Ðåéòèíã (ÏÐÍÄ) ñîòðóäíêîâ ÈßÈ ÐÀÍ ñåçîíà 23 [309]
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 | ÏÐÍÄ
ðóê | ê-ò óìíî
æåíèÿ | äàòà | ôàéë
ðàñ÷¸òà | äîëæí |
| Ìóñèåíêî Þðèé Âàñèëüåâè÷ | × | 208,7 | | | 25.01.2023 |  | Ñ |
Ìóñèåíêî Þðèé Âàñèëüåâè÷, ðîä. 07.02.1962, ñíñ ËÔÝÑÂ ÎÔÂÝ
Ñóììàðíûé ÏÐÍÄ (çà 2021-2022 ãã.) = 208,67
Ñòàòüè:
1. 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 = 1,121*30*0,047 = 1,58
2. 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 = 1,121*30*0,028 = 0,94
Ñóììàðíûé ÏÐÍÄ ïî ñòàòüÿì/ïðåïðèíòàì íå CMS = 2,52
Äîêëàäû íà êîíôåðåíöèÿõ è òðóäû êîíôåðåíöèé:
1. 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
2. Yu.Musienko, Yu.Andreev, A.Heering, A.Karneyeu, M.Wayne "Results of QA/QC tests of the Hamamatsu SiPM arrays for the CMS HCAL Phase I upgrade", 9th Conference on New Developments in Photodetection, Troyes, France 04-08, July 2022 (óñòíûé), https://www.ndip.fr/. ÏÐÍÄ = 10+15/3 = 15
3. Yu.Musienko, A.Heering, A.Karneyeu, M.Wayne "Monte-Carlo model for calculating SiPM noise in measuring systems", 9th Conference on New Developments in Photodetection, Troyes, France 04-08, July 2022 (ñòåíäîâûé), https://www.ndip.fr/. ÏÐÍÄ = 10*0,43 = 4,3
4. A.Heering, A.Karneyeu, Yu.Musienko, M.Wayne , I.Schmidt, “Integration of mini TECs on the CMSBTL 16 ch SiPM array to reduce the DCR after very high irradiation", 9th Conference on New Developments in Photodetection, Troyes, France 04-08, July 2022 (ñòåíäîâûé), https://www.ndip.fr/. ÏÐÍÄ = 10*0,38 = 3,8
Ñóììàðíûé ÏÐÍÄ ïî äîêëàäàì = 27,6
Ñòàòüè CMS:
1. 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 = 3,199*30*0,007 = 0,67
2. 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 = 6,379*30*0,007 = 1,34
3. 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 = 4,950*30*0,007 = 1,04
4. 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 = 6,379*30*0,007 = 1,34
5. 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 = 4,950*30*0,007 = 1,04
6. 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 = 6,379*30*0,007 = 1,34
7. 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 = 4,991*30*0,007 = 1,05
8. 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 = 4,991*30*0,007 = 1,05
9. 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 = 4,950*30*0,007 = 1,04
10. 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 = 5,407*30*0,007 = 1,14
11. 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 = 4,991*30*0,007 = 1,05
12. 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 = 6,379*30*0,007 = 1,34
13. 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 = 4,950*30*0,007 = 1,04
14. 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 = 4,950*30*0,007 = 1,04
15. 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 = 4,950*30*0,007 = 1,04
16. 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 = 6,379*30*0,007 = 1,34
17. 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 = 4,991*30*0,007 = 1,05
18. 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 = 6,379*30*0,007 = 1,34
19. 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 = 1,121*30*0,007 = 0,24
20. 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 = 4,991*30*0,007 = 1,05
21. 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 = 4,991*30*0,007 = 1,05
22. 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 = 9,185*30*0,007 = 1,93
23. 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 = 4,950*30*0,007 = 1,04
24. 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 = 6,379*30*0,007 = 1,34
