{s} $ = 7 TeV // JHEP 11: 1, 2020. DOI: 10.1007/JHEP11(2020)001. ÏÐÍÄ = 5,810*30*0,007 = 1,22
72. Sirunyan A. et al. (CMS Collaboration). Measurement of the $CP$-violating phase $\phi_\mathrm{s}$ in the B$^0_\mathrm{s}\to$ J$/\psi\, \phi$(1020) $\to \mu^+\mu^-$K$^+$K$^-$ channel in proton-proton collisions at $\sqrt{s} =$ 13 TeV // Phys.Lett.B816: 136188, 2021. DOI: 10.1016/j.physletb.2021.136188. ÏÐÍÄ = 4,771*30*0,007 = 1,00
73. Sirunyan A. et al. (CMS Collaboration). Measurement of the inclusive and differential Higgs boson production cross sections in the leptonic WW decay mode at $\sqrt{s} =$ 13 TeV // JHEP 3: 3, 2021. DOI: 10.1007/JHEP03(2021)003. ÏÐÍÄ = 5,810*30*0,007 = 1,22
74. Sirunyan A. et al. (CMS Collaboration). Reconstruction of signal amplitudes in the CMS electromagnetic calorimeter in the presence of overlapping proton-proton interactions // JINST 15: 10, P10002, 2020. DOI: 10.1088/1748-0221/15/10/P10002. ÏÐÍÄ = 1,415*30*0,007 = 0,30
75. Sirunyan A. et al. (CMS Collaboration). Inclusive search for highly boosted Higgs bosons decaying to bottom quark-antiquark pairs in proton-proton collisions at $\sqrt{s} =$ 13 TeV // JHEP 12: 85, 2020. DOI: 10.1007/JHEP12(2020)085. ÏÐÍÄ = 5,810*30*0,007 = 1,22
76. Sirunyan A. et al. (CMS Collaboration). Observation of the Production of Three Massive Gauge Bosons at $\sqrt {s}$ =13 TeV // Phys.Rev.Lett. 125: 15, 151802, 2020. DOI: 10.1103/PhysRevLett.125.151802. ÏÐÍÄ = 9,161*30*0,007 = 1,92
77. Sirunyan A. et al. (CMS Collaboration). Evidence for Top Quark Production in Nucleus-Nucleus Collisions // Phys.Rev.Lett. 125: 22, 222001, 2020. DOI: 10.1103/PhysRevLett.125.222001. ÏÐÍÄ = 9,161*30*0,007 = 1,92
78. Sirunyan A. et al. (CMS Collaboration). Performance of the CMS Level-1 trigger in proton-proton collisions at $\sqrt{s} =$ 13 TeV // JINST 15: 10, P10017, 2020. DOI: 10.1088/1748-0221/15/10/P10017. ÏÐÍÄ = 1,415*30*0,007 = 0,30
79. Sirunyan A. et al. (CMS Collaboration). Measurement of the azimuthal anisotropy of Image 1 and Image 2 mesons in PbPb collisions at sNN=5.02TeV // Phys.Lett.B819: 136385, 2021. DOI: 10.1016/j.physletb.2021.136385. ÏÐÍÄ = 4,771*30*0,007 = 1,00
80. Sirunyan A. et al. (CMS Collaboration). Search for resonant pair production of Higgs bosons in the $bbZZ$ channel in proton-proton collisions at $\sqrt{s}=$ 13 TeV // Phys.Rev.D102: 3, 032003, 2020. DOI: 10.1103/PhysRevD.102.032003. ÏÐÍÄ = 5,296*30*0,007 = 1,11
81. Sirunyan A. et al. (CMS Collaboration). Measurement of b jet shapes in proton-proton collisions at $\sqrt{s} =$ 5.02 TeV // JHEP 5: 54, 2021. DOI: 10.1007/JHEP05(2021)054. ÏÐÍÄ = 5,810*30*0,007 = 1,22
82. Sirunyan A. et al. (CMS Collaboration). Search for a light charged Higgs boson in the H$^\pm$ $\to $ cs channel in proton-proton collisions at $\sqrt{s} =$ 13 TeV // Phys.Rev.D102: 7, 072001, 2020. DOI: 10.1103/PhysRevD.102.072001. ÏÐÍÄ = 5,296*30*0,007 = 1,11
83. Sirunyan A. et al. (CMS Collaboration). Search for a light pseudoscalar Higgs boson in the boosted $\mu\mu\tau\tau$ final state in proton-proton collisions at $\sqrt{s}=$ 13 TeV // JHEP 8: 139, 2020. DOI: 10.1007/JHEP08(2020)139. ÏÐÍÄ = 5,810*30*0,007 = 1,22
84. Sirunyan A. et al. (CMS Collaboration). Dependence of inclusive jet production on the anti-k$_{T}$ distance parameter in pp collisions at $ \sqrt{\mathrm{s}} $ = 13 TeV // JHEP 12: 82, 2020. DOI: 10.1007/JHEP12(2020)082. ÏÐÍÄ = 5,810*30*0,007 = 1,22
85. Sirunyan A. et al. (CMS Collaboration). Observation of the B$^0_\mathrm{s}\to $X(3872)$\phi$ decay // Phys.Rev.Lett. 125: 15, 152001, 2020. DOI: 10.1103/PhysRevLett.125.152001. ÏÐÍÄ = 9,161*30*0,007 = 1,92
86. Aad G. et al. (CMS and ATLAS Collaborations). Combination of the W boson polarization measurements in top quark decays using ATLAS and CMS data at $\sqrt{s} =$ 8 TeV // JHEP 8: 08, 051, 2020. DOI: 10.1007/JHEP08(2020)051. ÏÐÍÄ = 5,810*30*0,007 = 1,22
87. Sirunyan A. et al. (CMS Collaboration). Measurements of production cross sections of WZ and same-sign WW boson pairs in association with two jets in proton-proton collisions at $\sqrt{s} =$ 13 TeV // Phys.Lett.B809: 135710, 2020. DOI: 10.1016/j.physletb.2020.135710. ÏÐÍÄ = 4,771*30*0,007 = 1,00
