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K_L -> pi^0 nu nubar at the AGS (E926)
High Energy Physics - Experiment · Submitted 11 Mar 1999
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Backgrounds are suppressed to a level well below an anticipated signal in the range 3 x 10^{-11}.
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The abstract, sentence by sentence
A proposed experiment to measure K_L -> pi^0 nu nubar at the AGS (E926) is described. It adopts a unique but general strategy of rare decay measurements with two independent rejection criteria, which allows reliable measurements of background levels. The method employs hermetic veto and full kinematic reconstruction using kaon time of flight and kinematic reconstruction of pi^0. Backgrounds are suppressed to a level well below an anticipated signal in the range 3 x 10^{-11}.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | A proposed experiment to measure K_L -> pi^0 nu nubar at the AGS (E926) is described. | contribution 0.97 | 0.33 | 0.09 | asserted 0.96 |
| s1 | It adopts a unique but general strategy of rare decay measurements with two independent rejection criteria, which allows reliable measurements of background levels. | method 0.96 | 0.52 | 0.11 | asserted 1.00 |
| s2 | The method employs hermetic veto and full kinematic reconstruction using kaon time of flight and kinematic reconstruction of pi^0. | method 1.00 | 0.44 | 0.05 | asserted 1.00 |
| s3 | Backgrounds are suppressed to a level well below an anticipated signal in the range 3 x 10^{-11}. | result 0.86 | 0.43 | 0.45 | asserted 0.99 |
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The paper
Original abstract
A proposed experiment to measure K_L -> pi^0 nu nubar at the AGS (E926) is described. It adopts a unique but general strategy of rare decay measurements with two independent rejection criteria, which allows reliable measurements of background levels. The method employs hermetic veto and full kinematic reconstruction using kaon time of flight and kinematic reconstruction of pi^0. Backgrounds are suppressed to a level well below an anticipated signal in the range 3 x 10^{-11}.
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