KTeV KL->pi pi gamma plots
Updated August 29, 2006.
[KL->pi pi gamma Results]
Plots from
[PRD74 (2006)]
[PRL86 (2001)]
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pmgmass4.eps,
pmgmass4.pdf
FIG.1. pi+pi-gamma mass for events passing all KL->pi+pi-gamma physics cuts except for the Mpi+pi-gamma cut. Crosses are data and the solid line is fit to the background components.
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cosprlplot8.eps,
cosprlplot8.pdf
FIG.2. Likelihood fit to the two indepedent variables in the KL rest frame: a) the angle theta between the pi+ and the gamma in the pi+pi- center of mass and
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egprlplot8.eps,
egprlplot8.pdf
FIG.2.b) the photon energy spectrum Egamma in the KL rest frame. The compoenents of the photon energy spectrum and the cos theta spectrum due to the bremsstrahlung and M1 direct emission processes are shown.
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060214_6.eps,
060214_6.pdf
FIG.3. 90% CL contours of gM1 vs. a1/a2 for various experimental measurements; 90% CL results from the KL->pi+pi-gamma mode from this paper (5-shaded contour) with the 68% CL contour also shown (white contour); For comparison, we show the results from the KL->pi+pi-e+e- mode for NA48 data (3-dotted countour) of Ref. [7], for KTeV 1997 data (2-dashed contour) in Ref.[5], and for KTeV 1997+1999 data (4-solid contour) of Ref.[6], and for a1/a2 from earlier KTeV 96 KL->pi+pi-gamma data (1-light gray vertical region) of Ref.[3].
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belz0404fig8.eps,
belz0404fig8.pdf
FIG.1. The decay KL->pi+pi-gamma arises preliminary from the contributions of the electric dipole (E1) "inner Bremsstrahlung" (left) and
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belz0404fig7.eps,
belz0404fig7.pdf
magnetic dipole (M1) "Direct emission" (right) diagrams above.
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linmas.eps,
linmas.pdf
FIG.2. (a) Mpipig distribution of cnadidate KL0->pi+pi-gamma events, all other cuts applied. Arrows indicate final cuts at Mk+-8 MeV/c2.
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logpt2.eps,
logpt2.pdf
(b) Kaon transverse momentum squared (PT2) distribution of candidate KL0->pi+pi-gamma events, all other cuts applied. The cut on this quntity required events to be within the first bin (0.000250 GeV2/c2) on this plot.
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egcom.eps,
egcom.pdf
FIG.3. KL0->pi+pi-gamma Monte Carlo/data overlay of photon energy distribution in the center of mass, for the rho-propagator fit result (Table I). Shown also (shaded) are the expected distributions for pure E1 inner Bremsstrahlung nd form-factor-modified M1 direct emission. The "combined" Monte Carlo plot shown assumes these two are the only contribution to the deay.
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ffcomp.eps,
ffcomp.pdf
FIG.4. Ratio (points) of (IB-subtracted) direct-emission data to teh expectation for a pure M1 E*gamma spectrum. Vertical scale is arbitrary. Shown for comparison are the best-fit results (Table I) for the rho-propagator (solid), linear (dashed), and quadratic (dotted) form-factor parametrizations. A modification to the pure-M1 spectrum is clearly supported by the data.
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