Measurements of the groomed jet radius and momentum splitting fraction with the soft drop and dynamical grooming algorithms in pp collisions at $$ \sqrt{s} $$ = 5.02 TeVS. Acharya, A. Balbino, A. Akindinov et al.|Journal of High Energy Physics|2023Cited by 12
Measurement of the production of charm jets tagged with D0 mesons in pp collisions at $$ \sqrt{s} $$ = 5.02 and 13 TeVS. Acharya, A. Balbino, D. Adamová et al.|Journal of High Energy Physics|2023Cited by 11
<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msup><mml:mi>K</mml:mi><mml:mo>*</mml:mo></mml:msup><mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:mn>892</mml:mn><mml:mo>)</mml:mo></mml:mrow><mml:mn>0</mml:mn></mml:msup></mml:mrow></mml:math> and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi>ϕ</mml:mi><mml:mo>(</mml:mo><mml:mn>1020</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math> production in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi>p</mml:mi><mml:mtext>−</mml:mtext><mml:mi>Pb</mml:mi></mml:math> collisions at <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msqrt><mml:msub><mml:mi>s</mml:mi><mml:mrow><mml:mi>N</mml:mi><mml:mi>N</mml:mi></mml:mrow></mml:msub></mml:msqrt><mml:mo>=</mml:mo><mml:mn>8.16</mml:mn><mml:mo> </mml:mo><mml:mi>TeV</mml:mi></mml:mrow></mml:math>S. Acharya, X. Bai, D. Adamová et al.|Physical Review C|2023Cited by 9
Measurement of inclusive and leading subjet fragmentation in pp and Pb–Pb collisions at $$ \sqrt{s_{\textrm{NN}}} $$ = 5.02 TeVS. Acharya, A. Balbino, D. Adamová et al.|Journal of High Energy Physics|2023Cited by 8
Measurement of ψ (2S) production as a function of charged-particle pseudorapidity density in pp collisions at $$ \sqrt{s} $$ = 13 TeV and p–Pb collisions at $$ \sqrt{s_{\textrm{NN}}} $$ = 8.16 TeV with ALICE at the LHCS. Acharya, A. Balbino, D. Adamová et al.|Journal of High Energy Physics|2023Cited by 6