25. 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 = 5,407*30*0,007 = 1,14
26. 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 = 6,379*30*0,007 = 1,34
27. 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 = 6,379*30*0,007 = 1,34
28. 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 = 4,950*30*0,007 = 1,04
29. 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 = 1,121*30*0,007 = 0,24
30. 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 = 6,379*30*0,007 = 1,34
31. 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 = 4,950*30*0,007 = 1,04
32. 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 = 6,379*30*0,007 = 1,34
33. 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 = 6,379*30*0,007 = 1,34
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 = 6,379*30*0,007 = 1,34
35. 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 = 9,185*30*0,007 = 1,93
36. 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 = 9,185*30*0,007 = 1,93
37. 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 = 1,121*30*0,007 = 0,24
38. 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 = 5,407*30*0,007 = 1,14
39. 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 = 5,407*30*0,007 = 1,14
40. 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 = 4,991*30*0,007 = 1,05
41. 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 = 4,991*30*0,007 = 1,05
42. Sirunyan A.M. et al. (CMS Collaboration). Evidence for X(3872) in Pb-Pb Collisions and Studies of its Prompt Production at $\sqrt {s_{NN}}$=5.02??TeV // Phys.Rev.Lett. 128: 3, 032001, 2022. DOI: 10.1103/PhysRevLett.128.032001. ÏÐÍÄ = 9,185*30*0,007 = 1,93
43. 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 = 6,379*30*0,007 = 1,34
44. 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 = 6,379*30*0,007 = 1,34
45. 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 = 5,407*30*0,007 = 1,14
46. 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 = 6,379*30*0,007 = 1,34
47. Sirunyan A.M. et al. (CMS Collaboration). Using Z Boson Events to Study Parton-Medium Interactions in Pb-Pb Collisions // Phys.Rev.Lett. 128: 12, 122301, 2022. DOI: 10.1103/PhysRevLett.128.122301. ÏÐÍÄ = 9,185*30*0,007 = 1,93
48. 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 = 4,991*30*0,007 = 1,05
49. 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 = 6,379*30*0,007 = 1,34
50. 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 = 9,185*30*0,007 = 1,93
51. 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 = 4,991*30*0,007 = 1,05
52. 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 = 4,991*30*0,007 = 1,05
53. 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 = 4,950*30*0,007 = 1,04
54. 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 = 5,407*30*0,007 = 1,14
55. 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 = 6,379*30*0,007 = 1,34
56. 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 = 5,407*30*0,007 = 1,14
57. 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 = 5,407*30*0,007 = 1,14
58. Tumasyan A. et al. (CMS Collaboration). Search for strongly interacting massive particles generating trackless jets in proton–proton collisions at $\sqrt{s} = 13\,\text {TeV} $ // Eur.Phys.J.C82: 3, 213, 2022. DOI: 10.1140/epjc/s10052-022-10095-5. ÏÐÍÄ = 4,991*30*0,007 = 1,05
59. 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 = 6,379*30*0,007 = 1,34
60. 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 = 6,379*30*0,007 = 1,34
61. 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 = 6,379*30*0,007 = 1,34
