Production of the eta meson with nucleons and nuclei

Slides:



Advertisements
Similar presentations
Paweł Moskal MESON th International Workshop on Meson Production, Properties and Interaction, Cracow, Poland, 31 May - 5 June 2012 Jagiellonian.
Advertisements

Izabella Zychor EPIPHANY, Krakow, January 6-8, Hyperon production in pp collisions with ANKE at COSY I. Zychor ( IPJ Świerk ) for the ANKE Collaboration.
Mitglied der Helmholtz-Gemeinschaft TSU HEPI Double-polarised np-scattering experiments at ANKE David Mchedlishvili for the ANKE collaboration HEPI, Tbilisi.
1 Eta production Resonances, meson couplings Humberto Garcilazo, IPN Mexico Dan-Olof Riska, Helsinki … exotic hadronic matter?
Paweł Moskal HADRONS IN NUCLEAR MEDIUM II KEK Tokai Campus (JPARC), Japan, October 2014 Jagiellonian University, Cracow, Poland Interaction of pseudoscalar.
Near threshold production of pseudoscalar mesons at the COSY-11 facility Paweł Moskal on behalf of the COSY-11 collaboration NSTAR 2007, Bonn
Kˉ- 4 He, Kˉ- 3 He interactions at low energies Vera Grishina (INR RAS, Moscow, Russia) University of Bonn, Germany August 31 – September 5, 2009.
Analyzing Powers of the Deuteron-Proton Breakup in a Wide Phase Space Region Elżbieta Stephan Institute of Physics University of Silesia Katowice, Poland.
T.C. Jude D.I. Glazier, D.P. Watts The University of Edinburgh Strangeness Photoproduction At Threshold Energies.
Hartmut Machner, MENU04 Beijing 1 Physics at COSY - up to 3.6 GeV/c - e and stochastic cooling, - stochastic extraction (10 s - min) - luminosity achieved:
Paweł Moskal Hadrons and Hadron Interaction in QCD 2015 Kyoto, YITP, 1-6 March 2015 Jagiellonian University, Cracow, Poland Interaction of η and η ́ meson.
1 Formation spectra of  -mesic nuclei by (  +,p) reaction at J-PARC and chiral symmetry for baryons Hideko Nagahiro (RCNP) Collaborators : Daisuke Jido.
On nuclear states of ƞ ( and K - ) S. Wycech NCBJ Warsaw 1) Introduction 2) Non-mesic decay modes.
Paweł Moskal EFB22 The 22nd European Conference on Few-Body Problems in Physics, Cracow, Poland, 9-13 September 2013 Jagiellonian University, Cracow, Poland.
Breakup reaction for polarimetry of tensor polarized deuteron beams 1 A.P. Kobushkin Bogolyubov Institute for Theoretical Physics Metrologicheskaya str.
Mitglied der Helmholtz-Gemeinschaft TSU TBILISI STATE UNIVERSITY The pn-system Study at Internal ANKE Experiment HEPI, Tbilisi State University IKP, Forschungszentrum.
Search for New Physics via η Rare Decay Liping Gan University of North Carolina Wilmington Wilmington, NC, USA.
The Final State Interaction in the pp  + (np) and pp  + (Λp) Reactions R. Siudak Institut für Strahlen- und Kernphysik der Universität Bonn, Bonn,
Generalized Dalitz Plot analysis of the near threshold pp → ppK + K - reaction in view of the K + K - interaction Excited QCD, Stara Lesna, 4th February.
Improved Measurement of d/u Asymmetry in the Nucleon Sea
Mitglied der Helmholtz-Gemeinschaft Physics at COSY-Jülich December 2010 | Hans Ströher (Forschungszentrum Jülich, Univ. Cologne) Baryons´10, Osaka (Japan),
NPD-2009 Conference, ITEP, Moscow, November , Spin structure of the “forward” charge exchange reaction n + p  p + n and the deuteron.
NSTAR2011, Jefferson Lab, USA May 17-20, 2011 Mitglied der Helmholtz-Gemeinschaft Tamer Tolba for the WASA-at-COSY collaboration Institut für Kernphysik.
