ץ + n K 0 + Λ With decays: K 0 π 0 + π 0 Λ π 0 + n
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Proposal for an Experiment: Photoproduction of Neutral Kaons on Deuterium Spokespersons: D. M. Manley (Kent State University) W. J. Briscoe (The George Washington University) A. Starostin (UCLA). ץ + n K 0 + Λ With decays: K 0 π 0 + π 0 Λ π 0 + n - PowerPoint PPT Presentation
Transcript of ץ + n K 0 + Λ With decays: K 0 π 0 + π 0 Λ π 0 + n
Proposal for an Experiment: Photoproduction of Neutral Kaons on Deuterium
Spokespersons: D. M. Manley (Kent State University)
W. J. Briscoe (The George Washington University)A. Starostin (UCLA)
n K0 +Λ + ץ With decays: K0 π0 + π0
Λ π0 + n π0 ץ + ץ Net reaction:n + ץn 6 + ץ
The elementary strangeness photoproduction reactions
1. γ + p→K+ + Λ2. γ + p→K+ + Σ0
3. γ + p→K0 + Σ+
4. γ + n→K0 + Λ5. γ + n→K0 + Σ0
6. γ + n→K+ + Σ-
Kaon photoproduction is a fundamental process and an important tool for gaining new insights into nucleon resonances. Focus of this proposal is reaction (4), which serves as an isospin filter for N* resonances. Until very recently, there have been no experimental studies of this reaction.
Integrated cross section for π-p→K0Λ as a function of c.m. energy W
Prior PWAs and quark-model predictions suggest appreciable KΛ couplings for S11(1650) and P11(1710).
There is a possible hint of a narrow structure in the cross section near 1.7 GeV that merits investigation.
Isobar-model predictions for γp→K+Λ and γn→K0Λ using two different parameter sets
(a) and (c): predicted angular distributions at Eγ = 1.05 GeV
(b) and (d): predicted total cross sections
These calculations show the urgent need for γn→K0Λ data to constrain the models.
Theoretical considerations
The γn→K0Λ reaction is expected to help clarify the strangeness production mechanism because of the following features:
In contrast to γp→K+Λ, the Born term in the t channel does not contribute to γn→K0Λ because no charge is involved.
The strong coupling constants in the u channel for Σ0 and other isovector exchanges have the same value but are of opposite sign to those in γp→K+Λ because of isospin symmetry.
The electromagnetic coupling constants of resonances in the s channel (e.g., gN*nγ) and in
the t channel are different from those in γp→K+Λ.
The γn→K0Λ reaction excites only I=½ N* resonances in the s channel. At MAMI-C, we expect good statistics up to Eγ = 1400 MeV, corresponding to a c.m. energy W = 1.85 GeV.
Thus, we have full coverage of the “second resonance region”.
Prior measurements
Until very recently, there were NO experimental investigations of γn→K0Λ:
2006 – Data were measured in Fall 2006 as part of the g13 experiment at JLab for Eγ = 0.4-1.9 GeV and 0.5-2.5 GeV using tagged photons with circular polarization; no results of analysis have yet been published. [E. Munevar, B.L. Berman, and P. Nadel-Turoński (CLAS Collaboration), AIP Conf. Proc. 947, 146 (2007).]
2007 – Quasifree production of neutral kaons on 12C was measured for Eγ = 0.8-1.1 GeV using tagged photons at LNS of Tohoku University in Sendai, Japan. Momentum spectra and integrated cross sections were obtained, but dσ/dΩ could not be obtained due to limited kinematical acceptance. [T. Watanabe et al., Phys. Lett. B 651, 269 (2007).]
2008 – First measurement of K0 photoproduction on deuterium was reported. Data were measured for Eγ = 0.8-1.1 GeV using tagged photons at LNS of Tohoku University in Sendai, Japan. Extracted momentum spectra differed considerably in shape and magnitude from those predicted with Kaon-MAID. [K. Tsukada et al., Phys. Rev. C 78, 014001 (2008).]
Detector efficiency for γn→K0Λ calculated from MC simulation
Detector efficiency for background reaction γp→K0Σ+
December 2007 Test Run at MAMI-C
During 5-21 December 2007, 277 hours of beam time using unpolarized tagged photons incident on a LD2 target were obtained. Experimental
parameters are listed below:
Electron maximum beam energy: 1.508 GeV Tagged photon energy range : 0.4 – 1.4 GeV Beam current: 10-20 nA Radiator: 10 μm Cu Diameter of collimator: 4 mm Target: Liquid deuterium Target cell length: 4.76 ± 0.03 cm CB multiplicity: 2+
Some results of our analysis of these data will now be presented using kinematic fitting for event selection.
Invariant mass of 2ץ from all 6-cluster events (no kinematic fitting)
(Possible Combination of 6ץ to yield a π0 )
ץ+ ץ = π0
Kinematic fit and confidence level
Z-vertex of primary interaction from kinematic fit
Distance travelled by K0 and Λ
Invariant mass of 2 photons from pions produced in K0 decays in γn→K0Λ with kinematic fitting
Invariant mass of
2 photons from decay
KS →2π0→4γ in events
identified as from γn→K0Λ.
Invariant mass of 4 photons in γn→K0Λ
Invariant mass of
4 photons from
decay of KS in events identified as from γn→K0Λ.
Missing mass of 4 photons in γn→K0Λ
Missing mass of
4 photons from
decay of KS in events identified as from γn→K0Λ.
Missing mass of 4 photons in γp→K0Σ+
Missing mass of
4 photons from
decay of KS in events identified as from γp→K0Σ+.
Summary and beam-time request
Our main objective is to measure dσ/dΩ for γn→K0Λ with a precision of about 11%. We will also measure the Λ recoil polarization.
We need the maximum beam energy for MAMI-C, a 5-cm liquid deuterium target, and unpolarized (or circularly polarized) photons. We require a high multiplicity trigger.
We will simultaneously measure dσ/dΩ for γp→K0Σ+, which will provide a check of systematics since there are published cross sections for this reaction with which to compare our results.
Our requested beam time for data taking is 400 hours.
