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Recent results and future prospects of the KbarNN search
via the (K-,N) reaction at J-PARC F. Sakuma, RIKEN
for the J-PARC E15 collaboration
Results of the E15 1st physics runFuture prospects of E15Summary
Achievements and Perspectives in Low-Energy QCD with Strangeness, ECT*, 2014 10/27-31
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Kaonic NucleiKaonic nucleus is a bound state of nucleus and
anti-kaon (KbarNN, KbarNNN, KbarKbarNN, ...)
2
Y.Akaishi & T.Yamazaki, PLB535, 70(2002).
Density [1/fm
3]
T.Yamazaki, A.Dote, Y.Akiaishi, PLB587, 167 (2004).
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K-pp Bound State
3
A.Gal, NPA914(2013)270
K-pp : the simplest Kbar-nuclear state
All theoretical studies predict existence of the K-pp However, B.E. and G are controversial
Y.Ichikawa, EXA2014
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Experimental Principle of E15A search for the simplest kaonic nucleus, K-pp,
using 3He(in-flight K-,n) reaction
4
• two-nucleon absorption• hyperon decays CAN be discriminated kinematically
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Experimental Setup
5
15m
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E15 1st Stage Physics-Run
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• Production run of ~1% of the approved proposal was successfully performed in 2013.
• All detector systems worked well as designed.
Primary-beam intensity
Secondary-kaon intensity Duration Kaons on target
(w/ tgt selection)
March, 2013(Run#47)
14.5 kW(18 Tppp, 6s) 80 k/spill 30 h 1.1 x 109
May, 2013(Run#49c)
24 kW(30 Tppp, 6s) 140 k/spill 88 h 5.3 x 109
* production target: Au 50% loss, spill length: 2s, spill duty factor: ~45%, K/pi ratio: ~1/2* ~70% of beam kaons hit the fiducial volume of 3He target
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Summary of E15 1st
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3He(K-,n)X M.M.
Formation ChannelSemi-Inclusive 3He(K-,n)X No significant bump structure
in the deeply bound region Excess below the threshold
attributed to 2NA of L*n?
FINUDA/DISTO
Decay ChannelExclusive 3He(K-,Lp)n Hint of the excess around
the threshold Cannot be from 2NA of L*n
(final state = Lpn)
Lp I.M.of 3He(K-,Lp)n
preliminary
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Formation Channel,Semi-Inclusive 3He(K-,n)X
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T.Hashimoto et al., arXiv:1408.5637, submitted to PLB
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Semi-Inclusive Spectrum
Quasi ElasticK- + 3He K- + n + ps + ps
ds/dWq=0deg ~ 6mb/sr
Charge-ExchangeK- + 3He K0 + n + ds
K0 p+ + p-
ds/dWq=0deg ~ 11mb/sr
and
The tail structure is not due to “the detector resolution”
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Background Evaluation
evaluated using empty-target data
1/b distribution for g/n
(Phys. BG)
(Exp. BG)
(Exp. BG)
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Spectrum below the Threshold
FINUDA/DISTO
No significant bump-structure in the deep-binding region Statistically significant excess just below the threshold
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Comparison between E15 and
Other Results
M(K+p+p)
FINUDA@DAFNEPRL94(2005)212303
A(stopped K-, Lp)
DISTO@SATURNEPRL104(2010)132502
p + p (L + p) + K+ @ 2.85GeV
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Comparison between E15 and
Other Results
d(p+, K+) @ 1.7GeV/c
E27@J-PARCEXA2014 conference
M(K+p+p)
• Bump structure in the deep-binding region reported from other experiments was NOT seen in E15
• Excess near the threshold can be seen only in E15
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95%
C.L
.
AssumptionsK-pp Lp decay mode (isotropic decay)K-pp shape = Breit-Wigner
U.L. depends on the decay mode
U.L. of the deeply-Bound K-pp
K-ppLp
CDS tagging eff.
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U.L. of the deeply-Bound K-pp
LEPS@SPring-8PLB728(2014)616
g + d K+ + p- + X @ 1.5-2.4GeV
E15(K-+3He): (UL) 0.5-5% of QFFINUDA(stopped K-): ~0.1% of stopped K-
DISTO(p+p): larger than L* @ 2.85GeV LEPS(g+d) (UL) 1.5-26% of gNK+p-Y
Upper limits (CS) can be directly compared
with QF yield.
95%
C.L
.
K-ppLp
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Spectrum below the Threshold
No significant bump-structure in the deep-binding region Statistically significant excess just below the threshold
?
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•Detector acceptance and all known K-N interactions are taken in to account:– Cross-section [CERN-HERA-83-02]– Fermi-motion– Angular distribution
• Simple assumptions:– stot = 2*sK-p + sK-n (~150mb)
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Excess = Elementary Processes?
SIM
The tail structure is NOT reproduced by well known processeswould be attributed to the imaginary part of the attractive KbarN Multi-NA? K-pp?
S decay contributions
DATA(BG subtracted)
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Excess = pSN, pSNN, etc?
