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The AMADEUS project – precision studies of the low-
energy antikaon nucleon interaction
Johann Zmeskal, SMI – Vienna, Austria for the AMADEUS collaboration
International Workshop on Hadronic Atoms and Kaonic Nuclei ECT*, Trento 12 – 16 October 2009
AMADEUS at DANE
Antikaon
Matter
At
DANE:
Experiments with
Unraveling
Spectroscopy
International Workshop on Hadronic Atoms and Kaonic Nuclei
AMADEUS collaboration
International Workshop on Hadronic Atoms and Kaonic Nuclei
110 scientists from 34 Institutes of 14 Countries
Letter of Indent
Study of deeply bound kaonic nuclear states
at DANE2
March 2006
Introduction
Investigations of antikaon-mediated bound nuclear systems were done, are ongoing or planned at several facilities - KEK, LNF, GSI, J-PARC, CERN-AD
Next-generation experiments should be exclusive, i.e. require the measurement of formation and decay
AMADEUS @ DAΦNE2 aims to do that with - stopped K− in low-density gas targets - unique features available at DAΦNE2 - measurement of all decay particles, charged and neutral, using the KLOE detector
International Workshop on Hadronic Atoms and Kaonic Nuclei
DAFN at LNF
International Workshop on Hadronic Atoms and Kaonic Nuclei
AMADEUS’s main aim is to perform a full acceptance, high precision measurement of antikaon-mediated bound nuclear systems – studying the formation as well as the decay process, by implementing the KLOE detector with an inner AMADEUS dedicated setup, containing a cryogenic target and a trigger system (and an inner tracker in a second phase).
First actions:Results of the KLOE data analysis were presented by O. VazquezTest measurements of the AMADEUS trigger system were presented by A. Scordo
The goal of AMADEUS
International Workshop on Hadronic Atoms and Kaonic Nuclei
The experimental program - 1
study of the (most) fundamental antikaon-mediated bound nuclear systems, the kaonic dibaryon states:
ppK- and (pnK-)
produced in a 3He gas target, by their formation and decay processes
and as next step, the kaonic tri-baryon states:
ppnK- and (pnnK-)
produced in a 4He gas target, by their formation and decay processes
International Workshop on Hadronic Atoms and Kaonic Nuclei
The experimental program - 2
Low-energy charged kaon cross section on p, d, He-3 and He-4, for K- momentum lower than 100 MeV/c
The K- nuclear interactions in Helium (poorly known – based on one paper from 1970 …)
Properties of L and charged S´s
Resonance states as L(1405) or the S(1385) in addition their behaviour in a nuclear
mediumcan be studied
International Workshop on Hadronic Atoms and Kaonic Nuclei
Production methods of antikaon-mediated bound nuclear cluster
stopped K- reactions on light nuclei
in-flight K- reactions
protons on proton (or light nuclei)
heavy ion collisions
strangeness production in antiproton annihilation
International Workshop on Hadronic Atoms and Kaonic Nuclei
tri-baryon systems with S = -1
formation process:
K- + 4He ppnK- + n
possible decay channels:
ppnK- + d
+ p + n - + p +
p 0 + d 0 + p + n
L p + - n + 0
S- n + - S0 +
International Workshop on Hadronic Atoms and Kaonic Nuclei
Hyperon production
K-N Y
International Workshop on Hadronic Atoms and Kaonic Nuclei
Non-mesonic absorption
K-NN YN
International Workshop on Hadronic Atoms and Kaonic Nuclei
13
Schematicside view ofthe KLOE detectorwith AMADEUScomponents added:
e+ e-
K-
K+
Amadeus @ KLOE
International Workshop on Hadronic Atoms and Kaonic Nuclei
KLOE CDC
= 0.289 ± 0.003
Lambda invariant mass,
using existing KLOE data (O. Vazquez
Doce)Minv= 1115,723 ±0. 003stat (MeV/c2)
PDG: MΛ= 1115,683 ±0.006stat±0.006syst (MeV/c2)
systematic dependents on momentum calibration, has to be evaluated using 2-body decays: K±→μ±ν and K±→π±π0
International Workshop on Hadronic Atoms and Kaonic Nuclei
KLOE calorimeter
International Workshop on Hadronic Atoms and Kaonic Nuclei
Reconstructed Ks mass
Photon energy resolution (E)/E = 5.7%xE(GeV)-1/2
time resolution t/t = 54 [ps]xE(GeV)-1/2
Ks oo, with o
International Workshop on Hadronic Atoms and Kaonic Nuclei
Neutron detection efficiency
