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from / production data and in-medium properties Shuntaro Sakai - - PowerPoint PPT Presentation

Study of interaction from / production data and in-medium properties Shuntaro Sakai (Institute of Theoretical Physics, CAS (Beijing,China)) Introduction - O rigin of the mass Anomaly-induced coupling U A (1)


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Study of η′𝑂 interaction from Ξ·/Ξ·β€² production data and in-medium Ξ·β€² properties

Shuntaro Sakai (Institute of Theoretical Physics, CAS (Beijing,China))

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Introduction

  • Origin of the η’ mass

←UA(1) anomaly and chiral symmetry breaking (3flavor)

η’-nucleon interaction = basic information

Moskal(2000), Czerwinski et al.(2014),… Borasoy (2000), Bass-Thomas (2006), Oset-Ramos (2011), S.S.-Jido(2013),

  • η’-nucleus system

Tsushima(2000),Nagahiro-Hirenzaki(2005),Nagahiro-Takizawa-Hirenzaki (2006),Jido-Nagahiro-Hirenzaki (2012), Tanaka et al. (2016),Metag-Naova-Paryev (2017),… Pisarski-Wilzek(1984), Kunihiro-Hatsuda(1988), Cohen (1996), Lee-Hatsuda (1996),…

  • η’ mass in finite density

Costa-Ruivo-Kalinovsky(2003), Kwon-Lee-Morita-Wolf(2012), Fejos-Hosaka(2017)…

 Study of η’-few nucleon system:

Sekihara-Fujioka-Ishikawa(2018) for η’d

s-wave η’p scattering length from ppοƒ ppη’

In-medium η’ as a probe of chiral symmetry in nuclear medium

Witten(1979),’t Hooft(1986),…

οƒŸ Chiral restoration in nuclear medium (reduction of order parameter of chiral symmetry breaking)

Anomaly-induced coupling

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Recent data on Ξ·/Ξ·β€² photoproduction

Ξ·β€²π‘ž threshold effect

A2 Collaboration at MAMI, PRL118(2017)212001

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  • Ξ·β€² photoproduction from proton

Data: A2 Collaboration at MAMI, PRL118(2017)212001

Near-threshold enhancement

  • - Comparison with phase space

Phase space

β–  N(1895) contribution: PRL118(2017)212001[A2 Collaboration], PLB785(2018)626[Anisovich et al.]

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SLIDE 5

from latest PDG [PRD98,030001(2018)]

Broad resonance @Ξ·β€²π‘ž threshold(=1896MeV)

  • Ο€Nοƒ Ο€N: PRC89(2014)045205[Svarc et al.]
  • Ξ³pοƒ K*Ξ›: PLB771(2017)142[CLAS Collab.]
  • Ξ³p and Ο€pοƒ KΞ›: EPJA53(2017)242[Anisovivh et al.]
  • Multichannel: PRL119(2017)062004[Anisovich et al.]
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SLIDE 6
  • Ξ· photoproduction from proton

MAID analysis: A2MAMI, PRL118(2017)212001 Partial-wave analysis: Anisovich et al, arxiv:1803.06814

Threshold effect

  • - Threshold effect: Flatte parametrization or K-matrix approach

Partial-wave analysiss-wave Ξ·β€²π‘ž scattering length

Anisovich et al., arxiv:1803.06814

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SLIDE 7

Threshold cusp

  • A simple t matrix with channel coupling:

(ΞΊ: real and positive)

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Extraction of the Ξ·β€²π‘ž amplitude from Ξ·/Ξ·β€²-photoproduction data

β–‘ Ξ·β€²π‘ž scattering length β–‘ Ξ·β€²-optical potential

  • - Focus on Ξ·β€²π‘ž-threshold behavior

 Focus on the Ξ·β€²π‘ž-threshold region (~100MeV around Ξ·β€²π‘ž threshold) Information on πœ½β€²π’’ amplitude (𝑁𝐢 can be Ξ·β€²π‘ž, Ξ·π‘ž, Ο€π‘ž, 𝐿Λ, 𝐿Σ, Ο‰π‘ž,…)