62. 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 // Phys.Lett.B826: 136888, 2022. DOI: 10.1016/j.physletb.2022.136888. ÏÐÍÄ = 4,950*30*0,007 = 1,04
63. 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 = 5,407*30*0,007 = 1,14
64. 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 // Phys.Lett.B825: 136842, 2022. DOI: 10.1016/j.physletb.2021.136842. ÏÐÍÄ = 4,950*30*0,007 = 1,04
65. Tumasyan A. et al. (CMS Collaboration). Search for electroweak production of charginos and neutralinos in proton-proton collisions at $ \sqrt{s} $ = 13 TeV // JHEP 4: 147, 2022. DOI: 10.1007/JHEP04(2022)147. ÏÐÍÄ = 6,379*30*0,007 = 1,34
66. 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 = 9,185*30*0,007 = 1,93
67. 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 = 6,379*30*0,007 = 1,34
68. 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 = 4,991*30*0,007 = 1,05
69. 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 // Phys.Rev.Lett. 128: 8, 081805, 2022. DOI: 10.1103/PhysRevLett.128.081805. ÏÐÍÄ = 9,185*30*0,007 = 1,93
70. 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 = 6,379*30*0,007 = 1,34
71. 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 = 6,379*30*0,007 = 1,34
72. 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 = 6,379*30*0,007 = 1,34
73. 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 = 5,407*30*0,007 = 1,14
74. 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 = 6,379*30*0,007 = 1,34
75. Tumasyan A. et al. (CMS Collaboration). Observation of Bs0 mesons and measurement of the Bs0/B+ yield ratio in PbPb collisions at Image 1 TeV // Phys.Lett.B829: 137062, 2022. DOI: 10.1016/j.physletb.2022.137062. ÏÐÍÄ = 4,950*30*0,007 = 1,04
76. Tumasyan A. et al. (CMS Collaboration). Study of quark and gluon jet substructure in Z+jet and dijet events from pp collisions // JHEP 1: 188, 2022. DOI: 10.1007/JHEP01(2022)188. ÏÐÍÄ = 6,379*30*0,007 = 1,34
77. 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 // Phys.Rev.D105: 3, 032008, 2022. DOI: 10.1103/PhysRevD.105.032008. ÏÐÍÄ = 5,407*30*0,007 = 1,14
78. 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 // Phys.Rev.D106: 1, 012004, 2022. DOI: 10.1103/PhysRevD.106.012004. ÏÐÍÄ = 5,407*30*0,007 = 1,14
79. 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 // JHEP 1: 177, 2022. DOI: 10.1007/JHEP01(2022)177. ÏÐÍÄ = 6,379*30*0,007 = 1,34
80. 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\,\text {Te}\text {V} $ // Eur.Phys.J.C82: 2, 153, 2022. DOI: 10.1140/epjc/s10052-022-10027-3. ÏÐÍÄ = 4,991*30*0,007 = 1,05
81. 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 // JHEP 6: 12, 2022. DOI: 10.1007/JHEP06(2022)012. ÏÐÍÄ = 6,379*30*0,007 = 1,34
82. 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 // Phys.Rev.Lett. 129: 1, 011801, 2022. DOI: 10.1103/PhysRevLett.129.011801. ÏÐÍÄ = 9,185*30*0,007 = 1,93
83. 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 // JHEP 7: 32, 2022. DOI: 10.1007/JHEP07(2022)032. ÏÐÍÄ = 6,379*30*0,007 = 1,34
84. 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 // JHEP 3: 160, 2022. DOI: 10.1007/JHEP03(2022)160. ÏÐÍÄ = 6,379*30*0,007 = 1,34
85. Tumasyan A. et al. (CMS Collaboration). Search for low-mass dilepton resonances in Higgs boson decays to four-lepton final states in proton–proton collisions at $\sqrt{s}=13\,\text {TeV} $ // Eur.Phys.J.C82: 4, 290, 2022. DOI: 10.1140/epjc/s10052-022-10127-0. ÏÐÍÄ = 4,991*30*0,007 = 1,05
