1997
DOI: 10.1016/s0370-2693(97)01193-3
|View full text |Cite
|
Sign up to set email alerts
|

Measurement of the neutral kaon regeneration amplitude in carbon at momenta below 1 Gev/c

Abstract: The neutral kaon regeneration amplitude in carbon at momenta between 250 and 750 MeV/c was determined by measuring the interference of inherent and coherently regenerated K S amplitudes. This interference appears in the rates of initially pure (tagged) K 0 and K 0 decaying to + after crossing a carbon absorber.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

2
13
0

Year Published

1999
1999
2021
2021

Publication Types

Select...
6
2

Relationship

0
8

Authors

Journals

citations
Cited by 27 publications
(15 citation statements)
references
References 18 publications
2
13
0
Order By: Relevance
“…Regeneration was corrected on an event-by-event basis using the amplitudes measured by CPLEAR [96], depending on the momentum of the neutral kaon and on the positions of its production and decay vertices. Typically, this correction amounts to a positive shift of the asymmetry A exp T of 0.3 × 10 −3 with an error dominated by the amplitude measurement.…”
Section: Weighting Eπν Events and Building Measured Asymmetriesmentioning
confidence: 99%
“…Regeneration was corrected on an event-by-event basis using the amplitudes measured by CPLEAR [96], depending on the momentum of the neutral kaon and on the positions of its production and decay vertices. Typically, this correction amounts to a positive shift of the asymmetry A exp T of 0.3 × 10 −3 with an error dominated by the amplitude measurement.…”
Section: Weighting Eπν Events and Building Measured Asymmetriesmentioning
confidence: 99%
“…A dedicated experimental setup had been used to improve the knowledge on regeneration amplitudes, magnitudes and phases, in the momentum range relevant for the CPLEAR experiment. 4 The effect is being corrected for by applying a weight to each K 0 (K 0 ) event equal to the ratio of the decay probabilities for an initial K 0 (K 0 ) propagating in vacuum and through the detector.…”
Section: The Cplear Experimental Methodsmentioning
confidence: 99%
“…Whenever the LEAR machine was ready to take a shot (≈ 5 × 10 9 ) of p , the AA released a part of its stack to the PS, where the p 's were decelerated to 609 MeV/c , injected into LEAR, and stochastically cooled down for another 5 min to a momentum spread of σ p /p = 10 −3 . This was followed by electron cooling, resulting in a relative momentum spread of only 5×10 − 4 . LEAR had been equipped with fast and ultra-slow extraction systems, the latter being used for the CPLEAR experiment providing a rate of 1 MHz antiprotons in spills of about 1 h. The last part of extraction line comprised two horizontal and two vertical bending magnets followed by a quadrupole doublet to align and focus the beam on the target in the centre of the detector.…”
Section: The Low Energy Antiproton Ringmentioning
confidence: 99%
“…Each event selected, labeled by the initial kaon strangeness and the decay electron charge, was then properly weighted before forming the numbers N of events entering the asymmetries A Weighting eπν events and building measured asymmetries Regeneration was corrected on an event-by-event basis using the amplitudes measured by CPLEAR [92], depending on the momentum of the neutral kaon and on the positions of its production and decay vertices. Typically, this correction amounts to a positive shift of the asymmetry A exp T of 0.3 × 10 −3 with an error dominated by the amplitude measurement.…”
Section: Selection Of Eπν Eventsmentioning
confidence: 99%