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Setup

〇 Final-State Interaction

= + +… β€» Resonance is not assumed in Ξ·(’)p amplitude

  • for channel coupling effect (Ο€π‘ž, 𝐿Λ, 𝐿Σ, Ο‰π‘ž)

~1.7GeV

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  • for Ξ·π‘ž and Ξ·β€²π‘ž
  • to take account of other channels

(Ο€π‘ž, 𝐿Λ, 𝐿Σ, Ο‰π‘ž,…)

Fit Ξ·/Ξ·β€²-photoproduction data in

  • : polynomial of 𝑑

(Ξ”<70MeV) Fit parameter -- Interaction kernel of Ξ·(β€²)π‘ž

  • - Ξ·(β€²)π‘ž production amplitude from photon

with

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Constraint on scattering amplitude

〇 Optical theorem

Restriction

a large number

can happen

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()

A simple test: fit Ξ³π‘ž β†’ Ξ·β€²π‘ž data with Ξ·β€²π‘ž FSI

with Flip sign below Ξ·β€²π‘ž threshold οƒŸ phase space οƒŸ fit Ξ·β€²π‘ž-threshold

Data: A2MAMI, PRL118(2017)212001

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SLIDE 13

𝑁𝐢 = Ξ·β€²π‘ž would be responsible for the enhancement

A simple test: fit Ξ³π‘ž β†’ Ξ·β€²π‘ž data with Ξ·β€²π‘ž FSI

with

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SLIDE 14

Results of Ξ³π‘ž β†’ Ξ·(β€²)π‘ž fitting

Fit

Ξ³π‘ž β†’ Ξ·π‘ž data: A2MAMI, PRL118(2017)212001 and CLAS, PRC80(2009)045213 Ξ³π‘ž β†’ Ξ·β€²π‘ž data: A2MAMI, PRL118(2017)212001

Ξ”=50-70MeV

Ξ” varied (nmax=1)

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Ξ·β€²π‘ž scattering amplitude

Flip sign below Ξ·β€²π‘ž threshold

π‘žπ‘ž β†’ π‘žπ‘žΞ·β€² [Czerwinski et al., PRL113, 062004(2014)]

Anisovich et al., arxiv:1803.06814

Ξ·β€²π‘ž-threshold (Ξ”=60MeV) β€»Error of parameters: ~10%

Ξ” varied (nmax=1)

  • - pole~(1877-63i)MeV(Ξ”=60MeV)

〇 Too far away from real axis…

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Results of Ξ³π‘ž β†’ Ξ·(β€²)π‘ž fitting

nmax varied

Fit (Ξ”=60MeV fixed)

  • : polynomial of 𝑑
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Ξ·β€²π‘ž-threshold

nmax varied (Ξ”=60MeV)

Ξ·β€²π‘ž scattering amplitude

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Ξ” varied

(Ξ”=30MeV)

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Ξ·β€²-optical potential @ρ = ρ0

Ξ” varied (nmax=1)

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SLIDE 20

Ξ·β€²-optical potential @ρ = ρ0

nmax varied (Ξ”=60MeV)

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Ξ” varied

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Summary

  • Analysis of Ξ·/Ξ·β€² photoproduction data

with Ξ·(β€²)π‘ž Final-State Interaction

  • Threshold effect
  • Near-threshold enhancement in Ξ³π‘ž β†’ Ξ·β€²π‘ž
  • Cusp of Ξ³π‘ž β†’ Ξ·π‘ž cross section @Ξ·β€²π‘ž thr.
  • For s-wave Ξ·β€²π‘ž scattering length,
  • Contribution from broad resonance @1880MeV? ~N(1895)?
  • - Similar result to other analyses
  • - Too far away from real axis: large uncertainties…
  • Ξ·β€²-optical potential from Ξ·β€²π‘ž amplitude with 𝑒ρ approximation
  • Magnitude: O(10) MeV @ρ=ρ0 (typical hadronic scale)
  • Characteristic energy dependence near Ξ·β€²π‘ž threshold

Reproduced by Ξ·(β€²)π‘ž FSI well +some uncertainties…