88. Sirunyan A. et al. (CMS Collaboration). Measurement of CKM matrix elements in single top quark $t$-channel production in proton-proton collisions at $\sqrt{s} = $ 13 TeV // Phys.Lett.B808: 135609, 2020. DOI: 10.1016/j.physletb.2020.135609. ÏÐÍÄ = 4,771*30*0,007 = 1,00
89. Sirunyan A. et al. (CMS Collaboration). Identification of heavy, energetic, hadronically decaying particles using machine-learning techniques // JINST 15: 06, P06005, 2020. DOI: 10.1088/1748-0221/15/06/P06005. ÏÐÍÄ = 1,415*30*0,007 = 0,30
90. Sirunyan A. et al. (CMS Collaboration). Search for disappearing tracks in proton-proton collisions at $\sqrt{s} =$ 13 TeV // Phys.Lett.B806: 135502, 2020. DOI: 10.1016/j.physletb.2020.135502. ÏÐÍÄ = 4,771*30*0,007 = 1,00
91. Sirunyan A. et al. (CMS Collaboration). Measurement of quark- and gluon-like jet fractions using jet charge in PbPb and pp collisions at 5.02 TeV // JHEP 7: 115, 2020. DOI: 10.1007/JHEP07(2020)115. ÏÐÍÄ = 5,810*30*0,007 = 1,22
92. Sirunyan A. et al. (CMS Collaboration). The production of isolated photons in PbPb and pp collisions at $\sqrt{s_\mathrm{NN}} =$ 5.02 TeV // JHEP 7: 116, 2020. DOI: 10.1007/JHEP07(2020)116. ÏÐÍÄ = 5,810*30*0,007 = 1,22
93. Sirunyan A. et al. (CMS Collaboration). Measurements of $\mathrm{t\bar{t}}H$ Production and the CP Structure of the Yukawa Interaction between the Higgs Boson and Top Quark in the Diphoton Decay Channel // Phys.Rev.Lett. 125: 6, 061801, 2020. DOI: 10.1103/PhysRevLett.125.061801. ÏÐÍÄ = 9,161*30*0,007 = 1,92
94. Sirunyan A. et al. (CMS Collaboration). Measurement of the cross section for $\text{t}\bar{\text{t}}$ production with additional jets and b jets in pp collisions at $\sqrt{s}=$ 13 TeV // JHEP 7: 125, 2020. DOI: 10.1007/JHEP07(2020)125. ÏÐÍÄ = 5,810*30*0,007 = 1,22
95. Sirunyan A. et al. (CMS Collaboration). Study of central exclusive $\pi^+\pi^-$ production in proton-proton collisions at $\sqrt{s} =$ 5.02 and 13 TeV // Eur.Phys.J.C80: 8, 718, 2020. DOI: 10.1140/epjc/s10052-020-8166-5. ÏÐÍÄ = 4,590*30*0,007 = 0,96
96. Sirunyan A. et al. (CMS Collaboration). Pileup mitigation at CMS in 13 TeV data // JINST 15: 09, P09018, 2020. DOI: 10.1088/1748-0221/15/09/P09018. ÏÐÍÄ = 1,415*30*0,007 = 0,30
97. Sirunyan A. et al. (CMS and TOTEM Collaborations). Measurement of single-diffractive dijet production in proton-proton collisions at $\sqrt{s} =$ 8 TeV with the CMS and TOTEM experiments // Eur.Phys.J.C80: 12, 1164, 2020. DOI: 10.1140/epjc/s10052-020-08562-y. ÏÐÍÄ = 4,590*30*0,007 = 0,96
98. Sirunyan A. et al. (CMS Collaboration). Measurement of the cross section for electroweak production of a Z boson, a photon and two jets in proton-proton collisions at $\sqrt{s} =$ 13 TeV and constraints on anomalous quartic couplings // JHEP 6: 76, 2020. DOI: 10.1007/JHEP06(2020)076. ÏÐÍÄ = 5,810*30*0,007 = 1,22
99. Sirunyan A. et al. (CMS Collaboration). A measurement of the Higgs boson mass in the diphoton decay channel // Phys.Lett.B805: 135425, 2020. DOI: 10.1016/j.physletb.2020.135425. ÏÐÍÄ = 4,771*30*0,007 = 1,00
100. Sirunyan A. et al. (CMS Collaboration). Measurement of the $\Upsilon$(1S) pair production cross section and search for resonances decaying to $\Upsilon$(1S)$\mu^+\mu^-$ in proton-proton collisions at $\sqrt{s} =$ 13 TeV // Phys.Lett.B808: 135578, 2020. DOI: 10.1016/j.physletb.2020.135578. ÏÐÍÄ = 4,771*30*0,007 = 1,00
101. Sirunyan A. et al. (CMS Collaboration). Search for physics beyond the standard model in events with jets and two same-sign or at least three charged leptons in proton-proton collisions at $\sqrt{s}=$ 13 TeV // Eur.Phys.J.C80: 8, 752, 2020. DOI: 10.1140/epjc/s10052-020-8168-3. ÏÐÍÄ = 4,590*30*0,007 = 0,96
102. Sirunyan A. et al. (CMS Collaboration). Search for charged Higgs bosons decaying into a top and a bottom quark in the all-jet final state of pp collisions at $ \sqrt{s} $ = 13 TeV // JHEP 7: 126, 2020. DOI: 10.1007/JHEP07(2020)126. ÏÐÍÄ = 5,810*30*0,007 = 1,22
