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Theta+ Analysis Updates [K-p mode]
Theta+ & L* differential cross section - Rough estimations have been shown. (Theta+:~15 nb & L*: ~1 ub in total cross section) - L* isospin asymmetry is indicated. BG shape estimations needed for precise cross sections MC-based estimation: better for smaller samples & L* - KKp + KL* w/o phi & higher MKp tail has been shown at EINN. - off-shell correction was updated for new ntuple production. Remaining part of BG estimation will be shown. (not completed)
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Off-shell correction Solid line : new correction [EN = MN – BE/2]
Dashed line: original correction [EN = MN – BE – PS2/2MS] KKp MMd(g,K-p) KL* MMd(g,K-p) Differences are small but slightly sharper w/ new correction.
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Inclusion of phi w/ LH2 data
phi MC w/ realistic t-dependence and spin density matrix Energy & polar angle filters were obtained from LH2 Normalization in < MKK < GeV & cosKp < 0 Ecms dependence Kp dependence
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Consistency with LH2 data
GeV : chi2 = , prob = 0.142 GeV : chi2 = , prob = 0.166 GeV : chi2 = , prob = 0.746 GeV : chi2 = , prob = 0.066
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Application to LD2 data w/ phi
Threshold improved by true MMd(g,K-p) at MC level > MK+ + Mn phi normalization improved in higher energies w/ cosKp < 0. Ecms<2.10 2.10<Ecms<2.18 2.18<Ecms<2.26 2.26<Ecms
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Inclusion of MK-p tail w/ LD2 data
No way to deduce from LH2 data ECMS, CMS(K-p), CMS(p), PCMS(p), PCMS(K-) dependences from LD2 data – KKp MC – KL* MC w/ MKK > GeV These dependences were applied to non-resonant KKp MC with Fermi motion. [Note: It does not look that acceptance corrected MKK and MK-p distributions indicate KK or K-p resonances.]
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Application to LD2 data w/ MKp tail
Filters were made by using MKp>1.54 GeV
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Consistencies in side bands
M(K-p) < 1.50 GeV M(K-p) > 1.54 GeV
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Inclusion of phi and MKp tail
Ecms dependence of M(K-p) Ecms dependence of M(KK) Generally consistencies are good.
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Over-estimation of MKp tail
Solid line: (1.45<MKp< <MKp<1.59)x0.4 Dashed line: KKp MC + MKp tail MC Note: phi and L* is not included. MMd(g,K-p) shape looks good but over-estimated.
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