2008
DOI: 10.1103/physrevd.77.112004
|View full text |Cite
|
Sign up to set email alerts
|

Final results from the KTeV experiment on the decayKLπ0γγ

Abstract: We report on a new measurement of the branching ratio B(KL → π 0 γγ) using the KTeV detector. We reconstruct 1982 events with an estimated background of 608, that results in B(KL → π 0 γγ) = (1.29 ± 0.03stat ± 0.05syst) × 10 −6. We also measure the parameter, aV , which characterizes the strength of vector meson exchange terms in this decay. We find aV = −0.31 ± 0.05stat ± 0.07syst. These results utilize the full KTeV data set collected from 1997 to 2000 and supersede earlier KTeV measurements of the branching… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

7
122
0

Year Published

2011
2011
2020
2020

Publication Types

Select...
9

Relationship

0
9

Authors

Journals

citations
Cited by 98 publications
(129 citation statements)
references
References 19 publications
7
122
0
Order By: Relevance
“…The B(KL → π 0 X) = 10 −4 , 10 −6 and 10 −8 are indicated on the plot. The green shaded region is constrained from KTEV search for KL → π 0 γγ assuming B(X → γγ) = 1 [20]. of the fact that K L → π 0 νν search is the neutrino flavor blind, these upper bounds would be the same order as the predictions of Eq.…”
Section: Heavy New Physicsmentioning
confidence: 92%
“…The B(KL → π 0 X) = 10 −4 , 10 −6 and 10 −8 are indicated on the plot. The green shaded region is constrained from KTEV search for KL → π 0 γγ assuming B(X → γγ) = 1 [20]. of the fact that K L → π 0 νν search is the neutrino flavor blind, these upper bounds would be the same order as the predictions of Eq.…”
Section: Heavy New Physicsmentioning
confidence: 92%
“…Their differential branching fractions are given by Eq. (66 We notice in the last row of Table 9 that a very stringent constraint arises from the current experimental upper limit on these modes [115]. The lepton-flavour-violating decays are absent in the SM and have not yet been seen in experiments.…”
Section: Rare Semileptonic Decays Of Kaonsmentioning
confidence: 96%
“…• The are also some searches of the rare decays K + → π + χχ with χχ = e + e − , µ + µ − , γγ, which have been performed by NA48/2 [41,42] and NA62 [43]. The neutral lepton decays K L → π 0 χχ (with χχ = e + e − , µ + µ − , γγ) are also searched for in the KTeV experiment [44][45][46]. In these searches, the electrons, muons and photons are all from the primary kaon decay vertex, thus they are not applicable for the long-lived S discussed here for the KOTO anomaly.…”
Section: Laboratory Constraintsmentioning
confidence: 99%