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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)


  1. Study of Ξ· β€² 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))

  2. Introduction - O rigin of the η’ mass Anomaly-induced coupling ← U A (1) anomaly and chiral symmetry breaking (3flavor) Witten(1979),’t Hooft (1986),… Pisarski-Wilzek(1984), Kunihiro-Hatsuda(1988), Cohen (1996), Lee- Hatsuda (1996),… οƒŸ Chiral restoration in nuclear medium (reduction of order parameter of chiral symmetry breaking) In- medium η’ as a probe of chiral symmetry in nuclear medium - η’ mass in finite density Costa-Ruivo-Kalinovsky(2003), Kwon-Lee-Morita-Wolf(2012), Fejos-Hosaka (2017)… - η’ -nucleus system Tsushima(2000),Nagahiro-Hirenzaki(2005),Nagahiro-Takizawa-Hirenzaki (2006),Jido-Nagahiro-Hirenzaki (2012), Tanaka et al . (2016),Metag-Naova-Paryev (2017),… η’ -nucleon interaction = basic information Borasoy (2000), Bass-Thomas (2006), Oset-Ramos (2011), S.S.-Jido(2013), Moskal(2000), Czerwinski et al .(2014) ,… s-wave η’p scattering length from pp οƒ  ppη’  Study of η’ -few nucleon system: Sekihara-Fujioka-Ishikawa(2018) for η’d

  3. Recent data on Ξ·/Ξ·β€² photoproduction Ξ· β€² π‘ž threshold effect A2 Collaboration at MAMI, PRL118(2017)212001

  4. - Ξ·β€² photoproduction from proton -- Comparison with phase space Data: A2 Collaboration at MAMI, PRL118(2017)212001 Phase space Near-threshold enhancement β–  N(1895) contribution: PRL118(2017)212001[A2 Collaboration], PLB785(2018)626[Anisovich et al.]

  5. from latest PDG [PRD98,030001(2018)] Broad resonance @ Ξ· β€² π‘ž threshold(=1896MeV) - Ο€N οƒ  Ο€N: PRC89(2014)045205[ Svarc et al .] - Ξ³p οƒ  K *Ξ›: PLB771(2017)142[CLAS Collab.] - Ξ³p and Ο€ p οƒ  KΞ› : EPJA53(2017)242[Anisovivh et al .] - Multichannel: PRL119(2017)062004[Anisovich et al .]

  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€² π‘ž scattering length Anisovich et al ., arxiv:1803.06814

  7. Threshold cusp οƒ˜ A simple t matrix with channel coupling: (ΞΊ: real and positive)

  8. Information on 𝜽 β€² 𝒒 amplitude ( 𝑁𝐢 can be Ξ· β€² π‘ž, Ξ·π‘ž, Ο€π‘ž , 𝐿Λ , 𝐿Σ , Ο‰π‘ž ,…) Extraction of the Ξ· β€² π‘ž amplitude β–‘ Ξ· β€² π‘ž scattering length β–‘ Ξ· β€² -optical potential from Ξ·/Ξ·β€² -photoproduction data -- Focus on Ξ· β€² π‘ž -threshold behavior  Focus on the Ξ· β€² π‘ž -threshold region (~100MeV around Ξ· β€² π‘ž threshold)

  9. Setup 〇 Final-State Interaction = + +… ~1.7GeV -- for channel coupling effect ( Ο€π‘ž , 𝐿Λ , 𝐿Σ , Ο‰π‘ž ) β€» Resonance is not assumed in Ξ· ( ’ ) p amplitude

  10. : polynomial of 𝑑 -- with 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 (Ξ” <70MeV) Fit parameter -- Interaction kernel of Ξ· (β€²) π‘ž -- Ξ· (β€²) π‘ž production amplitude from photon

  11. Constraint on scattering amplitude 〇 Optical theorem can happen Restriction a large number

  12. A simple test: fit Ξ³π‘ž β†’ Ξ· β€² π‘ž data with Ξ· β€² π‘ž FSI () with οƒŸ phase space οƒŸ fit Ξ· β€² π‘ž -threshold Data: A2MAMI, PRL118(2017)212001 0 Flip sign below Ξ· β€² π‘ž threshold

  13. A simple test: fit Ξ³π‘ž β†’ Ξ· β€² π‘ž data with Ξ· β€² π‘ž FSI with 𝑁𝐢 = Ξ· β€² π‘ž would be responsible for the enhancement

  14. Results of Ξ³π‘ž β†’ Ξ· (β€²) π‘ž fitting Ξ³π‘ž β†’ Ξ·π‘ž data: A2MAMI, PRL118(2017)212001 and CLAS, PRC80(2009)045213 Ξ³π‘ž β†’ Ξ· β€² π‘ž data : A2MAMI, PRL118(2017)212001 Fit Ξ” varied (n max =1) Ξ”=50 -70MeV

  15. Ξ· β€² π‘ž scattering amplitude Ξ” varied (n max =1) 0 (Ξ”=60MeV) Ξ· β€² π‘ž -threshold Flip sign below Ξ· β€² π‘ž threshold π‘žπ‘ž β†’ π‘žπ‘žΞ·β€² [Czerwinski et al ., PRL113, 062004(2014)] -- pole~(1877- 63i)MeV(Ξ”=60MeV) 〇 Too far away from real axis… β€» Error of parameters: ~10% Anisovich et al ., arxiv:1803.06814

  16. Results of Ξ³π‘ž β†’ Ξ· (β€²) π‘ž fitting : polynomial of 𝑑 -- Fit (Ξ”=60MeV fixed) n max varied

  17. Ξ· β€² π‘ž scattering amplitude n max varied (Ξ”=60MeV) 0 Ξ· β€² π‘ž -threshold

  18. Ξ” varied (Ξ”=30MeV)

  19. Ξ· β€² -optical potential @ ρ = ρ 0 Ξ” varied (n max =1)

  20. Ξ· β€² -optical potential @ ρ = ρ 0 n max varied (Ξ”=60MeV)

  21. Ξ” varied

  22. Summary β€’ Analysis of Ξ·/Ξ· β€² photoproduction data with Ξ· (β€²) π‘ž Final-State Interaction β€’ Threshold effect Reproduced β€’ Near-threshold enhancement in Ξ³π‘ž β†’ Ξ· β€² π‘ž by Ξ· (β€²) π‘ž FSI well β€’ Cusp of Ξ³π‘ž β†’ Ξ·π‘ž cross section @ Ξ· β€² π‘ž thr. β€’ For s-wave Ξ· β€² π‘ž scattering length, +some uncertainties… β€’ Contribution from broad resonance @1880MeV? ~N(1895)? -- Similar result to other analyses -- Too far away from real axis: large uncertainties… β€’ Ξ· β€² -optical potential from Ξ· β€² π‘ž amplitude with 𝑒ρ approximation β€’ Magnitude: O(10) MeV @ρ=ρ 0 (typical hadronic scale) β€’ Characteristic energy dependence near Ξ· β€² π‘ž threshold

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