103. Sirunyan A. et al. (CMS Collaboration). Measurement of the associated production of a $Z$ boson with charm or bottom quark jets in proton-proton collisions at $\sqrt {s}$=13 TeV // Phys.Rev.D102: 3, 032007, 2020. DOI: 10.1103/PhysRevD.102.032007. ÏÐÍÄ = 5,296*30*0,007 = 1,11
104. Sirunyan A. et al. (CMS Collaboration). Measurements with silicon photomultipliers of dose-rate effects in the radiation damage of plastic scintillator tiles in the CMS hadron endcap calorimeter // JINST 15: 06, P06009, 2020. DOI: 10.1088/1748-0221/15/06/P06009. ÏÐÍÄ = 1,415*30*0,007 = 0,30
105. Sirunyan A. et al. (CMS Collaboration). Study of excited $\Lambda_\mathrm{b}^0$ states decaying to $\Lambda_\mathrm{b}^0\pi^+\pi^-$ in proton-proton collisions at $\sqrt{s}=$ 13 TeV // Phys.Lett.B803: 135345, 2020. DOI: 10.1016/j.physletb.2020.135345. ÏÐÍÄ = 4,771*30*0,007 = 1,00
106. Sirunyan A. et al. (CMS Collaboration). Search for an excited lepton that decays via a contact interaction to a lepton and two jets in proton-proton collisions at $\sqrt{s} =$ 13 TeV // JHEP 5: 52, 2020. DOI: 10.1007/JHEP05(2020)052. ÏÐÍÄ = 5,810*30*0,007 = 1,22
107. Sirunyan A. et al. (CMS Collaboration). A deep neural network to search for new long-lived particles decaying to jets // Mach.Learn.Sci.Tech. 1: 35012, 2020. DOI: 10.1088/2632-2153/ab9023. ÏÐÍÄ = 2,940*30*0,007 = 0,62
108. Sirunyan A. et al. (CMS Collaboration). Measurement of the top quark forward-backward production asymmetry and the anomalous chromoelectric and chromomagnetic moments in pp collisions at $ \sqrt{s} $ = 13 TeV // JHEP 6: 146, 2020. DOI: 10.1007/JHEP06(2020)146. ÏÐÍÄ = 5,810*30*0,007 = 1,22
109. Sirunyan A. et al. (CMS Collaboration). Search for direct top squark pair production in events with one lepton, jets, and missing transverse momentum at 13 TeV with the CMS experiment // JHEP 5: 32, 2020. DOI: 10.1007/JHEP05(2020)032. ÏÐÍÄ = 5,810*30*0,007 = 1,22
110. Sirunyan A. et al. (CMS Collaboration). Constraints on the $\chi_\mathrm{c1}$ versus $\chi_\mathrm{c2}$ Polarizations in Proton-Proton Collisions at $\sqrt{s} =$ 8 TeV // Phys.Rev.Lett. 124: 16, 162002, 2020. DOI: 10.1103/PhysRevLett.124.162002. ÏÐÍÄ = 9,161*30*0,007 = 1,92
111. Sirunyan A. et al. (CMS Collaboration). A Deep Neural Network for Simultaneous Estimation of b Jet Energy and Resolution // Comput.Softw.Big Sci. 4: 1, 10, 2020. DOI: 10.1007/s41781-020-00041-z. ÏÐÍÄ = 8*0,007 = 0,06
112. Sirunyan A. et al. (CMS Collaboration). Search for a Narrow Resonance Lighter than 200 GeV Decaying to a Pair of Muons in Proton-Proton Collisions at $\sqrt{s} =$ TeV // Phys.Rev.Lett. 124: 13, 131802, 2020. DOI: 10.1103/PhysRevLett.124.131802. ÏÐÍÄ = 9,161*30*0,007 = 1,92
113. Sirunyan A. et al. (CMS Collaboration). Determination of the strong coupling constant $\alpha_{S}(m_\mathrm{Z})$ from measurements of inclusive W$^\pm$ and Z boson production cross sections in proton-proton collisions at $ \sqrt{\mathrm{s}} $ = 7 and 8 TeV // JHEP 6: 18, 2020. DOI: 10.1007/JHEP06(2020)018. ÏÐÍÄ = 5,810*30*0,007 = 1,22
114. Sirunyan A. et al. (CMS Collaboration). Performance of the reconstruction and identification of high-momentum muons in proton-proton collisions at $\sqrt{s} =$ 13 TeV // JINST 15: 02, P02027, 2020. DOI: 10.1088/1748-0221/15/02/P02027. ÏÐÍÄ = 1,415*30*0,007 = 0,30
115. Sirunyan A. et al. (CMS Collaboration). A search for the standard model Higgs boson decaying to charm quarks // JHEP 3: 131, 2020. DOI: 10.1007/JHEP03(2020)131. ÏÐÍÄ = 5,810*30*0,007 = 1,22
116. Sirunyan A. et al. (CMS Collaboration). Search for a heavy Higgs boson decaying to a pair of W bosons in proton-proton collisions at $\sqrt{s} =$ 13 TeV // JHEP 3: 34, 2020. DOI: 10.1007/JHEP03(2020)034. ÏÐÍÄ = 5,810*30*0,007 = 1,22
117. Sirunyan A. et al. (CMS Collaboration). Measurement of the top quark pair production cross section in dilepton final states containing one $\tau$ lepton in pp collisions at $\sqrt{s}=$ 13 TeV // JHEP 2: 191, 2020. DOI: 10.1007/JHEP02(2020)191. ÏÐÍÄ = 5,810*30*0,007 = 1,22
