Toward a study of Λ(1405) via the d(K-, πΣ) reaction
Кілттік сөздер:
kaon,E31, invariant mass spectrumАннотация
There is a long-standing argument if Λ(1405) is a KbarN bound system. Theoretical analyses of Chiral Unitary model, suggests a double-pole structure of Λ(1405): Σπ and KbarN. The theoretical statement about the double pole structure of Λ(1405) shows a new picture of Λ(1405) as a resonant meson-baryon state, which is different from the so-called traditional picture of Λ(1405). In order to solve above-mentioned questions, it is necessary to clarify how Λ(1405) is coupled to KbarN. Therefore, we have conducted an experiment to study Λ(1405) in KbarN scattering (E31). Since Λ (1405) cannot be formed directly from the K-p reaction in free space, we use the d(K-, n)Σπ reactions at a kaon momentum of 1GeV / c, where we expect the incident kaon to knock out a neutron in the deuteron and the recoiled Kbar reacts with the residual nucleon with the formation of Λ(1405).
We have finished a beam time for the second run of E31 in January and February, 2018. The E31 experiment is performed at the K1.8BR beam line in the Hadron Experiment Hall of J-PARC. In the second run, by increasing statistics to several times, we expect to measure Λ(1405) in the Σ+π-/Σ-π+ invariant mass spectra in the d(K−, Σπ)”n”. In particular, we expect to measure angular dependence of widely production of Λ(1405) in the d(K−, Σπ ) reaction.
Библиографиялық сілтемелер
2 C. Amsler et al., Phys. Lett. B667, 1 (2008); doi org/10.1016/j.physletb.2008.07.018. Particle Data Group, http://ccwww.kek.jp/pdg/index.html.
3 R.H. Dalitz and A. Deloff, J. Phys. G17, 289 (1991). doi: org/10.1088/0954-3899/17/3/011
4 R.J. Hemingway, Nucl. Phys. B253, 742-752 (1985). doi: org/10.1016/0550-3213(85)90556-5
5 A.W. Hendry, D.B. Lichtenberg, Prog. of Phys., 33 (3), 139-231 (1985). doi: org/10.1103/PhysRevC.61.055205
6 S. Hirenzaki, Y. Okumura, H. Toki, E. Oset, and A. Ramos, Phys. Rev. C 61, 055205 (2000). doi: org/10.1103/Phys.RevC.61.055205
7 D. Jido et al. Nuclear Phys. A 725 181 (2003). doi:org/10.1016/S0375-9474(03)01598-7.
8 M . Niiyama et al., Phys. Rev. C78, 035202 (2008). doi:org/10.1103/PhysRevC.78.035202
9 O. Braun et al., Nucl. Phys. B129, 1-17 (1977). doi.org/10.1016/0550-3213(77)90015-3
10 M . Iwasaki et al, Phys.Rev.Lett 78, 3067 (1997). doi.org/10.1103/PhysRevLett.78.3067
11 S. Piano, The search for bound kaonic states in nuclei, experimental status and theoretical predictions, INFN sez. Trieste, Hadron 07 - LNF - 11/10/2007
12 Y. Akaishi and T. Yamazaki, Phys. Rev. C65, 044005(2002) doi.org/10.1103/PhysRevC.65.044005; Y. Akaishi and T. Yamazaki, Phys. Rev. C76, 045201 (2007). doi.org/10.1103/PhysRevC.76.045201
13 T. Hyodo, D. Jido, and A. Hosaka, Phys. Rev. Lett. 97, 192002(2006) doi.org/10.1103/PhysRevLett.97.192002; T. Hyodo, D. Jido and A. Hosaka, Phys. Rev. D75, 034002(2007) doi.org/10.1103/PhysRevD.75.034002
14 T. Hyodo and A. Weise, Phys. Rev. C77, 035204 (2008) doi.org/10.1103/PhysRevC.77.035204
15 H. Noumi et al. J-PARC E31 proposal. http://jparc/researcher/Hadron/en/pac_0907/pdf/Noumi.pdf
16 H. Noumi et al. Proposal for the J-PARC 50 GeV Proton Synchrotron. Spectroscopic study of hyperon resonances below KbarN threshold via the (K-n) reaction on Deuteron.
17 D. Jido, E. Oset, and T. Sekihara, The European Physical Journal A 42, P.257, (2009) doi.org/10.1140/epja/i2009-10875-5; D. Jido, private communication, 2009.
18 H. Noumi et al.: J-PARC E31 proposal. http://jparc/researcher/Hadron/en/pac_0907/pdf/Noumi.pdf
19 S. Kawasaki et al., Proc. of the 14th Intern. Conf. on Meson-Nucleon Physics and the Structure of the Nucleon (MENU2016).
20 M . Iwasaki, T. Nagae et al., J-PARC E15 proposal. http://j-parc.jp/NuclPart/pac0606/pdf/p15-Iwasaki.pdf