86. Tumasyan A. et al. (CMS Collaboration). Search for Flavor-Changing Neutral Current Interactions of the Top Quark and Higgs Boson in Final States with Two Photons in Proton-Proton Collisions at $\sqrt{s}=13\text{ }\text{ }\mathrm{TeV}$ // Phys.Rev.Lett. 129: 3, 032001, 2022. DOI: 10.1103/PhysRevLett.129.032001. ÏÐÍÄ = 9,185*30*0,007 = 1,93
87. Tumasyan A. et al. (CMS Collaboration). Inclusive and differential cross section measurements of single top quark production in association with a Z boson in proton-proton collisions at $ \sqrt{s} $ = 13 TeV // JHEP 2: 107, 2022. DOI: 10.1007/JHEP02(2022)107. ÏÐÍÄ = 6,379*30*0,007 = 1,34
88. Tumasyan A. et al. (CMS Collaboration). A new calibration method for charm jet identification validated with proton-proton collision events at $\sqrt{s}$ =13 TeV // JINST 17: 03, P03014, 2022. DOI: 10.1088/1748-0221/17/03/P03014. ÏÐÍÄ = 1,121*30*0,007 = 0,24
89. Tumasyan A. et al. (CMS Collaboration). Study of dijet events with large rapidity separation in proton-proton collisions at $ \sqrt{s} $ = 2.76 TeV // JHEP 3: 189, 2022. DOI: 10.1007/JHEP03(2022)189. ÏÐÍÄ = 6,379*30*0,007 = 1,34
90. 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 // JHEP 4: 91, 2022. DOI: 10.1007/JHEP04(2022)091. ÏÐÍÄ = 6,379*30*0,007 = 1,34
91. Tumasyan A. et al. (CMS Collaboration). Strategies and performance of the CMS silicon tracker alignment during LHC Run 2 // Nucl.Instrum.Meth.A 1037: 166795, 2022. DOI: 10.1016/j.nima.2022.166795. ÏÐÍÄ = 1,335*30*0,007 = 0,28
92. 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 // JHEP 4: 48, 2022. DOI: 10.1007/JHEP04(2022)048. ÏÐÍÄ = 6,379*30*0,007 = 1,34
93. Tumasyan A. et al. (CMS Collaboration). Addendum to: Measurement and QCD analysis of double-differential inclusive jet cross sections in proton-proton collisions at $ \sqrt{\textrm{s}} $ = 13 TeV // JHEP 12: 35, 2022. DOI: 10.1007/JHEP12(2022)035 , 10.1007/JHEP02(2022)142. ÏÐÍÄ = 6,379*30*0,007 = 1,34
94. 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 // JHEP 4: 87, 2022. DOI: 10.1007/JHEP04(2022)087. ÏÐÍÄ = 6,379*30*0,007 = 1,34
95. 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 // Phys.Rev.D105: 5, 052003, 2022. DOI: 10.1103/PhysRevD.105.052003. ÏÐÍÄ = 5,407*30*0,007 = 1,14
96. 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\,\text {TeV} $ // Eur.Phys.J.C82: 12, 1094, 2022. DOI: 10.1140/epjc/s10052-022-10897-7. ÏÐÍÄ = 4,991*30*0,007 = 1,05
97. 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 // JHEP 5: 5, 2022. DOI: 10.1007/JHEP05(2022)005. ÏÐÍÄ = 6,379*30*0,007 = 1,34
98. 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 // JHEP 4: 47, 2022. DOI: 10.1007/JHEP04(2022)047. ÏÐÍÄ = 6,379*30*0,007 = 1,34
99. Tumasyan A. et al. (CMS Collaboration). Evidence for WW/WZ vector boson scattering in the decay channel ??qq produced in association with two jets in proton-proton collisions at s=13 TeV // Phys.Lett.B834: 137438, 2022. DOI: 10.1016/j.physletb.2022.137438. ÏÐÍÄ = 4,950*30*0,007 = 1,04
100. Tumasyan A. et al. (CMS Collaboration). Measurement of the inclusive $ \mathrm{t}\overline{\mathrm{t}} $ production cross section in proton-proton collisions at $ \sqrt{s} $ = 5.02 TeV // JHEP 4: 144, 2022. DOI: 10.1007/JHEP04(2022)144. ÏÐÍÄ = 6,379*30*0,007 = 1,34
101. 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 // Phys.Rev.D105: 9, 092014, 2022. DOI: 10.1103/PhysRevD.105.092014. ÏÐÍÄ = 5,407*30*0,007 = 1,14
102. Tumasyan A. et al. (CMS Collaboration). Search for flavor-changing neutral current interactions of the top quark and the Higgs boson decaying to a bottom quark-antiquark pair at $ \sqrt{s} $ = 13 TeV // JHEP 2: 169, 2022. DOI: 10.1007/JHEP02(2022)169. ÏÐÍÄ = 6,379*30*0,007 = 1,34
