- and p- - interaction measurements with femtoscopy in ALICE - PowerPoint PPT Presentation

Λ-Λ and p-Ξ - interaction measurements with femtoscopy in ALICE VALENTINA MA VA MANTOVANI SA SARTI FO FOR THE ALICE COLLABORATION PHYSI PH SIK-DE DEPARTMENT NT - TE TECHNISCHE UN UNIVERSITÄT MÜ MÜNCHEN QNP SATELLIT QN ITE WORKSHO HOP – TO TOKAI CAMPUS 11 NOVEMBER 2018 0 Va Valentina Ma Mantovani Sa Sarti (T (TUM P Physics D Department – E6 E62) 11.11. 11. 11.18 18 – QN QNP18 Satellite Worksho hop p (Tokai)

Outline 1. Hyperon-Nucleon and Hyperon-Hyperon interactions in Neutron Stars 2. Femtoscopy at ALICE experiment 3. Results pp 13 TeV and p-Pb 5.02 TeV ◦ Λ-Λ correlation function and the existence of H di-baryon ◦ First observation of the p-Ξ - strong attractive potential 4. Summary and Outlooks 3 Valentina Ma Va Mantovani Sa Sarti (T (TUM P Physics D Department – E6 E62) 11.11. 11. 11.18 18 – QN QNP18 Satellite Worksho hop p (Tokai)

Hyperon Puzzle in Neutron Stars • Hyperons production becomes energetically The appearance of Hyperons softens the EoS • favorable at moderate-large densities in dense neutron-rich matter • Threshold strongly depends on the Y-N interaction D. Lonardoni, A. Lovato, S. Gandolfi, F. Pederiva Phys. Rev. Lett. 114, 092301 (2015) 5 Valentina Ma Va Mantovani Sa Sarti (T (TUM P Physics D Department – E6 E62) 11.11. 11. 11.18 18 – QN QNP18 Satellite Worksho hop p (Tokai)

Hyperon Puzzle in Neutron Stars • Hyperons production becomes energetically The appearance of Hyperons softens the EoS • favorable at moderate-large densities in dense neutron-rich matter Maximum NS masses get smaller ⇒ HYPERON PUZZLE • • Threshold strongly depends on the Y-N interaction TOV D. Lonardoni, A. Lovato, S. Gandolfi, F. Pederiva Phys. Rev. Lett. 114, 092301 (2015) 6 Va Valentina Ma Mantovani Sa Sarti (T (TUM P Physics D Department – E6 E62) 11.11. 11. 11.18 18 – QN QNP18 Satellite Worksho hop p (Tokai)

YN and YY interactions: the traditional ways Scattering experiments / Hypernuclei data • ? SCATTERING DATA: • Constraint only on pΛ/pΣ interaction • Exp Data from scattering experiments from 1968 and • LO 1971 in bubble chambers NLO Production threshold: p LAB ≳ 100 MeV • LO: H. Polinder, J.H., U. Meiβner, NPA 779 (2006) 244 NLO: J.Haidenbauer., N.Kaiser, et al., NPA 915 (2013) 24 7 Va Valentina Ma Mantovani Sa Sarti (T (TUM P Physics D Department – E6 E62) 11.11. 11. 11.18 18 – QN QNP18 Satellite Worksho hop p (Tokai)

YN and YY interactions: scattering experiments Scattering experiments / Hypernuclei data • ? SCATTERING DATA: • Constraint only on pΛ/pΣ interaction • Exp Data from scattering experiments from 1968 and • LO 1971 in bubble chambers NLO Production threshold: p LAB ≳ 100 MeV • Cannot probe low momentum region • LO: ALWAYS ATTRACTIVE NLO: BECOMES REPULSIVE ⇒ REPULSIVE CORE LO: H. Polinder, J.H., U. Meiβner, NPA 779 (2006) 244 NLO: J.Haidenbauer., N.Kaiser, et al., NPA 915 (2013) 24 8 Va Valentina Ma Mantovani Sa Sarti (T (TUM P Physics D Department – E6 E62) 11.11. 11. 11.18 18 – QN QNP18 Satellite Worksho hop p (Tokai)

YN and YY interactions: hypernuclei HYPERNUCLEI DATA: • Λ hypernuclei data: B Λnucleus = 30 MeV • Ξ hypernuclei data show shallow attractive • interaction [Kiso Evt] ΛΛ hypernuclei exist as well showing weakly • attraction [Nagara Evt] Σ hypernuclei: nothing known so far! • 9 Va Valentina Ma Mantovani Sa Sarti (T (TUM P Physics D Department – E6 E62) 11.11. 11. 11.18 18 – QN QNP18 Satellite Worksho hop p (Tokai)

YN and YY interactions: hypernuclei HYPERNUCLEI DATA: • Λ hypernuclei data: B λnucleus = 30 MeV [ref] • Ξ hypernuclei data show shallow attractive • interaction [Kiso Evt] ΛΛ hypernuclei exist as well showing weakly • attraction [Nagara Evt] Σ hypernuclei: nothing known so far! • 10 Va Valentina Ma Mantovani Sa Sarti (T (TUM P Physics D Department – E6 E62) 11.11. 11. 11.18 18 – QN QNP18 Satellite Worksho hop p (Tokai)