118. Sirunyan A. et al. (CMS Collaboration). Search for lepton flavour violating decays of a neutral heavy Higgs boson to $\mu\tau$ and e$\tau$ in proton-proton collisions at $\sqrt{s}=$ 13 TeV // JHEP 3: 103, 2020. DOI: 10.1007/JHEP03(2020)103. ÏÐÍÄ = 5,810*30*0,007 = 1,22
119. Sirunyan A. et al. (CMS Collaboration). Search for supersymmetry in pp collisions at $\sqrt{s}=$ 13 TeV with 137 fb$^{-1}$ in final states with a single lepton using the sum of masses of large-radius jets // Phys.Rev.D101: 5, 052010, 2020. DOI: 10.1103/PhysRevD.101.052010. ÏÐÍÄ = 5,296*30*0,007 = 1,11
120. Sirunyan A. et al. (CMS Collaboration). Search for physics beyond the standard model in multilepton final states in proton-proton collisions at $\sqrt{s} =$ 13 TeV // JHEP 3: 51, 2020. DOI: 10.1007/JHEP03(2020)051. ÏÐÍÄ = 5,810*30*0,007 = 1,22
121. Sirunyan A. et al. (CMS Collaboration). Search for high mass dijet resonances with a new background prediction method in proton-proton collisions at $\sqrt{s} =$ 13 TeV // JHEP 5: 33, 2020. DOI: 10.1007/JHEP05(2020)033. ÏÐÍÄ = 5,810*30*0,007 = 1,22
122. Sirunyan A. et al. (CMS Collaboration). Measurement of the Jet Mass Distribution and Top Quark Mass in Hadronic Decays of Boosted Top Quarks in $pp$ Collisions at $\sqrt{s} =$ TeV // Phys.Rev.Lett. 124: 20, 202001, 2020. DOI: 10.1103/PhysRevLett.124.202001. ÏÐÍÄ = 9,161*30*0,007 = 1,92
123. Sirunyan A. et al. (CMS Collaboration). Observation of the $\Lambda_\mathrm{b}^0 \to$ J/$\psi \Lambda \phi$ decay in proton-proton collisions at $\sqrt{s}=$ 13 TeV // Phys.Lett.B802: 135203, 2020. DOI: 10.1016/j.physletb.2020.135203. ÏÐÍÄ = 4,771*30*0,007 = 1,00
124. Sirunyan A. et al. (CMS Collaboration). Search for new neutral Higgs bosons through the H$\to$ ZA $\to \ell^{+}\ell^{-} \mathrm{b\bar{b}}$ process in pp collisions at $\sqrt{s} =$ 13 TeV // JHEP 3: 55, 2020. DOI: 10.1007/JHEP03(2020)055. ÏÐÍÄ = 5,810*30*0,007 = 1,22
125. Sirunyan A. et al. (CMS Collaboration). Search for dijet resonances using events with three jets in proton-proton collisions at s=13TeV // Phys.Lett.B805: 135448, 2020. DOI: 10.1016/j.physletb.2020.135448. ÏÐÍÄ = 4,771*30*0,007 = 1,00
126. Sirunyan A. et al. (CMS Collaboration). Studies of charm quark diffusion inside jets using PbPb and pp collisions at $\sqrt{s_\mathrm{NN}} =$ 5.02 TeV // Phys.Rev.Lett. 125: 10, 102001, 2020. DOI: 10.1103/PhysRevLett.125.102001. ÏÐÍÄ = 9,161*30*0,007 = 1,92
127. Sirunyan A. et al. (CMS Collaboration). Search for top squark pair production in a final state with two tau leptons in proton-proton collisions at $ \sqrt{s} =$ 13 TeV // JHEP 2: 15, 2020. DOI: 10.1007/JHEP02(2020)015. ÏÐÍÄ = 5,810*30*0,007 = 1,22
128. Sirunyan A. et al. (CMS Collaboration). Measurement of properties of B$^0_\mathrm{s}\to\mu^+\mu^-$ decays and search for B$^0\to\mu^+\mu^-$ with the CMS experiment // JHEP 4: 188, 2020. DOI: 10.1007/JHEP04(2020)188. ÏÐÍÄ = 5,810*30*0,007 = 1,22
129. Sirunyan A.M. et al. (CMS Collaboration). Search for a heavy pseudoscalar Higgs boson decaying into a 125 GeV Higgs boson and a Z boson in final states with two tau and two light leptons at $\sqrt{s}=$ 13 TeV // JHEP 3: 65, 2020. DOI: 10.1007/JHEP03(2020)065. ÏÐÍÄ = 5,810*30*0,007 = 1,22
130. Sirunyan A.M. et al. (CMS Collaboration). Bose-Einstein correlations of charged hadrons in proton-proton collisions at $\sqrt{s} =$ 13 TeV // JHEP 3: 14, 2020. DOI: 10.1007/JHEP03(2020)014. ÏÐÍÄ = 5,810*30*0,007 = 1,22
131. Sirunyan A.M. et al. (CMS Collaboration). Mixed higher-order anisotropic flow and nonlinear response coefficients of charged particles in $\mathrm {PbPb}$ collisions at $\sqrt{\smash [b]{s_{_{\mathrm {NN}}}}} = 2.76$ and 5.02$\,\text {TeV}$ // Eur.Phys.J.C80: 6, 534, 2020. DOI: 10.1140/epjc/s10052-020-7834-9. ÏÐÍÄ = 4,590*30*0,007 = 0,96
132. Sirunyan A.M. et al. (CMS Collaboration). Strange hadron production in pp and pPb collisions at $\sqrt{s_\mathrm{NN}}= $ 5.02 TeV // Phys.Rev.C101: 6, 064906, 2020. DOI: 10.1103/PhysRevC.101.064906. ÏÐÍÄ = 3,296*30*0,007 = 0,69