103. Tumasyan A. et al. (CMS Collaboration). Search for resonant production of strongly coupled dark matter in proton-proton collisions at 13 TeV // JHEP 6: 156, 2022. DOI: 10.1007/JHEP06(2022)156. ÏÐÍÄ = 6,379*30*0,007 = 1,34
104. Tumasyan A. et al. (CMS Collaboration). Probing Charm Quark Dynamics via Multiparticle Correlations in Pb-Pb Collisions at $\sqrt{s_\mathrm{NN}}$ =5.02 TeV // Phys.Rev.Lett. 129: 2, 022001, 2022. DOI: 10.1103/PhysRevLett.129.022001. ÏÐÍÄ = 9,185*30*0,007 = 1,93
105. Tumasyan A. et al. (CMS Collaboration). Search for resonances decaying to three $W$ bosons in the hadronic final state in proton-proton collisions at $\sqrt s$ =13 TeV // Phys.Rev.D106: 1, 012002, 2022. DOI: 10.1103/PhysRevD.106.012002. ÏÐÍÄ = 5,407*30*0,007 = 1,14
106. Tumasyan A. et al. (CMS Collaboration). Search for long-lived particles decaying into muon pairs in proton-proton collisions at $ \sqrt{s} $ = 13 TeV collected with a dedicated high-rate data stream // JHEP 4: 62, 2022. DOI: 10.1007/JHEP04(2022)062. ÏÐÍÄ = 6,379*30*0,007 = 1,34
107. Tumasyan A. et al. (CMS Collaboration). Search for high-mass resonances decaying to a jet and a Lorentz-boosted resonance in proton-proton collisions at s=13TeV // Phys.Lett.B832: 137263, 2022. DOI: 10.1016/j.physletb.2022.137263. ÏÐÍÄ = 4,950*30*0,007 = 1,04
108. Tumasyan A. et al. (CMS Collaboration). Search for single production of a vector-like T quark decaying to a top quark and a Z boson in the final state with jets and missing transverse momentum at $ \sqrt{s} $ = 13 TeV // JHEP 5: 93, 2022. DOI: 10.1007/JHEP05(2022)093. ÏÐÍÄ = 6,379*30*0,007 = 1,34
109. Tumasyan A. et al. (CMS Collaboration). Observation of the $B_c^+$ Meson in Pb-Pb and pp Collisions at $\sqrt{s_{NN}}$=5.02??TeV and Measurement of its Nuclear Modification Factor // Phys.Rev.Lett. 128: 25, 252301, 2022. DOI: 10.1103/PhysRevLett.128.252301. ÏÐÍÄ = 9,185*30*0,007 = 1,93
110. Tumasyan A. et al. (CMS Collaboration). Search for higgsinos decaying to two Higgs bosons and missing transverse momentum in proton-proton collisions at $ \sqrt{s} $ = 13 TeV // JHEP 5: 14, 2022. DOI: 10.1007/JHEP05(2022)014. ÏÐÍÄ = 6,379*30*0,007 = 1,34
111. Tumasyan A. et al. (CMS Collaboration). Search for long-lived heavy neutral leptons with displaced vertices in proton-proton collisions at $ \sqrt{\mathrm{s}} $ =13 TeV // JHEP 7: 81, 2022. DOI: 10.1007/JHEP07(2022)081. ÏÐÍÄ = 6,379*30*0,007 = 1,34
112. Tumasyan A. et al. (CMS Collaboration). Measurement of the inclusive and differential $\mathrm{t\bar{t}}\gamma$ cross sections in the dilepton channel and effective field theory interpretation in proton-proton collisions at $\sqrt{s}$ =13 TeV // JHEP 5: 91, 2022. DOI: 10.1007/JHEP05(2022)091. ÏÐÍÄ = 6,379*30*0,007 = 1,34
113. Tumasyan A. et al. (CMS Collaboration). Search for charged-lepton flavor violation in top quark production and decay in pp collisions at $ \sqrt{s} $ = 13 TeV // JHEP 6: 82, 2022. DOI: 10.1007/JHEP06(2022)082. ÏÐÍÄ = 6,379*30*0,007 = 1,34
114. Tumasyan A. et al. (CMS Collaboration). Precision measurement of the W boson decay branching fractions in proton-proton collisions at $\sqrt{s}$ = 13 TeV // Phys.Rev.D105: 7, 072008, 2022. DOI: 10.1103/PhysRevD.105.072008. ÏÐÍÄ = 5,407*30*0,007 = 1,14
115. Tumasyan A. et al. (CMS Collaboration). Identification of hadronic tau lepton decays using a deep neural network // JINST 17: P07023, 2022. DOI: 10.1088/1748-0221/17/07/P07023. ÏÐÍÄ = 1,121*30*0,007 = 0,24