Threshold at 1 MeVThreshold at 3 MeV
MC simulation, confirmed with measurements at TSL (Uppsala
International Workshop on Hadronic Atoms and Kaonic Nuclei
AMADEUS @ KLOE
International Workshop on Hadronic Atoms and Kaonic Nuclei
AMADEUS @ KLOE
International Workshop on Hadronic Atoms and Kaonic Nuclei
half-toroidal cryogenic target cell
1st inner-layer ofscintillating fibrefiber size: 1x1mm2
2nd inner-layer ofscintillating fibrefiber size: 1x1mm2
three outer-layersof scintillating fibrefiber size: 1x1mm2
AMADEUS setup Low-mass cryogenic gas target cell:T = 10 KP = 1.0 barRin = 5 cmRout = 15 cmL = 20 cm
International Workshop on Hadronic Atoms and Kaonic Nuclei
The AMADEUS trigger system
• Cilindrical layer of scintillating fibers surrounding the beam pipe to trigger K+ K- in opposite directions
• Readout to be done by SiPM
• Inner tracker (eventually, a first tracking stage before the DC)
• Target ( A gaseous He target for a first phase of study)
• Trigger (1 or 2 layers of ScFi surrounding the interaction point)
target
Trigger systemScFi + SiPM readout
K+
K-
A. Scordo
International Workshop on Hadronic Atoms and Kaonic Nuclei
Sketch of the AMADEUS setup
International Workshop on Hadronic Atoms and Kaonic Nuclei
View in beam direction
Cryo target cell
Beam pipe: Æ= 60 mm,thickness = 0.25 mmmade of BeAl alloy
Kaon trigger
International Workshop on Hadronic Atoms and Kaonic Nuclei
AMADEUS setup II
full toroidalcryogenictarget cell
vacuum chamber
thin-walledbeam pipe
2 outer-layer ofscintillating fibrefiber size: 1x1mm2
kaon trigger:2 inner-layer ofscintillating fibrefiber size: 1x1mm2
International Workshop on Hadronic Atoms and Kaonic Nuclei
Tracking device:TPC-GEM or3-4 C-GEMs
Target system:cylindrical
cryogenic cellin vacuum chamber
Kaon trigger:Scint. fiberswith SiPMs
25
AMADEUS setup – phase II
inner tracker
FEE
AMADEUS setup – phase II
Cylindrical GEMs
International Workshop on Hadronic Atoms and Kaonic Nuclei
Beam-pipe solutions
International Workshop on Hadronic Atoms and Kaonic Nuclei
Number of charged kaon pairs
N = L s b = 2.9 × 109 K-
2 fb
-1 = 2
× 1
039 c
m-2
inte
grat
ed
lum
inos
ity
0.49
bra
nchi
ng
ratio
for K
±
Total number of produced charged Kaon pairs for L = 2 fb-1
1 barn = 10-24 cm2
1 femtobarn = 10-15 barn = 10-
39 cm2
3 × 1
0-3
0 cm
2
F p
rodu
ctio
n
cros
s se
ctio
n
International Workshop on Hadronic Atoms and Kaonic Nuclei
Number of events for the channel:
K- +4He (K-ppn) + n with (K-ppn) +d
Assumptions: 20% stopped kaons Y = 5.10-4 (K-ppn) formation
BR for decay channel = 10% (with p + -)
For an integrated luminosity of 2 fb-1:
N = 3x109 x 0.2 (stops) x 5x10-4 (Y) x 0.1 (BR) = 30 000 ev
Detection efficiency for charged particles (40%) 12 000 ev
Detection efficiency for neutrons (30%) 3 600 evfor which both missing and invariant mass can be reconstructed International Workshop on Hadronic Atoms and Kaonic Nuclei
Beam time request
• 2 fb-1 of integrated luminosity with He4 target in order to study the tribaryon (S=-1)
• 2 fb-1 of integrated luminosity with He3 target in order to study the dibaryon (S=-1)
overall integrated luminosity of 4 fb-1
With the luminosity upgrade of DANE, the machine should deliver at least 500 pb-1/month, which means that the overall AMADEUS Phase-1 program could be completed in about 8 months
International Workshop on Hadronic Atoms and Kaonic Nuclei
AMADEUS R&D, construction and tests the R&D for AMADEUS are ongoing, construction, assembly and tests have to be finished 2010/11
roll-in of AMADEUS roll-in 2011/12 (end of KLOE step 0)
AMADEUS data taking for an integrated luminosity of about 4 fb-1
AMADEUS time schedule
International Workshop on Hadronic Atoms and Kaonic Nuclei
Conclusion
The goal of AMADEUS is to perform a complete measurement - formation and decay processes - of di - and tri-baryon antikaon-mediated bound nuclear systems in helium-3 and helium-4.
It will contribute to a definite answer of the existence of antikaon-mediated bound nuclear systems in light systems.
The antikaon – nucleon/nucleus interaction will be studied in detail with AMADEUS.
International Workshop on Hadronic Atoms and Kaonic Nuclei