133. Sirunyan A.M. et al. (CMS Collaboration). Study of J/$\psi$ meson production inside jets in pp collisions at $\sqrt{s} =$ 8 TeV // Phys.Lett.B804: 135409, 2020. DOI: 10.1016/j.physletb.2020.135409. ÏÐÍÄ = 4,771*30*0,007 = 1,00
134. Sirunyan A.M. et al. (CMS Collaboration). Search for Supersymmetry with a Compressed Mass Spectrum in Events with a Soft $\tau$ Lepton, a Highly Energetic Jet, and Large Missing Transverse Momentum in Proton-Proton Collisions at $\sqrt{s}=$ TeV // Phys.Rev.Lett. 124: 4, 041803, 2020. DOI: 10.1103/PhysRevLett.124.041803. ÏÐÍÄ = 9,161*30*0,007 = 1,92
135. Sirunyan A.M. et al. (CMS Collaboration). Calibration of the CMS hadron calorimeters using proton-proton collision data at $\sqrt{s} =$ 13 TeV // JINST 15: 05, P05002, 2020. DOI: 10.1088/1748-0221/15/05/P05002. ÏÐÍÄ = 1,415*30*0,007 = 0,30
136. Sirunyan A.M. et al. (CMS Collaboration). Running of the top quark mass from proton-proton collisions at $\sqrt{s} =$ 13TeV // Phys.Lett.B803: 135263, 2020. DOI: 10.1016/j.physletb.2020.135263. ÏÐÍÄ = 4,771*30*0,007 = 1,00
137. Sirunyan A.M. et al. (CMS Collaboration). Evidence for $\text {W}\text {W}$ production from double-parton interactions in proton–proton collisions at $\sqrt{s} = 13 \,\text {TeV} $ // Eur.Phys.J.C80: 1, 41, 2020. DOI: 10.1140/epjc/s10052-019-7541-6. ÏÐÍÄ = 4,590*30*0,007 = 0,96
138. Sirunyan A.M. et al. (CMS Collaboration). Measurement of the $\mathrm{t\bar{t}}\mathrm{b\bar{b}}$ production cross section in the all-jet final state in pp collisions at $\sqrt{s} =$ 13 TeV // Phys.Lett.B803: 135285, 2020. DOI: 10.1016/j.physletb.2020.135285. ÏÐÍÄ = 4,771*30*0,007 = 1,00
139. Sirunyan A.M. et al. (CMS Collaboration). Search for electroweak production of a vector-like T quark using fully hadronic final states // JHEP 1: 36, 2020. DOI: 10.1007/JHEP01(2020)036. ÏÐÍÄ = 5,810*30*0,007 = 1,22
140. Sirunyan A.M. et al. (CMS Collaboration). Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV // Eur.Phys.J.C80: 1, 3, 2020. DOI: 10.1140/epjc/s10052-019-7493-x. ÏÐÍÄ = 4,590*30*0,007 = 0,96
141. Sirunyan A.M. et al. (CMS Collaboration). Search for a charged Higgs boson decaying into top and bottom quarks in events with electrons or muons in proton-proton collisions at $ \sqrt{\mathrm{s}} $ = 13 TeV // JHEP 1: 96, 2020. DOI: 10.1007/JHEP01(2020)096. ÏÐÍÄ = 5,810*30*0,007 = 1,22
142. Sirunyan A.M. et al. (CMS Collaboration). Search for production of four top quarks in final states with same-sign or multiple leptons in proton-proton collisions at $\sqrt{s}=$ 13 TeV // Eur.Phys.J.C80: 2, 75, 2020. DOI: 10.1140/epjc/s10052-019-7593-7. ÏÐÍÄ = 4,590*30*0,007 = 0,96
143. Sirunyan A.M. et al. (CMS Collaboration). Search for dark matter particles produced in association with a Higgs boson in proton-proton collisions at $ \sqrt{\mathrm{s}} $ = 13 TeV // JHEP 3: 25, 2020. DOI: 10.1007/JHEP03(2020)025. ÏÐÍÄ = 5,810*30*0,007 = 1,22
144. Sirunyan A.M. et al. (CMS Collaboration). Search for heavy Higgs bosons decaying to a top quark pair in proton-proton collisions at $\sqrt{s} =$ 13 TeV // JHEP 4: 171, 2020. DOI: 10.1007/JHEP04(2020)171. ÏÐÍÄ = 5,810*30*0,007 = 1,22
145. Sirunyan A.M. et al. (CMS Collaboration). Search for direct pair production of supersymmetric partners to the $\tau$ lepton in proton-proton collisions at $\sqrt{s}=$ 13 TeV // Eur.Phys.J.C80: 3, 189, 2020. DOI: 10.1140/epjc/s10052-020-7739-7. ÏÐÍÄ = 4,590*30*0,007 = 0,96
146. Sirunyan A.M. et al. (CMS Collaboration). Measurement of top quark pair production in association with a Z boson in proton-proton collisions at $\sqrt{s}=$ 13 TeV // JHEP 3: 56, 2020. DOI: 10.1007/JHEP03(2020)056. ÏÐÍÄ = 5,810*30*0,007 = 1,22
147. Sirunyan A.M. et al. (CMS Collaboration). Measurement of differential cross sections and charge ratios for t-channel single top quark production in proton–proton collisions at $\sqrt{s}=13\,\text {Te}\text {V}$ // Eur.Phys.J.C80: 5, 370, 2020. DOI: 10.1140/epjc/s10052-020-7858-1. ÏÐÍÄ = 4,590*30*0,007 = 0,96
