JPARC Hadron physics WS 2014 11 30 What

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J-PARC Hadron physics WS 2014. 11. 30 What can we learn about X resonances

J-PARC Hadron physics WS 2014. 11. 30 What can we learn about X resonances at K 1. 8 K. Imai (JAEA)

X resonances in PDG

X resonances in PDG

PDG Table of X

PDG Table of X

X* quark model: Chao, Isgur, Karl PRD 23 (1981) X(1690)JP? X(1530)3/2+ X(1820)3/2 L(1520)3/2 L(1405)1/2

X* quark model: Chao, Isgur, Karl PRD 23 (1981) X(1690)JP? X(1530)3/2+ X(1820)3/2 L(1520)3/2 L(1405)1/2 -

X* spectroscopy at K 1. 8 X*(1530) radiative decay X*(1690) Spin-parity, Branching ratio If

X* spectroscopy at K 1. 8 X*(1530) radiative decay X*(1690) Spin-parity, Branching ratio If ½-, it may be s=-2 analogue of L(1405). SK molecule?

Radiative decay of X(1530) is not known! • Radiative decay were measured for all

Radiative decay of X(1530) is not known! • Radiative decay were measured for all other 10 -> 8 baryons. • Radiative decay is the best probe to study its structure.

X(1690) Why it is interesting? • Just below or above SK threshold S-K 0

X(1690) Why it is interesting? • Just below or above SK threshold S-K 0 1695. 0 Me. V S 0 K- 1686. 3 Me. V S 0 K 0 1690. 2 Me. V S+K- 1683. 1 Me. V • Very small branching to Xp • Narrow width ~10 Me. V candidate of exotic baryon (meson-baryon molecule)

Hyperon spectrometer (Hyp. TPC) for E 42, E 45 at JPARC TPC with GEM

Hyperon spectrometer (Hyp. TPC) for E 42, E 45 at JPARC TPC with GEM in Superconducting Helmholtz magnet of 1. 5 T 2021/12/11 Seoul-meeting 2010/11/30

2021/12/11

2021/12/11

GEM sheet and the pad plane Test of full size TPC is under progress

GEM sheet and the pad plane Test of full size TPC is under progress at JAEA 2021/12/11

Hyp. TPC • Target is inside TPC track of short life hyperons L, S

Hyp. TPC • Target is inside TPC track of short life hyperons L, S , X-, (K 0) • High rate operation beam pass through up to 106 Hz (If GEM at beam path is killed, 107~108 Hz) • Large acceptance almost 4 p • High resolution DM(LL) ~ 1 Me. V 2021/12/11 Seoul-meeting 2010/11/30

X*(1530) X g • K-p -> K+ X-*(1530) ds/d. W ~ 40 mb/sr at

X*(1530) X g • K-p -> K+ X-*(1530) ds/d. W ~ 40 mb/sr at p(K-) = 1. 65 Ge. V/c p(K+) ~ 700 Me. V/c T. Iijima et al. , (E 176) N. P. (1992) • Yield estimation 5 cm liq. H target, 106 K-/5 sec, 0. 1 str. Kurama acceptance, 100 shifts, 4. 6 x 105 X*-(1530) Hyp. TPC acceptance for X- p-L, L pp- 60% Charged branch of L : 64%, branch for radiative decay: 0. 5% 900 (3% error) If you require g position to reduce background 450 (5% error)

Mass spectra 1) X(1530) 2) X(1321) 3) L by S. Hwang • 1) •

Mass spectra 1) X(1530) 2) X(1321) 3) L by S. Hwang • 1) • 2) 2)

Miss mass of p(K-, K+ X) gamma pi 0

Miss mass of p(K-, K+ X) gamma pi 0

HBC data on X(1690) P(K-)=4. 2 Ge. V/c (CERN) cross section for X(1690) ~

HBC data on X(1690) P(K-)=4. 2 Ge. V/c (CERN) cross section for X(1690) ~ 7. 6 mb • C. Dionisi et al. , PL 80 B (1978) 145. • An enhancement at the Sigma K threshold (1680 Me. V) observed in K-p reactions at 4. 2 Ge. V/c. M(S+K-) M(LK-)