Take home message • Hyperon-nucleon and hyperon-hyperon interactions are fundamental ingredients for the EoS of NSs but unfortunately already in vacuum they are still not well fully understood • Scattering experiments cannot be applied to all hyperon species and cannot access the low-momentum range • Hypernuclei experiments are based on single events and their interpretation is model dependent • How can we do the next step? Femtoscopy 11 Valentina Ma Va Mantovani Sa Sarti (T (TUM P Physics D Department – E6 E62) 11.11. 11. 11.18 18 – QN QNP18 Satellite Worksho hop p (Tokai)

Basics of Femtoscopy Source function !(# ⃗) & ' # Ψ(*, # ⃗) & ( two particle wave function § Look for particle pairs § Measure the relative momentum * distribution in your experimental set up § Search for correlations 12 Va Valentina Ma Mantovani Sa Sarti (T (TUM P Physics D Department – E6 E62) 11.11. 11. 11.18 18 – QN QNP18 Satellite Worksho hop p (Tokai)

Key observable: the correlation function Source function 8(9 ⃗) % ' 9 Ψ(", 9 ⃗) % ) two particle wave function Statistical definition Experimental definition Theoretical definition >→@ 1 $ % ⃗ ' , % ⃗ ) = * + ,-./ (") ; d = 9 ! " = + 234/5 (") = 7 8 9 ⃗ Ψ ", 9 ⃗ ⃗ $ % ⃗ ' $ % ⃗ ) Relative distance / reduced momentum in Single-particle momenta the rest frame of the pair Lisa, Pratt, Wiedemann,Solz, Ann.Rev.Nucl.Part.Sci. 55 (2005) 357-402 13 Valentina Ma Va Mantovani Sa Sarti (T (TUM P Physics D Department – E6 E62) 11.11. 11. 11.18 18 – QN QNP18 Satellite Worksho hop p (Tokai)

Femtoscopy at A L arge I on C ollider E xperiment We measure p-p , p-Λ , Λ-Λ , p-Ξ • Proton identification with TPC and TOF • " Reconstruction of hyperons $ • ! Λ → '( ) (BR ~ 64%) • Ξ ) → Λ( ) (BR ~ 100%) • " # Datasets: • 3.4·10 8 Events pp 7 TeV: • 10·10 8 Events pp 13 TeV: • 6.0·10 8 Events p-Pb 5.02 TeV: • Assumption of a common Gaussian source • ⇒ fixing the radius from p-p 8→9 1 5 d 7 1 ⇒ p- L , p- X and L-L Correlation Function to , - = / 0 1 ⃗ Ψ -, 1 ⃗ ⃗ study the interaction 16 Valentina Ma Va Mantovani Sa Sarti (T (TUM P Physics D Department – E6 E62) 11. 11.11. 11.18 18 – QN QNP18 Satellite Worksho hop p (Tokai)

Lednicky Model Source Potential Analytic Transport model Full Scattering parameters Numerically solve Eff. range expansion the Schrödinger eq. => phase shifts “ Exact ” solution Approximate solution Wave function Correlation function Depends on scattering parameters, might locally break down for small sources 2 0 Valentina Ma Va Mantovani Sa Sarti (T (TUM P Physics D Department – E6 E62) 11.11. 11. 11.18 18 – QN QNP18 Satellite Worksho hop p (Tokai)

CATS – Correlation Analysis Tool Using the Schrödinger Equation Source Potential Full Analytic Transport model Scattering parameters Numerically solve the Eff. range expansion Schrödinger eq. => phase shifts “Exact” solution Approximate solution Wave function Correlation function 21 (D.L.Mihaylov et al. Eur.Phys.J. C78 (2018) no.5,394) 21 21 Valentina Ma Va Mantovani Sa Sarti (T (TUM P Physics D Department – E6 E62) 11.11. 11. 11.18 18 – QN QNP18 Satellite Worksho hop p (Tokai)

Length scales involved in Femtoscopy + .→0 d - ' ! " = % & ' ⃗ Ψ ", ' ⃗ ⃗ 1 § A-A collisions: 2 345ß ~ 4 fm § p-A collisions: 9 :;<ß ~ = fm § p-p collisions: 9 :;<ß ~ > fm 22 Va Valentina Ma Mantovani Sa Sarti (T (TUM P Physics D Department – E6 E62) 11.11. 11. 11.18 18 – QN QNP18 Satellite Worksho hop p (Tokai)

Correlation function and Interactions > 1 attraction C ( k ∗ ) − → = 1 no interaction < 1 repulsion J.Holt et al, Prog.Part.Nucl.Phys. 73 (2013) 23 Valentina Ma Va Mantovani Sa Sarti (T (TUM P Physics D Department – E6 E62) 11.11. 11. 11.18 18 – QN QNP18 Satellite Worksho hop p (Tokai)

- and p- - interaction measurements with femtoscopy in ALICE - PowerPoint PPT Presentation

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