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Jinhui Chen

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The first hypernucleus was discovered by Danysz and Pniewski in 1952. ... Theory input: the L is lightly bound in the hypertriton, so it's not expected that the ... – PowerPoint PPT presentation

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Title: Jinhui Chen


1
Jinhui Chen Kent State University for the STAR
Collaboration
2
What are hypernuclei?
Hypernuclei of lowest A
Nucleus which contains at least one hyperon in
addition to nucleons.
  • Y-N interaction a good window to
  • understand the baryon potential
  • Binding energy and lifetime are very
    sensitive to Y-N interactions
  • Hypertriton DB13050 KeV r10fm
  • Production rate via coalescence at RHIC
    depends on overlapping wave functions of
    npL in final state
  • Hypertriton and anti-hypertriton ratios
    sensitive to matter and anti-matter profiles
    in heavy-ion collisions
  • Important first step for searching for other
    exotic hypernuclei (double-L)
  • ? ? p ? - (64) ? ? n ? 0 (36)

The first hypernucleus was discovered by Danysz
and Pniewski in 1952. It was formed in a cosmic
ray interaction in a balloon-flown emulsion
plate. M. Danysz and J. Pniewski, Phil.
Mag. 44 (1953) 348
No one has ever observed any anti-hypernucleus
3
from Hypernuclei to Neutron Stars
Nuclei Baryon-Baryon Interaction
Neutron Stars
  • Several possible configurations of Neutron Stars
  • hyperons, strange quark matter
  • Single and double hypernuclei in the laboratory
  • study the strange sector of the baryon-baryon
    interaction
  • provide info on EOS of neutron stars

4
Current status
5
Can we observe hypernuclei at RHIC?
  • Low energy and cosmic ray experiments
  • hypernucleus production via
  • L or K capture by nuclei
  • the direct strangeness exchange reaction
  • hypernuclei observed
  • energetic but delayed decay,
  • measure momentum of the K and p mesons
  • In high energy heavy-ion collisions
  • nucleus production by coalescence, characterized
    by penalty factor.
  • AGS data1 indicated that hypernucleus
    production will be further suppressed.
  • Whats the case at RHIC?

1 AGS-E864, Phys. Rev. C70,024902 (2004)
6
Data-set and track selection
  • 3LH mesonic decay, m2.991 GeV, B.R. 0.25
  • Data-set used, AuAu 200 GeV
  • 67M Run7 MB,
  • 23M Run4 central,
  • 22M Run4 MB,
  • VZ lt 30cm
  • Tracks quality cuts, global track
  • nFitsPts gt 25, nFitsPts/Max gt 0.52
  • nHitsdEdx gt 15
  • Pt gt 0.20, eta lt 1.0
  • Pion n-sigma (-2.0, 2.0)

Secondary vertex finding technique
DCA of v0 to PV lt 1.2 cm DCA of p to PV gt 0.8
cm DCA of p to 3He lt 1.0 cm Decay length gt 2.4 cm
7
3He anti-3He selection
Select pure 3He sample -0.1ltZlt0.3 dca lt1.0cm
p gt2 GeV 3He 2931(MB07)
2008(central04) 871(MB04) 5810 Anti-3He
1105(MB07) 735(centtral04) 328(MB04) 2168
8
signal from the data
  • background shape determined from rotated
    background analysis
  • Signal observed from the data (bin-by-bin
    counting) 177 30
  • Mass 2.990 0.001 GeV Width (fixed)
    0.0025 GeV.

9
signal from the data
  • Signal observed from the data (bin-by-bin
    counting) 6818
  • Mass 2.9910.001 GeV Width (fixed) 0.0025
    GeV

10
Measured lifetime
Combine hypertriton and anti-hypertriton signal
24435
11
Measured signal vs. ct bins
  • Our data
  • Consistency check on L lifetime yields
    t(L)2675 ps PDG 263 ps.

12
Comparison to world data
  • Theory input the L is lightly bound in the
    hypertriton, so its not expected that the
  • hypertriton decay rate should be very much
    different from that of the free L.

1 R. H. Dalitz, Nuclear Interactions of the
Hyperons (Oxford Uni. Press, London, 1965). 2
R.H. Dalitz and G. Rajasekharan, Phys. Letts. 1,
58 (1962). 3 H. Kamada, W. Glockle at al.,
Phys. Rev. C 57, 1595(1998).
13
Measured invariant yield and ratio
In the coalescence picture 0.45 (0.77)3
14
Conclusions
  • has been observed for 1st time
    significance 4s.
  • Consistency check has been done on
    analysis
  • significance is 6s
  • The lifetime is measured to be
    , 2s deviation from
  • lifetime for free Ls.

/ 3He is 0.82 0.16. No extra penalty
factor observed for hypertritons at RHIC.
15
International Hyper-nuclear network
  • PANDA at FAIR
  • 2012
  • Anti-proton beam
  • Double ?-hypernuclei
  • ?-ray spectroscopy
  • SPHERE at JINR
  • Heavy ion beams
  • Single ?-hypernuclei
  • HypHI at GSI/FAIR
  • Heavy ion beams
  • Single ?-hypernuclei at
  • extreme isospins
  • Magnetic moments
  • MAMI C
  • 2007
  • Electro-production
  • Single ?-hypernuclei
  • ?-wavefunction
  • JLab
  • 2000
  • Electro-production
  • Single ?-hypernuclei
  • ?-wavefunction
  • FINUDA at DA?NE
  • ee- collider
  • Stopped-K- reaction
  • Single ?-hypernuclei
  • ?-ray spectroscopy
  • (2012)
  • J-PARC
  • 2009
  • Intense K- beam
  • Single and double ?-hypernuclei
  • ?-ray spectroscopy ?
  • BNL
  • Heavy ion beams
  • Anti-hypernuclei
  • Single ?-hypernuclei
  • Double L-hypernuclei

Basic map from Saito, HYP06
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