116. Tumasyan A. et al. (CMS Collaboration). Search for resonances decaying to three W bosons in proton-proton collisions at $\sqrt{s}$ = 13 TeV // Phys.Rev.Lett. 129: 2, 021802, 2022. DOI: 10.1103/PhysRevLett.129.021802. ÏÐÍÄ = 9,185*30*0,007 = 1,93
117. Tumasyan A. et al. (CMS Collaboration). Observation of B$^0$$\to$$\psi$(2S)K$^0_\mathrm{S}\pi^+\pi^-$ and B$^0_\mathrm{S}$$\to$$\psi$(2S)K$^0_\mathrm{S}$ decays // Eur.Phys.J.C82: 499, 2022. DOI: 10.1140/epjc/s10052-022-10315-y. ÏÐÍÄ = 4,991*30*0,007 = 1,05
118. Tumasyan A. et al. (CMS Collaboration). Search for invisible decays of the Higgs boson produced via vector boson fusion in proton-proton collisions at s=13??TeV // Phys.Rev.D105: 9, 092007, 2022. DOI: 10.1103/PhysRevD.105.092007. ÏÐÍÄ = 5,407*30*0,007 = 1,14
119. Tumasyan A. et al. (CMS Collaboration). Search for new physics in the lepton plus missing transverse momentum final state in proton-proton collisions at $\sqrt{s} =$ 13 TeV // JHEP 7: 67, 2022. DOI: 10.1007/JHEP07(2022)067. ÏÐÍÄ = 6,379*30*0,007 = 1,34
120. Tumasyan A. et al. (CMS Collaboration). Measurement of the Higgs boson width and evidence of its off-shell contributions to ZZ production // Nature Phys. 18: 11, 1329-1334, 2022. DOI: 10.1038/s41567-022-01682-0. ÏÐÍÄ = 19,684*30*0,007 = 4,13
121. Tumasyan A. et al. (CMS Collaboration). Inclusive nonresonant multilepton probes of new phenomena at $\sqrt s$=13??TeV // Phys.Rev.D105: 11, 112007, 2022. DOI: 10.1103/PhysRevD.105.112007. ÏÐÍÄ = 5,407*30*0,007 = 1,14
122. Tumasyan A. et al. (CMS Collaboration). Search for Higgs Boson Pair Production in the Four b Quark Final State in Proton-Proton Collisions at s=13??TeV // Phys.Rev.Lett. 129: 8, 081802, 2022. DOI: 10.1103/PhysRevLett.129.081802. ÏÐÍÄ = 9,185*30*0,007 = 1,93
123. Tumasyan A. et al. (CMS Collaboration). Nuclear modification of $\Upsilon$ states in pPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV // Phys.Lett.B835: 137397, 2022. DOI: 10.1016/j.physletb.2022.137397. ÏÐÍÄ = 4,950*30*0,007 = 1,04
124. Tumasyan A. et al. (CMS Collaboration). Measurement of the Drell-Yan forward-backward asymmetry at high dilepton masses in proton-proton collisions at $\sqrt{s}$ = 13 TeV // JHEP 8: 63, 2022. DOI: 10.1007/JHEP08(2022)063. ÏÐÍÄ = 6,379*30*0,007 = 1,34
125. Tumasyan A. et al. (CMS Collaboration). Search for a W? boson decaying to a vector-like quark and a top or bottom quark in the all-jets final state at $ \sqrt{\mathrm{s}} $ = 13 TeV // JHEP 9: 88, 2022. DOI: 10.1007/JHEP09(2022)088. ÏÐÍÄ = 6,379*30*0,007 = 1,34
126. Tumasyan A. et al. (CMS Collaboration). Search for new particles in an extended Higgs sector with four b quarks in the final state at s=13TeV // Phys.Lett.B835: 137566, 2022. DOI: 10.1016/j.physletb.2022.137566. ÏÐÍÄ = 4,950*30*0,007 = 1,04
127. (CMS Collaboration). A portrait of the Higgs boson by the CMS experiment ten years after the discovery // Nature 607: 7917, 60-68, 2022. DOI: 10.1038/s41586-022-04892-x. ÏÐÍÄ = 69,504*30*0,007 = 14,60
128. Grippo M. et al. (CMS Collaboration). Wafer-level testing of the readout chip of the CMS Inner Tracker for HL-LHC // Nucl.Instrum.Meth.A 1044: 167496, 2022. DOI: 10.1016/j.nima.2022.167496. ÏÐÍÄ = 1,335*30*0,007 = 0,28
129. Isik C. et al. (CMS Collaboration). Phase 1 upgrade of the CMS Hadron Barrel Calorimeter // Nucl.Instrum.Meth.A 1042: 167389, 2022. DOI: 10.1016/j.nima.2022.167389. ÏÐÍÄ = 1,335*30*0,007 = 0,28
130. Wiehe M. et al. (CMS Collaboration). The CMS high granularity calorimeter for the High Luminosity LHC // Nucl.Instrum.Meth.A 1041: 167312, 2022. DOI: 10.1016/j.nima.2022.167312. ÏÐÍÄ = 1,335*30*0,007 = 0,28
