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[PDF] Top 20 Production of light-flavor hadrons in pp collisions at $\sqrt{s}~=~7\text { and }\sqrt{s} = 13 \, \text { TeV} $

Has 10000 "Production of light-flavor hadrons in pp collisions at $\sqrt{s}~=~7\text { and }\sqrt{s} = 13 \, \text { TeV} $" found on our website. Below are the top 20 most common "Production of light-flavor hadrons in pp collisions at $\sqrt{s}~=~7\text { and }\sqrt{s} = 13 \, \text { TeV} $".

Production of light-flavor hadrons in pp collisions at $\sqrt{s}~=~7\text { and }\sqrt{s} = 13 \, \text { TeV} $

Production of light-flavor hadrons in pp collisions at $\sqrt{s}~=~7\text { and }\sqrt{s} = 13 \, \text { TeV} $

... 6.1 Scaling properties of hadron production Two kinds of universal scaling of identified particle production have been observed in high energy pp collisions: transverse mass m T scaling[r] ... Voir le document complet

42

Multiplicity dependence of $\pi $, K, and p production in pp collisions at $\sqrt{s} = 13$ TeV

Multiplicity dependence of $\pi $, K, and p production in pp collisions at $\sqrt{s} = 13$ TeV

... versions of the two MC generators. In particular, the hadronization in P YTHIA 8 now considers overlapping color strings, which form color ropes with a larger effective string tension and are ... Voir le document complet

27

D-meson production in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV and in pp collisions at $\sqrt{s}=7$ TeV

D-meson production in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV and in pp collisions at $\sqrt{s}=7$ TeV

... modification of heavy-flavour hadron yields and momentum ...presence of significant final-state effects in high-multiplicity p–Pb collisions is suggested by different observations, ... Voir le document complet

43

Multiplicity dependence of (anti-)deuteron production in pp collisions at $\sqrt{s}$ = 7 TeV

Multiplicity dependence of (anti-)deuteron production in pp collisions at $\sqrt{s}$ = 7 TeV

... TPC, and via the measurement of the time-of-flight of the particles, performed with the ...acceptance of the two detectors, the TPC is used with- out the TOF for p T < 1 GeV/c, where ... Voir le document complet

24

Jet-associated deuteron production in pp collisions at $\sqrt{s}=13$ TeV

Jet-associated deuteron production in pp collisions at $\sqrt{s}=13$ TeV

... Measurements of deuterons in high-energy collisions provide insight into baryon production and baryon transport mechanisms which are sensitive to the space–time evolution of the ... Voir le document complet

18

Dielectron production in proton-proton collisions at $ \sqrt{s}=7 $ TeV

Dielectron production in proton-proton collisions at $ \sqrt{s}=7 $ TeV

... challenging at the LHC due to the dominant contribution of e + e − pairs from semileptonic decays of charm and beauty hadrons, correlated through flavour conservation 1 ...[16–20] ... Voir le document complet

40

Measurement of ${{\mathrm{D}}^0}$ , ${{\mathrm{D}}^+}$ , ${{\mathrm{D}}^{*+}}$ and ${{\mathrm{D}}^+_{\mathrm{s}}}$ production in pp collisions at ${\sqrt{{\textit{s}}}~=~5.02~{\text {TeV}}}$ with ALICE

Measurement of ${{\mathrm{D}}^0}$ , ${{\mathrm{D}}^+}$ , ${{\mathrm{D}}^{*+}}$ and ${{\mathrm{D}}^+_{\mathrm{s}}}$ production in pp collisions at ${\sqrt{{\textit{s}}}~=~5.02~{\text {TeV}}}$ with ALICE

... study of the production of hadrons containing heavy quarks, ...charm and beauty, in proton–proton (pp) collisions at LHC energies is a sensitive test ... Voir le document complet

32

Measurement of the $B^{\pm}$ production cross-section in pp collisions at $\sqrt{s} =$ 7 and 13 TeV

Measurement of the $B^{\pm}$ production cross-section in pp collisions at $\sqrt{s} =$ 7 and 13 TeV

... valid in the high p T region, with a full massive fixed-order calculation, reliable in the small p T ...ratio of cross-sections between different centre-of-mass energies is of ... Voir le document complet

25

Production of associated $\Upsilon$ and open charm hadrons in $pp$ collisions at $\sqrt{s}=7$ and $8$TeV via double parton scattering

Production of associated $\Upsilon$ and open charm hadrons in $pp$ collisions at $\sqrt{s}=7$ and $8$TeV via double parton scattering

... A. Lupato 22 , E. Luppi 16,f , O. Lupton 55 , A. Lusiani 23 , F. Machefert 7 , F. Maciuc 29 , O. Maev 30 , K. Maguire 54 , S. Malde 55 , A. Malinin 64 , G. Manca 7 , G. Mancinelli 6 , P. Manning 59 , A. ... Voir le document complet

