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

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

by D. D. Chinellato , A. Fantoni , H. Pereira Da Costa , Y. Schutz , J. L. Martinez , S. Panebianco , M. Pikna , C. Hadjidakis , M. Mazzilli , D. Andreou , L. K. Graczykowski , E. López Torres , R. Vernet , P. Bartalini , E. Ryabinkin , U. Dmitrieva , A. K. Pandey , B. Paul , A. Kravčáková , J. W. Myrcha , M. van Leeuwen , C. A. Pruneau , A. Kalweit , V. Petráček , R. E. Quishpe , R. Averbeck , A. M. Khan , M. J. Jakubowska , E. N. Umaka , C. Cicalo , M. Weber , N. Agrawal , A. Matyja , S. Sakai , M. Broz , A. De Caro , T. Lazareva , R. Bellwied , S. Ahmad , R. Bailhache , R. Tieulent , H. R. Schmidt , N. Kondratyeva , J. Takahashi , P. Dupieux , A. Shabetai , V. Zaccolo , B. Krimphoff , M. A. Mazzoni , S. Rajput , M. A. Lisa , I.-K. Yoo , K. Shigaki , F. Manso , C. Markert , A. R. Schmier , R. Caron , S. Chandra , P. González-Zamora , V. Manzari , N. A. Martin , L. Kumar , R. Renfordt , Ø. Djuvsland , S. Siddhanta , X. Zhang , K. Šafařík , S. Sambyal , A. D. C. Bell Hechavarria , L. Cifarelli , M. Krzewicki , D. Sekihata , A. De Falco , Y. Melikyan , A. Festanti , B. Mohanty , R. Arnaldi , V. Grabski , T. Herman , P. S. Rokita , T. Peitzmann , D. Mühlheim , K. Garner , R. Raniwala , G. Biro , M. Ogino , B. Sitar , P. Vande Vyvre , A. I. Sheikh , E.

2020

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

2020

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

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

2020

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

Journal Article

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

D. D. Chinellato,

A. Fantoni,

H. Pereira Da Costa,

Y. Schutz,

J. L. Martinez,

S. Panebianco,

M. Pikna,

C. Hadjidakis,

M. Mazzilli,

D. Andreou,

L. K. Graczykowski,

E. López Torres,

R. Vernet,

P. Bartalini,

E. Ryabinkin,

U. Dmitrieva,

A. K. Pandey,

B. Paul,

A. Kravčáková,

J. W. Myrcha,

M. van Leeuwen,

C. A. Pruneau,

A. Kalweit,

V. Petráček,

R. E. Quishpe,

R. Averbeck,

A. M. Khan,

M. J. Jakubowska,

E. N. Umaka,

C. Cicalo,

M. Weber,

N. Agrawal,

A. Matyja,

S. Sakai,

M. Broz,

A. De Caro,

T. Lazareva,

R. Bellwied,

S. Ahmad,

R. Bailhache,

R. Tieulent,

H. R. Schmidt,

N. Kondratyeva,

J. Takahashi,

P. Dupieux,

A. Shabetai,

V. Zaccolo,

B. Krimphoff,

M. A. Mazzoni,

S. Rajput,

M. A. Lisa,

I.-K. Yoo,

K. Shigaki,

F. Manso,

C. Markert,

A. R. Schmier,

R. Caron,

S. Chandra,

P. González-Zamora,

V. Manzari,

N. A. Martin,

L. Kumar,

R. Renfordt,

Ø. Djuvsland,

S. Siddhanta,

X. Zhang,

K. Šafařík,

S. Sambyal,

A. D. C. Bell Hechavarria,

L. Cifarelli,

M. Krzewicki,

D. Sekihata,

A. De Falco,

Y. Melikyan,

A. Festanti,

B. Mohanty,

R. Arnaldi,

V. Grabski,

T. Herman,

P. S. Rokita,

T. Peitzmann,

D. Mühlheim,

K. Garner,

R. Raniwala,

G. Biro,

M. Ogino,

B. Sitar,

P. Vande Vyvre,

A. I. Sheikh,

2020

Overview

Abstract The study of (anti-)deuteron production in pp collisions has proven to be a powerful tool to investigate the formation mechanism of loosely bound states in high-energy hadronic collisions. In this paper the production of $$\\text {(anti-)deuterons}$$ (anti-)deuterons is studied as a function of the charged particle multiplicity in inelastic pp collisions at $$\\sqrt{s}=13$$ s = 13 TeV using the ALICE experiment. Thanks to the large number of accumulated minimum bias events, it has been possible to measure (anti-)deuteron production in pp collisions up to the same charged particle multiplicity ( $${\\mathrm {d} N_{ch}/\\mathrm {d} \\eta } \\sim 26$$ d N ch / d η ∼ 26 ) as measured in p–Pb collisions at similar centre-of-mass energies. Within the uncertainties, the deuteron yield in pp collisions resembles the one in p–Pb interactions, suggesting a common formation mechanism behind the production of light nuclei in hadronic interactions. In this context the measurements are compared with the expectations of coalescence and statistical hadronisation models (SHM).

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