Study of e+e- annihilation at low energies Vladimir Druzhinin Budker Institute of Nuclear Physics (Novosibirsk, Russia) SND - BaBar Lepton-Photon, August,
The PAX Project and HEPI TSU Contribution 06 August, GGSWBS’12, Tbilisi. Mirian Tabidze High Energy Physic Institute of TSU.
1 Recent Results on J/  Decays Shuangshi FANG Representing BES Collaboration Institute of High Energy Physics, CAS International Conference on QCD and.
H.Nagahiro, S.Hirenzaki, Phys.Rev.Lett.94 (2005) H.Nagahiro, M.Takizawa, S.Hirenzaki, Phys.Rev.C74 (2006) D. Jido, H. Nagahiro, S. Hirenzaki,
Search for a nuclear kaon bound state K - pp at the J-PARC K1.8 beam line. Dep. of physics, Kyoto University / JAEA Y. Ichikawa for E27 Collaboration Korea-Japan.
HADRON 2009, FloridaAnar Rustamov, GSI Darmstadt, Germany 1 Inclusive meson production at 3.5 GeV pp collisions with the HADES spectrometer Anar Rustamov.
Search for a new light boson in  decays J.Stepaniak, M.Berłowski, NCBJ Warsaw For WASA-at-COSY Collaboration Meson2014,Krakow
D. Bettoni - The Panda experiment 1 Charmonium Spectroscopy The charmonium system has often been called the positronium of QCD. Non relativistic potential.
Statistical Significance & Its Systematic Uncertainties
The Strong Force: NN Interaction
Satoshi Nakamura (Osaka University)
Extracting h-neutron interaction from g d  h n p data
Mean free path and transport parameters from Brueckner-Hartree-Fock
Study of Kaon-pion interaction
National Centre for Nuclear Research
The study of pentaquark states in the unitary chiral approach
Exclusive w/h production in pp collisions at Ekin=3.5 GeV with HADES
Baryonium a common ground for atomic and high energy physics
Possible Ambiguities of Neutrino-Nucleus
Observation of a “cusp” in the decay K±  p±pp
Structure and dynamics from the time-dependent Hartree-Fock model
η-mesic nucleus by d + d reaction ー how to deduce η-Nucleus int. ー
Workshop on Precision Physics and Fundamental Constants
Poszukiwanie barionium
E. Wang, J. J. Xie, E. Oset Zhengzhou University
Luciano Pappalardo for the collaboration
G. Arnison et al., UA1 Collaboration
Precision Measurement of η Radiative Decay Width via Primakoff Effect
Study of New Hadron Spectroscopy at BESIII
In search of K+K- molecule
Search for New Physics via η Rare Decay
Marcin Zieliński Paweł Moskal Andrzej Kupść
Measurements of some J/ and c decays at BES
Dibaryon production and structure
STAR Spin alignment of vector mesons (K*0, φ) in Au+Au and p+p collisions at RHIC Jin Hui Chen Shanghai Institute of Applied Physics and UCLA For the STAR.
N*ews from COSY May 2011 | Hans Ströher (Forschungszentrum Jülich, Germany)
Search for f-N Bound State in Jefferson Lab Hall-B
Deeply Bound Mesonic States -Case of Kaon-
On a Search for -Mesic Nuclei at MAMI-C
how is the mass of the nucleon generated?
Study of the 3He-η System in d-p Collisions
N* Program at COSY April 19, 2009 | Hans Ströher (FZ-Jülich)
The np -> d p0 reaction measured with g11 data
Proposal for an Experiment: Photoproduction of Neutral Kaons on Deuterium Spokespersons: D. M. Manley (Kent State University) W. J. Briscoe (The George.
for the A1 collaboration
Search for X - - Pentaquark in COMPASS
f- meson production in pN collisions close to threshold
Presentation transcript:

Production of the eta meson with nucleons and nuclei Paweł Moskal Jagiellonian University, Cracow,Poland Abstract: We report on the status of the search for the eta-mesic nuclei. New results on the analyzing power for the pp->ppeta reaction close to the eta meson production threshold will be presented” I am truly glad to take part in the school and I regret.... Since I am the first time (shame on me) .... I have prepared a presentation on the Kindergarten level.... Maria left me kindly a choise of the subjcet.. So I guess, you may easly imagine all the agonies of having to make a choice which I experienced last week. Here I have to mention that I will explain the meaning of WASA and COSY … (WASA is the detector… and COSY is the proton Cooler Synchrotron) - Mesons in Nuclei 2016 Yukawa Institute for Theoretical Physics, Kyoto University, 31 August 2016 1 1

Production and interaction of the eta meson with nucleons and nuclei mesic-nuclei ppη production Kindergarten .... ; please be awake until the third point .... This is not anymore as fluctuations or efficiency artefacts .... contributing to the study of the muon anomalous magnetic moment Jakos to poskladac do kupy … dlaczego eta SM etc… Polaczyc z nastepna strona i nawiazac podobnie as two years ago I will repeat since …than to Falsify the theory !!! With Wasa at COSY we study both production and decays of the eta-meson but Today I will concentrate of decays which is also a primordial aim of the experiment In general we search for the phenomena which cannot be describe by the Standard Model…

η meson bound with nucleus via THE ETA-MESIC NUCLEUS η meson bound with nucleus via STRONG INTERACTION + + + N* π‾ + η N* + COSY, J-PARC, MAMI, GSI, LPI/JINR Talk by Wojciech Krzemień at this conference … G. A, Sokol et al., arXiv:nucl-ex/0106005

possible existence of bound states Attractive interaction between η and N (R. Bhalerao and L. C. Liu, Phys. Lett. B54 (1985) 685 )‏ possible existence of bound states of the η meson with nuclei for A>10 (Q. Haider and L. C. Liu, Phys. Lett. B172 (1986) 257 )‏ (C.Garcia-Recio, T. Inoue, J.Nieves, E. Oset, Phys. Lett. B550 (2002) 47).

+  - 3He η COSY dp 3He γ 3He  3He MAMI T. Mersmann et al., Phys. Rev. Lett. 98, 242301 (2007) SO its connected to the eta-3He system !!! Is it production or interaction in the final state??? It has rather something to do with hel-eta because… ANKE: T. Mersmann et al., Phys. Rev. Lett. 98 242301 (2007) MAMI: M. Pfeiffer et al., Phys. Rev. Lett. 92 252001 (2004) F. Pheron et al., Phys. Lett. B709 21 (2012) COSY-11: J. Smyrski et al., Phys. Lett B 649 258-262 (2007)

COoler SYnchrotron COSY polarised and unpolarised proton and deuteron beams stochastic and electron cooling momentum range: 600 – 3700 MeV/c meson production up to (1020)‏ spolaryzowana lub niespolaryzowana wiązka protonów i deuteronów chłodzenie stochasyczne i elektronowe zakres pędu: 600 – 3700 MeV/c produkcja mezonów do (1020) włącznie COoler SYnchrotron COSY 6 6

d+d → (4He-η)bound→ 3He + p + π- WASA-at-COSY d+d → (4He-η)bound→ 3He + p + π- d+d → 3He + p + π- → Tu wpsomniec o Pelletach … ( a może ktos ma szkic albo zdjęcie ..) TU PRZYDAŁOBY SIĘ WIDMO POKAZUJACE IDENTYFIKACJE … Magdalena ?? Polaryzacj at Q=15 and at Q=72…

WASA-at-COSY: Phys. Rev. C87(2013) 035204 d+d → (4He-η)bound→ 3He + p + π- d+d → 3He + p + π- SIMULATIONS EXPERIMENT Zamienic rysunek na nowy Magdy... Upper limit of about 25 nb WASA-at-COSY: Phys. Rev. C87(2013) 035204

 - 4He ~ 6 nb -- Present preliminary experimental upper limit . ~ 4 nb -- Theoretical estimation . S. Wycech, W. Krzemien , Acta. Phys. Pol. B45 (2014) 745 .  - 3He ~270 nb -- Present experimental upper limit pppπ- COSY-11: Acta Phys. Pol B41 (2010) 21 ~80 nb -- Theoretical estimation . C. Wilkin, Acta. Phys. Pol. B45 (2014) 603 ~ 10nb -- expected from New WASA-at-COSY data collected in May 2014

 - 4He ~ 6 nb -- Present preliminary experimental upper limit . ~ 4 nb -- Theoretical estimation . S. Wycech, W. Krzemien , Acta. Phys. Pol. B45 (2014) 745 .  - 3He ~270 nb -- Present experimental upper limit pppπ- COSY-11: Acta Phys. Pol B41 (2010) 21 ~80 nb -- Theoretical estimation . C. Wilkin, Acta. Phys. Pol. B45 (2014) 603 ~ 10nb -- expected from New WASA-at-COSY data collected in 2014