148. Sirunyan A.M. et al. (CMS Collaboration). Search for light pseudoscalar boson pairs produced from decays of the 125 GeV Higgs boson in final states with two muons and two nearby tracks in pp collisions at $\sqrt{s}=$ 13 TeV // Phys.Lett.B800: 135087, 2020. DOI: 10.1016/j.physletb.2019.135087. ÏÐÍÄ = 4,771*30*0,007 = 1,00
149. Sirunyan A.M. et al. (CMS Collaboration). Combined search for supersymmetry with photons in proton-proton collisions at $\sqrt{s}=$ 13 TeV // Phys.Lett.B801: 135183, 2020. DOI: 10.1016/j.physletb.2019.135183. ÏÐÍÄ = 4,771*30*0,007 = 1,00
150. Sirunyan A.M. et al. (CMS Collaboration). A multi-dimensional search for new heavy resonances decaying to boosted WW, WZ, or ZZ boson pairs in the dijet final state at 13 TeV // Eur.Phys.J.C80: 3, 237, 2020. DOI: 10.1140/epjc/s10052-020-7773-5. ÏÐÍÄ = 4,590*30*0,007 = 0,96
151. Sirunyan A.M. et al. (CMS Collaboration). Production of $\Lambda_\mathrm{c}^+$ baryons in proton-proton and lead-lead collisions at $\sqrt{s_\mathrm{NN}}=$ 5.02 TeV // Phys.Lett.B803: 135328, 2020. DOI: 10.1016/j.physletb.2020.135328. ÏÐÍÄ = 4,771*30*0,007 = 1,00
152. Sirunyan A. et al. (CMS Collaboration). Correlations of azimuthal anisotropy Fourier harmonics with subevent cumulants in $pPb$ collisions at $\sqrt{s_{NN}}=$8.16TeV // Phys.Rev.C103: 1, 014902, 2021. DOI: 10.1103/PhysRevC.103.014902. ÏÐÍÄ = 3,296*30*0,007 = 0,69
153. Sirunyan A.M. et al. (CMS Collaboration). Observation of nuclear modifications in W$^\pm$ boson production in pPb collisions at $\sqrt{s_\mathrm{NN}} =$ 8.16 TeV // Phys.Lett.B800: 135048, 2020. DOI: 10.1016/j.physletb.2019.135048. ÏÐÍÄ = 4,771*30*0,007 = 1,00
154. Sirunyan A.M. et al. (CMS Collaboration). Multiparticle correlation studies in pPb collisions at $\sqrt{s_\mathrm{NN}} =$ 8.16 TeV // Phys.Rev.C101: 1, 014912, 2020. DOI: 10.1103/PhysRevC.101.014912. ÏÐÍÄ = 3,296*30*0,007 = 0,69
155. Sirunyan A.M. et al. (CMS Collaboration). Measurement of $\mathrm{t\bar t}$ normalised multi-differential cross sections in pp collisions at $\sqrt s=13$ TeV, and simultaneous determination of the strong coupling strength, top quark pole mass, and parton distribution functions // Eur.Phys.J.C80: 7, 658, 2020. DOI: 10.1140/epjc/s10052-020-7917-7. ÏÐÍÄ = 4,590*30*0,007 = 0,96
156. Sirunyan A.M. et al. (CMS Collaboration). Extraction and validation of a new set of CMS PYTHIA8 tunes from underlying-event measurements // Eur.Phys.J.C80: 1, 4, 2020. DOI: 10.1140/epjc/s10052-019-7499-4. ÏÐÍÄ = 4,590*30*0,007 = 0,96
157. Sirunyan A. et al. (CMS Collaboration). Measurement of electroweak production of a $\mathrm{W} $ boson in association with two jets in proton–proton collisions at $\sqrt{s}=13\,\text {Te}\text {V} $ // Eur.Phys.J.C80: 1, 43, 2020. DOI: 10.1140/epjc/s10052-019-7585-7. ÏÐÍÄ = 4,590*30*0,007 = 0,96
158. Sirunyan A.M. et al. (CMS Collaboration). Measurement of the single top quark and antiquark production cross sections in the $t$ channel and their ratio in proton-proton collisions at $\sqrt{s}=$ 13 TeV // Phys.Lett.B800: 135042, 2020. DOI: 10.1016/j.physletb.2019.135042. ÏÐÍÄ = 4,771*30*0,007 = 1,00

Ïðåïðèíòû:
1. Tumasyan A. et al. (CMS Collaboration). Probing charm quark dynamics via multiparticle correlations in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ =5.02 TeV // arXiv:2112.12236 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
2. Tumasyan A. et al. (CMS Collaboration). Search for resonant production of strongly coupled dark matter in proton-proton collisions at 13 TeV // arXiv:2112.11125 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
3. Tumasyan A. et al. (CMS Collaboration). Measurement of the production cross section for Z + b jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV // arXiv:2112.09659 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
4. Tumasyan A. et al. (CMS Collaboration). Measurement of the inclusive $\mathrm{t\bar{t}}$ production cross section in proton-proton collisions at $\sqrt{s}$ = 5.02 TeV // arXiv:2112.09114 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