Each process is simulated with unreasonably large CS of 100mb contributions in the binding region are negligible
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BW shape withPDG values
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Excess = L*N, etc?
• LN/SN branches are negligibly small• L(1405)n branch seems to reproduce the excess
– need rather large CS of ~5mb/sr– L(1405) shape is controversial
careful quantitative analysis is required
• For further study, exclusive measurement of pSN is important.
CS of each process :20mb/sr @ 0 degrees
(consistent with KEK-PS E548)
“semi-inclusive measurement would distort the spectrum” by Magas et al., PRC81(2010)024609.
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Excess = Loosely-Bound K-pp?
CDS tagging eff.
K-pp?
• The excess is assumed to be fully attributed to the bound K-pp state
• ds/dW(qlab=0o) of the excess is ~ mb/sr
S decay contributions
DATA(BG subtracted)
(Excess/QF < ~10%)
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Comparison between E15 and Calc.
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Koite
, Har
ada,
PRC8
0(20
09)0
5520
8
integrated CS:~mb/sr Yamagata-Sekihara, et al.,
PRC80(2009)045204
integrated CS:~0.1 mb/sr
• CS is roughly consistent with KH• Loosely-bound K-pp state ???
pSN measurement is an important key
DATA(BG subtracted)
DATA(BG subtracted)
semi-inclusive
semi-inclusive
inclusiveinclusive
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Decay Channel,Exclusive 3He(K-,Lp)n
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Exclusive 3He(K-,Lp)n events
• K-3HeL(S0)pn events can be identified exclusively– # of L(S0)pn events: ~190
• S0pn contamination: ~20% 23
n
1GeV/cK- beam
p
p-
p
missing n
L
CDSpreliminary
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Dalitz plot
24
Observed events seem to be scattered widely in the
phase-space of K-+3He->L+p+n
3NA: e.g. K-3HeLpn
preliminary
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K-pp form.: K-3He(K-pp)n,
K-ppLp
2NA: e.g. K-3HeLpns
Dalitz plot
25
2NA+2step: e.g. K-3HeS0pns,
S0nsLn
2NA+2step: e.g. K-3HeS0nps,
S0psLp
2NA+2step: e.g. K-3HeLpns,
pnspn
preliminary
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K-induced vs p-induced
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[1] D. Gotta, et al., PRC51. 496 (1995)[2] P. Weber et al., NPA501 765 (1989)[3] G. Backenstoss et al., PRL55. 2782 (1985)
• p- stopped [1]– 2nucleon absorption &FSI (50%/ p stopped) are clearly seen
– 3nucleon absorption <3% / p stopped
• p- in-flight [2],[3]– 2nucleon absorption 0.85 ± 0.17mb (266 MeV/c)– 3nucleon absorption 3.7 ± 0.6 mb(220 MeV/c)– 3NA/2NA ~ 4
in-flight K stopped p
Data suggests that3NA reactions are dominant?
preliminary
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Lp Invariant Mass
27
SIM
2NAK-pp
B.E = 50MeVG = 50MeV
3NA
Excess around the threshold?
Further study is ongoing, such as contribution from
2NA+2step.S0p Lp
preliminary FS = L (S0 ) pn cannot be from
2NA of L*n
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~190 events
• total CS : ~200 mb– when phase-space distributions are assumed
• Excess around the threshold?
IM(Lp)
(~ 0.1% of total cross section of K-3He)
IM(Ln)
Comparison with Phase-Space
preliminary
preliminary
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• data cannot be reproduced by the phase-space?
Comparison with Phase-Space
29
cos(Lp) cos(Ln)
pLpp pn
preliminary
preliminary
preliminary
preliminary
preliminary
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Formation + Decay Channel,Kinematically Complete 3He(K-,Lpn)
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Kinematically-complete measurement of 3He(K-, Lpn)
• Minimum momentum transfer of the 3He(K-,n) reaction would enhance the S=-1 di-baryon production
• More beam time is required 31
only~15 eventspreliminary
preliminary
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Future Prospects of E15
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E15 2nd stage (approved)
E152nd: 50x109 kaons on target
33
x10
The goal of the E152nd
1. derive pSN decay information in 3He(K-,n)X reaction
2. confirm the spectral shape of the Lp invariant-mass by the exclusive measurement of 3He(K-,Lp)n
3. explore the neutron spectrum at qlab=0O with the kinematically complete measurement of 3He(K-,Lpn)
in 2015
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Summary of E15 1st
34
3He(K-,n)X M.M.
Formation ChannelSemi-Inclusive 3He(K-,n)X No significant bump structure
in the deeply bound region Excess below the threshold
attributed to 2NA of L*n?
FINUDA/DISTO
Decay ChannelExclusive 3He(K-,Lp)n Hint of the excess around
the threshold Cannot be from 2NA of L*n
(final state = Lpn)
Lp I.M.of 3He(K-,Lp)n
preliminary
• Interesting hints of S=-1 system have been obtained in E15 1st.
• E15 2nd will be performed in 2015.
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The J-PARC E15 Collaboration
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