S. F. Biagi et al. , Z. Phys. C 34 (1987) 15. X* resonances

S. F. Biagi et al. , Z. Phys. C 34 (1987) 15. X* resonances in X- Be interactions • Width < 8 Me. V CERN 116 Ge. V/c X- beam

M. I. Adomovich et al. , WA 89 EPJ C 5 (1998) 621. First

M. I. Adomovich et al. , WA 89 EPJ C 5 (1998) 621. First observation of X- p+ decay mode of the X 0(1690) hyperon. 345 Ge. V/c S- beam CERN 1400 events ! Width 10+-6 Me. V

K. Abe et al. , Belle PLB 524 (2002) 33. Observation of Cabbibo-suppressed and

K. Abe et al. , Belle PLB 524 (2002) 33. Observation of Cabbibo-suppressed and W exchange Lambda-c baryon decays. Lc X(1690)0 K+ at Belle. Width = 11+- 4 Me. V

Bar. Bar Lc L K 0 K+

Bar. Bar Lc L K 0 K+

spin of X(1690)

spin of X(1690)

B. Aubert et al. , Bar PRD 78 (2008) 34008. Measurement of the spin

B. Aubert et al. , Bar PRD 78 (2008) 34008. Measurement of the spin of the X(1530) resonance. Lc X- p+ K+ at Bar

How can we measure with Hyp. TPC at K 1. 8 • Spin-parity and

How can we measure with Hyp. TPC at K 1. 8 • Spin-parity and branching ratio to LK, SK, Xp, Xg • K-p -> K+ X-* -> LK-, S 0 K-, S-K 0, X-p 0, X 0 p-, X-g, • K-p -> K 0 X 0*, X 0* -> LK 0, S 0 K 0, S+K-, X-p+, • K 0 ->p+p-, X 0 ->Lp 0 Most of decay channels can be measured. (one neutral particle is allowed to reconstruct the decays ) Yield estimation: (5 cm liq. H, 106 K-/spill, 100 shifts) 4 mb 5 x 105 X*(1690) if 1 mb for each channel LK-, S 0 K-, Xp: 0. 6 x 0. 64=0. 38, -> 5 X 104 events S-K 0: 0. 35 x 0. 64 x 0. 6=0. 13 -> 1. 6 x 104 for K 0 X 0* channels, multiply 0. 35 x 0. 6=0. 2

mass spectra 1) X(1690) 2) L 3) X* 1) 3 2

mass spectra 1) X(1690) 2) L 3) X* 1) 3 2

How to determine spin-parity Angular distribution of decay particles !! 3/2 -> ½ +0

How to determine spin-parity Angular distribution of decay particles !! 3/2 -> ½ +0 D-> p +N L=1 -> cosq But it is not so simple. for parity determination of ½ state. interference with background ( p(s)-wave resonance on s(p)-wave background) polarization of daughter hyperon (L, S) if X* is polarized (L(1405) Moriya et al. , )

Summary • The new hyperon spectrometer (Hyp. TPC) is under construction at JAEA in

Summary • The new hyperon spectrometer (Hyp. TPC) is under construction at JAEA in collaboration with Korea and New Mexico U. • Following H search experiment (E 42) and E 45, X* spectroscopy should be carried out as well as X-p scattering experiment at J-PARC. 2021/12/11

Back up

Back up

Cross sections 3. 2+-0. 8 mb 1. 1+-0. 5 2. 3+-0. 3 1. 0+-0.

Cross sections 3. 2+-0. 8 mb 1. 1+-0. 5 2. 3+-0. 3 1. 0+-0. 4 < 1. 0 • Xi-* • • Xi 0* • • Sigma 0 K- (K 0 pi+) Lambda K- (K 0 pi+) Sigma+ K- (K+, pi-) Lambda K 0 (K+, pi-) Xi pi • Total cross section for Xi(1690) 7. 6 mb

WA 89 setup S- 105/spill S-/p- =2. 3 7. 5 Tm 45 MWPC 29

WA 89 setup S- 105/spill S-/p- =2. 3 7. 5 Tm 45 MWPC 29 SSD

E. Briefel et al. , PRD 16 (1977) 2706. Search for Xi* production in

E. Briefel et al. , PRD 16 (1977) 2706. Search for Xi* production in K-p interactions at 2. 87 Ge. V/c. sensitivity: 30 events/microbarn, BNL HB K-p K+ X- p+ X-p+ invariant mass