5. Tumasyan A. et al. (CMS Collaboration). Evidence for WW/WZ vector boson scattering in the decay channel $\ell\nu$qq produced in association with two jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV // arXiv:2112.05259 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
6. Tumasyan A. et al. (CMS Collaboration). Search for a right-handed W boson and a heavy neutrino in proton-proton collisions at $\sqrt{s}$ = 13 TeV // arXiv:2112.03949 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
7. Tumasyan A. et al. (CMS Collaboration). Search for heavy resonances decaying to a pair of Lorentz-boosted Higgs bosons in final states with leptons and a bottom quark pair at $\sqrt{s}$ = 13 TeV // arXiv:2112.03161 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
8. Tumasyan A. et al. (CMS Collaboration). Measurements of the associated production of a W boson and a charm quark in proton-proton collisions at $\sqrt{s}$ = 8 TeV // arXiv:2112.00895 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
9. Tumasyan A. et al. (CMS Collaboration). Measurement of W$^\pm\gamma$ differential cross sections in proton-proton collisions at $\sqrt{s}$ = 13 TeV and effective field theory constraints // arXiv:2111.13948 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
10. Tumasyan A. et al. (CMS Collaboration). Search for heavy resonances decaying to ZZ or ZW and axion-like particles mediating nonresonant ZZ or ZH production at $\sqrt{s}$ = 13 TeV // arXiv:2111.13669 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
11. Tumasyan A. et al. (CMS Collaboration). Measurement and QCD analysis of double-differential inclusive jet cross sections in proton-proton collisions at $\sqrt{s}$ = 13 TeV // arXiv:2111.10431 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
12. Tumasyan A. et al. (CMS Collaboration). Search for a heavy resonance decaying into a top quark and a W boson in the lepton+jets final state at $\sqrt{s}$= 13 TeV // arXiv:2111.10216 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
13. Tumasyan A. et al. (CMS Collaboration). Strategies and performance of the CMS silicon tracker alignment during LHC Run 2 // arXiv:2111.08757 [physics.ins-det], 2021. ÏÐÍÄ = 3*0,007 = 0,02
14. Acar B. et al. (CMS HGCAL Collaboration). Response of a CMS HGCAL silicon-pad electromagnetic calorimeter prototype to 20-300 GeV positrons // arXiv:2111.06855 [physics.ins-det], 2021. ÏÐÍÄ = 3*0,007 = 0,02
15. Tumasyan A. et al. (CMS Collaboration). Search for supersymmetry in final states with two or three soft leptons and missing transverse momentum in proton-proton collisions at $\sqrt{s}$ = 13 TeV // arXiv:2111.06296 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
16. Tumasyan A. et al. (CMS Collaboration). Observation of triple J/$\psi$ meson production in proton-proton collisions at $\sqrt{s}$ = 13 TeV // arXiv:2111.05370 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
17. Tumasyan A. et al. (CMS Collaboration). Study of dijet events with large rapidity separation in proton-proton collisions at $\sqrt{s}$ = 2.76 TeV // arXiv:2111.04605 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
18. Tumasyan A. et al. (CMS Collaboration). Search for long-lived particles produced in association with a Z boson in proton-proton collisions at $\sqrt{s}$ = 13 TeV // arXiv:2110.13218 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
19. Tumasyan A. et al. (CMS Collaboration). Measurement of the inclusive and differential WZ production cross sections, polarization angles, and triple gauge couplings in pp collisions at $\sqrt{s}$ = 13 TeV // arXiv:2110.11231 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
20. Tumasyan A. et al. (TOTEM and CMS Collaborations). First search for exclusive diphoton production at high mass with tagged protons in proton-proton collisions at $\sqrt{s}$ = 13 TeV // arXiv:2110.05916 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
21. Tumasyan A. et al. (CMS Collaboration). Analysis of the CP structure of the Yukawa coupling between the Higgs boson and $\tau$ leptons in proton-proton collisions at $\sqrt{s}$ = 13 TeV // arXiv:2110.04836 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