39

Prompt charm production in pp collisions at sqrt(s)=7 TeV

Prompt charm production in pp collisions at sqrt(s)=7 TeV

... Measurements of the production cross-sections of charmed hadrons test the predictions of quantum chromodynamic (QCD) fragmentation and hadronisation ...calculations of ... Voir le document complet

27

Light vector meson production in pp collisions at sqrt(s) = 7 TeV

Light vector meson production in pp collisions at sqrt(s) = 7 TeV

... n and p 0 were tuned iteratively to the results of this ...distribution of η is based on preliminary results from η production yields measured in the two-photon decay channel by ALICE ... Voir le document complet

18

(Anti-)deuteron production in pp collisions at $\sqrt{s}=13 \ \text {TeV}$

(Anti-)deuteron production in pp collisions at $\sqrt{s}=13 \ \text {TeV}$

... function of p T /A, being A = 2 the mass number of the deuteron. ities in different collisions systems and at different ...for pp and p–Pb collisions ... Voir le document complet

21

Measurement of $D_s^{\pm}$ production asymmetry in $pp$ collisions at $\sqrt{s} =7$ and 8 TeV

Measurement of $D_s^{\pm}$ production asymmetry in $pp$ collisions at $\sqrt{s} =7$ and 8 TeV

... C. Marin Benito 38 , M. Marinangeli 41 , P. Marino 41 , J. Marks 12 , G. Martellotti 26 , M. Martin 6 , M. Martinelli 41 , D. Martinez Santos 39 , F. Martinez Vidal 71 , A. Massafferri 1 , R. Matev 40 , A. Mathad 50 , Z. ... Voir le document complet

22

Measurement of charged particle spectra in minimum-bias events from proton–proton collisions at $\sqrt{s}=13\,\text {TeV} $

Measurement of charged particle spectra in minimum-bias events from proton–proton collisions at $\sqrt{s}=13\,\text {TeV} $

... study of the properties of particle production without any selection bias arising from requiring the presence of a hard scattering (a selection known as “minimum bias”) is one of the ... Voir le document complet

28

Measurement of $\psi(2S)$ polarisation in $pp$ collisions at $\sqrt{s}=7$ TeV

Measurement of $\psi(2S)$ polarisation in $pp$ collisions at $\sqrt{s}=7$ TeV

... R. Vazquez Gomez 18 , P. Vazquez Regueiro 37 , C. V´ azquez Sierra 37 , S. Vecchi 16 , J.J. Velthuis 46 , M. Veltri 17,h , G. Veneziano 39 , M. Vesterinen 11 , B. Viaud 7 , D. Vieira 2 , M. Vieites Diaz 37 , X. ... Voir le document complet

22

Measurement of Dijet Azimuthal Decorrelations in pp Collisions at sqrt(s)=7 TeV

Measurement of Dijet Azimuthal Decorrelations in pp Collisions at sqrt(s)=7 TeV

... GeV and |y| < ...(x) of the interacting partons are roughly equal and the experimental acceptance for multijet production is in- ...creased. In this region where ...π ... Voir le document complet

18

Measurement of J/psi production in pp collisions at sqrt(s)=2.76 TeV

Measurement of J/psi production in pp collisions at sqrt(s)=2.76 TeV

... cross-check and assign a systematic uncertainty to the Monte Carlo determination of the muon identification efficiency, the single track muon identification efficiency is measured on data using a ... Voir le document complet

18

Electroweak production of two jets in association with a Z boson in proton–proton collisions at $\sqrt{s}= $ 13 $\,\text {TeV}$

Electroweak production of two jets in association with a Z boson in proton–proton collisions at $\sqrt{s}= $ 13 $\,\text {TeV}$

... Study of the hadronic and jet activity in Z + jet events Now that the presence of an SM signal is established, the properties of the hadronic activity in the selected events can ... Voir le document complet

33

Measurement of the B+- production cross-section in pp collisions at sqrt(s)=7 TeV

Measurement of the B+- production cross-section in pp collisions at sqrt(s)=7 TeV

... The LHCb collaboration R. Aaij 38 , C. Abellan Beteta 33,n , B. Adeva 34 , M. Adinolfi 43 , C. Adrover 6 , A. Affolder 49 , Z. Ajaltouni 5 , J. Albrecht 35 , F. Alessio 35 , M. Alexander 48 , G. Alkhazov 27 , P. Alvarez ... Voir le document complet

13

Measurements of prompt charm production cross-sections in $pp$ collisions at $\sqrt{s} = 13\,\mathrm{TeV}$

Measurements of prompt charm production cross-sections in $pp$ collisions at $\sqrt{s} = 13\,\mathrm{TeV}$

... consists of a hardware stage, which for this analysis randomly selects a pre-defined fraction of all beam-beam crossings, followed by a software ...Alignment and calibration is performed in ... Voir le document complet

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