131. Damanakis K. et al. (CMS Collaboration). Silicon sensors for the Phase-2 upgrade of the CMS Outer Tracker; status and early results from the production phase // Nucl.Instrum.Meth.A 1040: 167034, 2022. DOI: 10.1016/j.nima.2022.167034. ÏÐÍÄ = 1,335*30*0,007 = 0,28
132. Auzinger G. et al. (CMS Collaboration). High-precision luminosity instrumentation for the CMS detector at the HL-LHC // Nucl.Instrum.Meth.A 1039: 167024, 2022. DOI: 10.1016/j.nima.2022.167024. ÏÐÍÄ = 1,335*30*0,007 = 0,28
133. Zuolo D. et al. (CMS Collaboration). Characterization of planar and 3D silicon pixel sensors for the high luminosity phase of the CMS experiment at LHC // Nucl.Instrum.Meth.A 1039: 167029, 2022. DOI: 10.1016/j.nima.2022.167029. ÏÐÍÄ = 1,335*30*0,007 = 0,28
134. Lanyov A. et al. (CMS Collaboration). Electroweak Measurements at CMS // Moscow Univ.Phys.Bull. 77: 2, 228-231, 2022. DOI: 10.3103/S0027134922020576. ÏÐÍÄ = 0,536*60*0,007 = 0,23
135. Kole G. et al. (CMS Collaboration). Search for Additional Higgs Boson with CMS Detector at LHC // Moscow Univ.Phys.Bull. 77: 2, 223-225, 2022. DOI: 10.3103/S0027134922020527. ÏÐÍÄ = 0,536*60*0,007 = 0,23
136. Kaur A. et al. (CMS Collaboration). Exotic Physics Signatures at CMS // Moscow Univ.Phys.Bull. 77: 2, 216-219, 2022. DOI: 10.3103/S0027134922020473. ÏÐÍÄ = 0,536*60*0,007 = 0,23
137. Tulupov A. et al. (CMS Collaboration). B-Physics Results from CMS // Moscow Univ.Phys.Bull. 77: 2, 263-267, 2022. DOI: 10.3103/S0027134922021004. ÏÐÍÄ = 0,536*60*0,007 = 0,23
138. Petrushanko S. et al. (CMS Collaboration). Heavy-Ion Physics at CMS // Moscow Univ.Phys.Bull. 77: 2, 247-249, 2022. DOI: 10.3103/S0027134922020801. ÏÐÍÄ = 0,536*60*0,007 = 0,23
139. Mazza G. et al. (CMS Collaboration). CMS ECAL upgrade for precision timing and energy measurements at the High-Luminosity LHC // Nucl.Instrum.Meth.A 1038: 166949, 2022. DOI: 10.1016/j.nima.2022.166949. ÏÐÍÄ = 1,335*30*0,007 = 0,28
140. Cooke C. et al. (CMS Collaboration). Upgrade of the CMS Barrel Electromagnetic Calorimeter for the High Luminosity LHC // Instruments 6: 3, 29, 2022. DOI: 10.3390/instruments6030029. ÏÐÍÄ = 8*0,007 = 0,06
141. Ferrero M. et al. (CMS Collaboration). The CMS MTD Endcap Timing Layer: Precision timing with Low Gain Avalanche Diodes // Nucl.Instrum.Meth.A 1032: 166627, 2022. DOI: 10.1016/j.nima.2022.166627. ÏÐÍÄ = 1,335*30*0,007 = 0,28
142. Sosnov D. et al. (CMS Collaboration). First Observation of Diffractive Processes in Proton-Lead Collisions at the LHC with the CMS Detector // Phys.Part.Nucl. 53: 2, 393-397, 2022. DOI: 10.1134/S1063779622020782. ÏÐÍÄ = 0,786*60*0,007 = 0,33
143. Das P. et al. (CMS Collaboration). An overview of the trigger system at the CMS experiment // Phys.Scripta 97: 5, 054008,, 2022. DOI: 10.1088/1402-4896/ac6302. ÏÐÍÄ = 3,081*30*0,007 = 0,65
144. Simone F.M. et al. (CMS Collaboration). Recent CMS heavy flavor physics results // Int.J.Mod.Phys.A37: 07, 2240003, 2022. DOI: 10.1142/S0217751X22400036. ÏÐÍÄ = 1,475*30*0,007 = 0,31
145. Aruta C. et al. (CMS Collaboration). Overview and recent results of the CMS muon system upgrade // Int.J.Mod.Phys.A37: 07, 2240008, 2022. DOI: 10.1142/S0217751X22400085. ÏÐÍÄ = 1,475*30*0,007 = 0,31
Ïðåïðèíòû:
1. 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
2. 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
3. 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
4. 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
Èòîãî: ÏÐÍÄ = 178,55
Ñóììàðíûé ÏÐÍÄ (çà 2021-2022 ãã.) = 208,67