22. Tumasyan A. et al. (CMS Collaboration). Search for long-lived particles decaying to leptons with large impact parameter in proton-proton collisions at $\sqrt{s}$ = 13 TeV // arXiv:2110.04809 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
23. Tumasyan A. et al. (CMS Collaboration). Measurement of double-parton scattering in inclusive production of four jets with low transverse momentum in proton-proton collisions at $\sqrt{s}$ = 13 TeV // arXiv:2109.13822 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
24. Tumasyan A. et al. (CMS Collaboration). Search for heavy resonances decaying to Z($\nu\bar{\nu}$)V(q$\bar{q}$') in proton-proton collisions at $\sqrt{s}$ = 13 TeV // arXiv:2109.08268 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
25. Tumasyan A. et al. (CMS Collaboration). Search for heavy resonances decaying to WW, WZ, or WH boson pairs in the lepton plus merged jet final state in proton-proton collisions at $\sqrt{s}$ = 13 TeV // arXiv:2109.06055 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
26. Tumasyan A. et al. (CMS Collaboration). Study of quark and gluon jet substructure in Z+jet and dijet events from pp collisions // arXiv:2109.03340 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
27. Tumasyan A. et al. (CMS Collaboration). Observation of B$^0_s$ mesons and measurement of the B$^0_s$/B$^+$ yield ratio in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV // arXiv:2109.01908 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
28. Tumasyan A. et al. (CMS Collaboration). Measurement of the top quark mass using events with a single reconstructed top quark in pp collisions at $\sqrt{s}$ = 13 TeV // arXiv:2108.10407 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
29. Tumasyan A. et al. (CMS Collaboration). Measurement of the inclusive and differential Higgs boson production cross sections in the decay mode to a pair of $\tau$ leptons in pp collisions at $\sqrt{s} = $ 13 TeV // arXiv:2107.11486 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
30. Tumasyan A. et al. (CMS Collaboration). Search for long-lived particles decaying in the CMS endcap muon detectors in proton-proton collisions at $\sqrt{s} = $ 13 TeV // arXiv:2107.04838 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
31. Tumasyan A. et al. (CMS Collaboration). Measurement of the inclusive and differential $\mathrm{t\overline{t}}\gamma$ cross sections in the single-lepton channel and EFT interpretation at $\sqrt{s}$ = 13 TeV // arXiv:2107.01508 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
32. Tumasyan A. et al. (CMS Collaboration). Search for electroweak production of charginos and neutralinos in proton-proton collisions at $\sqrt{s} = $ 13 TeV // arXiv:2106.14246 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
33. Tumasyan A. et al. (CMS Collaboration). Fragmentation of jets containing a prompt J$/\psi$ meson in PbPb and pp collisions at $\sqrt{s_\mathrm{NN}} =$ 5.02 TeV // arXiv:2106.13235 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
34. Tumasyan A. et al. (CMS Collaboration). Search for W$\gamma$ resonances in proton-proton collisions at $\sqrt{s} =$ 13 TeV using hadronic decays of Lorentz-boosted W bosons // arXiv:2106.10509 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
35. Tumasyan A. et al. (CMS Collaboration). Search for strongly interacting massive particles generating trackless jets in proton-proton collisions at $\sqrt{s} = $ 13 TeV // arXiv:2105.09178 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
36. Sirunyan A. et al. (CMS Collaboration). Using Z boson events to study parton-medium interactions in PbPb collisions // arXiv:2103.04377 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02
37. Sirunyan A. et al. (CMS Collaboration). Evidence for X(3872) in PbPb collisions and studies of its prompt production at $\sqrt{s_\mathrm{NN}}=$ 5.02 TeV // arXiv:2102.13048 [hep-ex], 2021. ÏÐÍÄ = 3*0,007 = 0,02

Èòîãî: ÏÐÍÄ = 176,48

Ñóììàðíûé ÏÐÍÄ (çà 2020-2021 ãã.) = 241.136