J.-J. Xie, W.-H. Liang, E.Oset et al., (priv. com. 2016) Chiral unitary approach Generates the 3He-eta amplitude from the eta-3He potential fitted to the data. With this optical potential solve the BSE for the η 3He system and find an η bound state around 0.3 MeV and a width around 3 MeV, Bethe-Salpeter equation (BSE),

p+d → (3He-η)bound→ p + p + p+ π- p+d → (3He-η)bound → d + p + π0 via N* p+d → (3He-η)bound→ p + p + p+ π- p+d → (3He-η)bound → d + p + π0 p+d → (3He-η)bound → p + p + n + π0 p+d → (3He-η)bound → d + n + π+ decay while orbiting p+d → (3He-η)bound → 3He 6γ p+d → (3He-η)bound → 3He γγ Based on C. Wilkin, Acta Phys. Pol. B45 (2014)

Production and interaction of the eta meson with nucleons and nuclei mesic-nuclei ppη production Kindergarten .... ; please be awake until the third point .... This is not anymore as fluctuations or efficiency artefacts .... contributing to the study of the muon anomalous magnetic moment Jakos to poskladac do kupy … dlaczego eta SM etc… Polaczyc z nastepna strona i nawiazac podobnie as two years ago I will repeat since …than to Falsify the theory !!! With Wasa at COSY we study both production and decays of the eta-meson but Today I will concentrate of decays which is also a primordial aim of the experiment In general we search for the phenomena which cannot be describe by the Standard Model…

in the centre of mass system threshold as a spin filter in the laboratory P 3 GeV/c h P before reaction: after reaction: in the centre of mass system Pauli principle and small energy => Ss DOPISAC O POCHODNEJ NA dm/dP …!!!  mass resolution etc… This was the most decisive factor in minimizing uncertainties of the missing-mass determination, since at threshold the partial derivative of the miss- ing mass with respect to the outgoing proton momentum tends to zero. In addition, close to threshold the signal- to-background ratio increases due to the more rapid reduction of the phase space for multimeson production than for the η′ !!! . etc Parity of eta = -1 … => L=1…., Experiment: So in the laboratory they fligh in small cone….small experiments … full 4pi Threshold: With small relative velocities … large effect expected from interaction…. P h 1 GeV/c P 1 GeV/c L = 1, S = 1 L = 0, l=0 3P01S0s  Reaction parameter b  0.2 fm

A. Deloff, nucl-th/0309059 Ss, Sp, Sd, Ps, Pp Ss, Sd, Ps, Pp

experimental challenge ! The challange is that the cross sections grows rapidly at threshold (phase spase opens…) by many orders of magnitudes at few MeV (few tens of MeV)…. Since many of you are intersted in eta-prime I will emphasise some aspects of eta-prime ....

COoler SYnchrotron COSY polarised and unpolarised proton and deuteron beams stochastic and electron cooling momentum range: 600 – 3700 MeV/c meson production up to (1020)‏ spolaryzowana lub niespolaryzowana wiązka protonów i deuteronów chłodzenie stochasyczne i elektronowe zakres pędu: 600 – 3700 MeV/c produkcja mezonów do (1020) włącznie COoler SYnchrotron COSY 23 23

production dynamics e.g. meson η σ = dVps |M|2 What would the first experimental physicists tell us? |M|2 ~ |M0|2 |MFSI|2 Salviati. But if, of many computations, not even two came out in agreement, what would you think of that? Simplicio. If that is how the matters stand, it is truly a serious defect GALILEO GALILEI ”Dialogue concerning the two chief world systems” dynamics → |M0|2 What would the best student of the Jagellonian University tell us? He is encouraging us to continue: For what is determinate cannot have innumerable explanations NICOLAUS COPERNICUS ”Minor Works III, Letter against Wagner” P P h 1 GeV/c P P 1 GeV/c P ONE NUMBER and MANY GRAPHS

dynamics → |M0|2 LARGE → RESONANSE CELSIUS COSY SATURNE

more coupiously produced X X X STRONG ISOSPIN DEPENDENCE Eta meson is by factor of 12 more coupiously produced when the total isospin of nucleons is equal to 0 than when it is equal to 1 Strong evidence of isovector meson exchange in production mechanism CELSIUS COSY SATURNE

