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R. Arnaldi

Soʻnggi maʼlum muassasa:
Istituto Nazionale di Fisica Nucleare, Sezione di Torino
ORCID:
0000-0001-6698-9577
5
h-indeks
2
i10-indeksi
144
Iqtiboslar
45
Asarlar
Vaqt boʻyicha

Vaqt boʻyicha tahlil

Iqtibos sharhi

Yillar boʻyicha nashrlar (ustun) va iqtiboslar (chiziq)

  • Nashrlar
  • Iqtiboslar
0134501325385020172018201920202021202220232024202520262017: Nashrlar 2, Iqtiboslar 22018: Nashrlar 1, Iqtiboslar 32019: Nashrlar 2, Iqtiboslar 02020: Nashrlar 4, Iqtiboslar 102021: Nashrlar 5, Iqtiboslar 142022: Nashrlar 0, Iqtiboslar 322023: Nashrlar 3, Iqtiboslar 182024: Nashrlar 3, Iqtiboslar 362025: Nashrlar 1, Iqtiboslar 52026: Nashrlar 0, Iqtiboslar 13

Iqtibos tarixi

01325385020172018201920202021202220232024202520262017: Iqtiboslar 22018: Iqtiboslar 32019: Iqtiboslar 02020: Iqtiboslar 102021: Iqtiboslar 142022: Iqtiboslar 322023: Iqtiboslar 182024: Iqtiboslar 362025: Iqtiboslar 52026: Iqtiboslar 13

Nashr tarixi

0134520172018201920202021202220232024202520262017: Nashrlar 22018: Nashrlar 12019: Nashrlar 22020: Nashrlar 42021: Nashrlar 52022: Nashrlar 02023: Nashrlar 32024: Nashrlar 32025: Nashrlar 12026: Nashrlar 0

h-indeks evolyutsiyasi

Yillar boʻyicha jamlangan h-indeks

0134520172018201920202021202220232024202520262017: h-indeks 22018: h-indeks 22019: h-indeks 22020: h-indeks 32021: h-indeks 32022: h-indeks 42023: h-indeks 52024: h-indeks 52025: h-indeks 52026: h-indeks 5

Eng koʻp iqtibos qilingan asarlar

  1. W and Z boson production in p-Pb collisions at s N N = 5.02 $$ \sqrt{s_{\mathrm{NN}}}=5.02 $$ TeV20170 iqtibos
  2. Measurement of the fraction of jet longitudinal momentum carried by <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msubsup><mml:mi mathvariant="normal">Λ</mml:mi><mml:mi>c</mml:mi><mml:mo>+</mml:mo></mml:msubsup></mml:math> baryons in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>p</mml:mi><mml:mi>p</mml:mi></mml:math> collisions20240 iqtibos
  3. Measurement of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msubsup><mml:mi mathvariant="normal">Ω</mml:mi><mml:mi mathvariant="normal">c</mml:mi><mml:mn>0</mml:mn></mml:msubsup></mml:math> baryon production and branching-fraction ratio <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>BR</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:msubsup><mml:mi mathvariant="normal">Ω</mml:mi><mml:mi mathvariant="normal">c</mml:mi><mml:mn>0</mml:mn></mml:msubsup><mml:mo stretchy="false">→</mml:mo><mml:msup><mml:mi mathvariant="normal">Ω</mml:mi><mml:mo>−</mml:mo></mml:msup><mml:msup><mml:mi mathvariant="normal">e</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:msub><mml:mi>ν</mml:mi><mml:mi mathvariant="normal">e</mml:mi></mml:msub><mml:mo stretchy="false">)</mml:mo><mml:mo>/</mml:mo><mml:mi>BR</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:msubsup><mml:mi mathvariant="normal">Ω</mml:mi><mml:mi mathvariant="normal">c</mml:mi><mml:mn>0</mml:mn></mml:msubsup><mml:mo stretchy="false">→</mml:mo><mml:msup><mml:mi mathvariant="normal">Ω</mml:mi><mml:mo>−</mml:mo></mml:msup><mml:msup><mml:mi>π</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:mo stretchy="false">)</mml:mo></mml:math> in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>p</mml:mi><mml:mi>p</mml:mi></mml:math> collisions at <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msqrt><mml:mi>s</mml:mi></mml:msqrt><mml:mo>=</mml:mo><mml:mn>13</mml:mn><mml:mtext> </mml:mtext><mml:mtext> </mml:mtext><mml:mi>TeV</mml:mi></mml:math>20240 iqtibos
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