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D. Schwarz

Исм вариантлари: Dennis Schwarz

Сўнгги маълум муассаса:
Institute of High Energy Physics
ORCID:
0000-0002-3821-7331
3
h-индекс
1
i10-индекси
55
Иқтибослар
133
Асарлар
Вақт бўйича

Вақт бўйича таҳлил

Иқтибос шарҳи

Йиллар бўйича нашрлар (устун) ва иқтибослар (чизиқ)

  • Нашрлар
  • Иқтибослар
013253850013253850202220232024202520262022: Нашрлар 5, Иқтибослар 02023: Нашрлар 38, Иқтибослар 52024: Нашрлар 32, Иқтибослар 52025: Нашрлар 42, Иқтибослар 342026: Нашрлар 16, Иқтибослар 11

Иқтибос тарихи

013253850202220232024202520262022: Иқтибослар 02023: Иқтибослар 52024: Иқтибослар 52025: Иқтибослар 342026: Иқтибослар 11

Нашр тарихи

013253850202220232024202520262022: Нашрлар 52023: Нашрлар 382024: Нашрлар 322025: Нашрлар 422026: Нашрлар 16

h-индекс эволюцияси

Йиллар бўйича жамланган h-индекс

01345202220232024202520262022: h-индекс 02023: h-индекс 12024: h-индекс 22025: h-индекс 32026: h-индекс 3

Энг кўп иқтибос қилинган асарлар

  1. The CMS Statistical Analysis and Combination Tool: Combine202433 иқтибос
  2. Search for pair production of vector-like quarks in leptonic final states in proton-proton collisions at $$ \sqrt{s} $$ = 13 TeV20231 иқтибос
  3. Measurements of Higgs boson production in the decay channel with a pair of $$\uptau $$ leptons in proton–proton collisions at $$\sqrt{s}=13$$ TeV20231 иқтибос
  4. Measurement of the top quark mass using a profile likelihood approach with the lepton + jets final states in proton–proton collisions at $$\sqrt{s}=13\,\text {Te}\hspace{-.08em}\text {V} $$20231 иқтибос
  5. Measurement of the top quark pole mass using $$ \textrm{t}\overline{\textrm{t}} $$+jet events in the dilepton final state in proton-proton collisions at $$ \sqrt{s} $$ = 13 TeV20231 иқтибос
  6. CMS pythia  8 colour reconnection tunes based on underlying-event data20231 иқтибос
  7. Search for long-lived particles decaying to leptons with large impact parameter in proton–proton collisions at $$\sqrt{s} = 13\,\text {Te}\text {V} $$20220 иқтибос
  8. Observation of B$$^0$$ $$\rightarrow $$ $$\uppsi $$(2S)K$$^0_\mathrm {S}\uppi ^+\uppi ^-$$ and B$$^0_\mathrm {s}$$ $$\rightarrow $$ $$\uppsi $$(2S)K$$^0_\mathrm {S}$$ decays20220 иқтибос
  9. Searches for additional Higgs bosons and for vector leptoquarks in ττ final states in proton-proton collisions at $$ \sqrt{s} $$ = 13 TeV20230 иқтибос
  10. A search for decays of the Higgs boson to invisible particles in events with a top-antitop quark pair or a vector boson in proton-proton collisions at $$\sqrt{s} = 13\,\text {Te}\hspace{-.08em}\text {V} $$20230 иқтибос