X X X X p r by the very first physicists This was PREDICTED already about 2500 years ago by the very first physicists Thus, it is suggested that among created beings there must be some basic agent which will move things and bring them together ARISTOTLE “Metaphysics” X X X X K. Nakayama et al., Phys. Rev. C 65 (2002) 045210 pseudoscalar G. F ̈aldt and C. Wilkin, Phys. Scripta 64 (2001) 427 vector meson p r ALBO TO TU WSPOMNIEC A WIECEJ PRZY OKAZJI interakcji… PERSPEKTYWY / WASA / POKAZAC WIDMA POLARYZACJI… !...dla XX %...WYKLAD MH z MAIUS… ORAZ O FOTOPRODUKCJI This will be improved by THE WASA-at-COSY collaboartion, I will come to this in few minutes… COSY-11: Phys. Rev. Lett. 98 (2007) 122003

Thus, it is suggested that among created beings This was PREDICTED already about 2500 years ago by the very first physicists Thus, it is suggested that among created beings there must be some basic agent which will move things and bring them together ARISTOTLE “Metaphysics” X X X X r ALBO TO TU WSPOMNIEC A WIECEJ PRZY OKAZJI interakcji… PERSPEKTYWY / WASA / POKAZAC WIDMA POLARYZACJI… !...dla XX %...WYKLAD MH z MAIUS… ORAZ O FOTOPRODUKCJI This will be improved by THE WASA-at-COSY collaboartion, I will come to this in few minutes… p K. Nakayama et al., Phys. Rev. C 65 (2002) 045210 pseudoscalar G. F ̈aldt and C. Wilkin, Phys. Scripta 64 (2001) 427 vector meson COSY-11: Phys. Rev. Lett. 98 (2007) 122003

WASA detector γ P P γ η UJ Krakow & IKP1 Juelich 6

WASA-at-COSY p p p p M 109  and 1011 π0 on discs p p  p p  106  mesons on discs ; Polarization of about 70% more than factor of 100 larger statistics I. Ozerianska, P.M., M. Zieliński, Acta Phys. Pol. B 46 (2015) 153 → Tu wpsomniec o Pelletach … ( a może ktos ma szkic albo zdjęcie ..) TU PRZYDAŁOBY SIĘ WIDMO POKAZUJACE IDENTYFIKACJE … Magdalena ?? Polaryzacj at Q=15 and at Q=72… SPIN DOWN SPIN UP

WASA-at-COSY p p p p M 109  and 1011 π0 on discs p p  p p  106  mesons on discs ; Polarization of about 70% more than factor of 100 larger statistics I. Ozerianska, P.M., M. Zieliński, Acta Phys. Pol. B 46 (2015) 153 → Tu wpsomniec o Pelletach … ( a może ktos ma szkic albo zdjęcie ..) TU PRZYDAŁOBY SIĘ WIDMO POKAZUJACE IDENTYFIKACJE … Magdalena ?? Polaryzacj at Q=15 and at Q=72…

Przykład Asymmetry dla Q=72 oraz eta->2g Masy brakujace dla 2g (lewy) i 6g(prawy)...

r p

WASA-at-COSY pp->ppη r p

Thus, it is suggested that among created beings This was PREDICTED already about 2500 years ago by the very first physicists Thus, it is suggested that among created beings there must be some basic agent which will move things and bring them together ARISTOTLE “Metaphysics” X X X X X r ALBO TO TU WSPOMNIEC A WIECEJ PRZY OKAZJI interakcji… PERSPEKTYWY / WASA / POKAZAC WIDMA POLARYZACJI… !...dla XX %...WYKLAD MH z MAIUS… ORAZ O FOTOPRODUKCJI This will be improved by THE WASA-at-COSY collaboartion, I will come to this in few minutes… p COSY-11: Phys. Rev. Lett. 98 (2007) 122003

s, p, d … s, p, d … Q =15 MeV Q = 72 X X X PRELIMINARY Na górze zdefiniowac P1 i P2 i do czego są proporcjonalne .... Q =15 MeV Q = 72 s, p, d … s, p, d … X X X

THANK YOU FOR YOUR ATTENTION