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DOI 10.1393/ncc/i2017-17024-7 Colloquia: IFAE 2016

IL NUOVO CIMENTO 40 C (2017) 24

Hypertriton and exotic bound states production in Pb-Pb

collisions at the LHC with the ALICE experiment

S. Trogolofor the ALICE Collaboration

University and INFN, Sezione di Torino - Via Giuria 1, Torino, Italy

received 17 October 2016

Summary. — The ALICE Collaboration has studied the production of (anti-) hypertriton,3

ΛH, and the exotic bound states, H-dibaryon and Λn, in Pb-Pb

colli-sions at√sN N = 2.76 TeV. The data sample has been collected during the LHC

heavy-ion run at the end of 2011. The3ΛH has been studied via its two-body mesonic

weak decay (3

ΛH3He + π−), while the H-dibaryon and Λn through their Λ+p+π−

and d+π+ final states, respectively.

1. – Introduction

Heavy-ion collisions at LHC energies provide a unique opportunity to understand the nature of the medium (Quark-Gluon Plasma) created during the collision. In heavy-ion collisions many strange hadrons are produced and hyperon-baryon bound systems can be formed. There are two distinct approaches used to estimate the production yield of these systems: thermal model [1] and coalescence model [2].

H-dibaryon and Λn bound state discovery would provide crucial information on the Λ-nucleon and Λ-Λ interaction.

2. – Hypertriton

The hypertriton 3

ΛH is the lightest known hypernucleus and consists of a proton, a

neutron and a Λ. Its mass is 2.991 ± 0.002 GeV/c2 and its lifetime is expected to be

compatible with the free Λ lifetime. The 3

ΛH and 3ΛH production yield were measured

through their mesonic weak decay. Topological cuts were applied for the identification of secondary vertices and the production yield was extracted from the invariant-mass

distributions of (3He+π) and (3He + π+) pairs.

In the left panel of fig. 1 the measured production yield dN /dy × BR of 3

ΛH is

compared to different theoretical models as a function of the branching ratio (BR) of the two-body decay channel. Assuming a theoretical BR = 25% [3], the models in agreement

c

 CERN on behalf of the ALICE Collaboration

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2 S. TROGOLO for the ALICE COLLABORATION B.R. 0.15 0.2 0.25 0.3 0.35 x B.R. y /d N d 4 − 10 Data

Hybrid UrQMD Model

Thermal model GSI - Heidelberg SHARE 0-10% centrality = 2.76 TeV NN s Pb-Pb ) -π He+ 3 ( → H Λ 3 ALICE Hypertriton lifetime (ps) 0 100 200 300 400 500

R. J. Prem and P. H. Steinberg PR 136 (1964) B1803

R. E. Phillips and J. Schneps PR 180 (1969) 1307 G. Bohm et al. NPB 16 (1970) 46 G. Keyes et al. PRD 1 (1970) 66 G. Keyes et al. NPB 67(1973)269 STAR Collaboration Science 328 (2010)58 HypHI Collaboration NPA 913(2013)170 ALICE (PDG) Λ Free H World Average Λ 3

Fig. 1. – Left: dN /dy comparison to different models for the 3ΛH measurement. Right: 3ΛH

lifetime (τ ) measured by the ALICE Collaboration compared to the published results.

with the measured yield are the equilibrium statistical model (GSI-Heidelberg [1]), with

a temperature Tchem = 156 MeV, and the Hybrid UrQMD model [2], which combines

the hadronic transport approach with an initial hydrodynamical stage for the hot dense phase.

The total sample of3

ΛH and3ΛH has been divided into four intervals of ct = MLc/p.

M is the mass and it has been fixed to 2.991 GeV/c2, L is the decay length, c is the speed

of light and p is the particle momentum. An exponential fit to the dN /d(ct ) distribution

was performed to determine the proper decay length, which is cτ = 5.4+1.6−1.2(stat.) ± 1.0

(syst.)cm. In the right panel of fig. 1 the lifetime measured by ALICE, τ = 181+54−39(stat.)

± 33 (syst.) ps, is contrasted with the free Λ lifetime and with previous measurements

of the hypertriton lifetime. The orange band shows the statistical combination of the

experimental lifetime estimates available which leads to τ = 216+19−18 ps [4], in agreement

with ALICE measurement.

3. – Exotic bound states

The H-dibaryon is a hypothetical uuddss bound state (ΛΛ) first predicted by Jaffe [5]

using a bag model approach. In this analysis the Λpπ− decay channel of the H-dibaryon

was investigated, under the assumption of a weakly-bound state. Since no evidence of a signal for the H-dibaryon was found in the invariant mass distribution, an upper limit (99% CL) of dN /dy was obtained, assuming a BR = 64% and the free Λ lifetime.

The limit ∼ 3.0 × 10−4 is a factor 20 below values predicted by the thermal models

(dN /dy≈ 6 × 10−3).

The Λn bound state was investigated in the decay dπ+, but no signal was found in

the invariant mass distribution. Assuming a BR = 54% and the free Λ lifetime, this

led to an upper limit (99% CL) of dN /dy ∼ 2.0×10−3 that is a factor 20 below values

predicted by thermal models (dN /dy≈ 4 × 10−2).

A detailed description of the results on the hypertriton and the exotic bound states can be found in [6] and [7].

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HYPERTRITON AND EXOTIC BOUND STATES PRODUCTION IN Pb-Pb COLLISIONS ETC. 3

REFERENCES

[1] Andronic A. et al., Phys. Lett. B, 697 (2011) 203. [2] Steinheimer J. et al., Phys. Lett. B, 714 (2012) 85. [3] Gloeckle W. et al., Nucl. Phys. A, 639 (1998) 297. [4] Rappold C. et al., Phys. Lett. B, 728 (2014) 543.

[5] Jaffe R. L., Phys. Rev. Lett., 38 (1977) 195; 38 (1977) 617(E). [6] ALICE Collaboration, Phys. Lett. B, 754 (2016) 360. [7] ALICE Collaboration, Phys. Lett. B, 752 (2016) 267.

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