Some properties of elementary particles or a determination of the lifetime of the neutral pi meson
Theoretical estimates of the lifetime of the neutral π meson have indicated a value of the order of 10<sup>−17</sup> secs. In order to determine the lifetime by flight distance measurements a method employing very fine resolution is required. Nuclear emulsions provide a...
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ndltd-bl.uk-oai-ethos.bl.uk-7346192018-05-12T03:14:16ZSome properties of elementary particles or a determination of the lifetime of the neutral pi mesonEvans, David Arthur1963Theoretical estimates of the lifetime of the neutral π meson have indicated a value of the order of 10<sup>−17</sup> secs. In order to determine the lifetime by flight distance measurements a method employing very fine resolution is required. Nuclear emulsions provide a medium for resolution of distances of the order of a micron. This experiment uses the same principle as that first tried by Harris et al.(1957). The decay at rest of the K<sup>+</sup> meson in the K<sub>π2</sub> mode (π<sup>+</sup>π<sup>0</sup>) provides a π<sup>0</sup> of unique velocity and a direction directly opposite to that of the π<sup>+</sup>; the latter being charged, leaves a track in the emulsion. The decay of the π<sup>0</sup> is detected in emulsion if it takes place in the Dalitz mode:- π<sup>0</sup> γ+e<sup>+</sup>+e<sup>−</sup> (br. ratio 1.2%). Detection is possible because of the emission of charged particles. A stack of Ilford L4 emulsions was exposed to a beam of stopping K mesons. After processing, the stack was scanned for K<sub>π2</sub> decays with the emission of a Dalitz pair. Other π<sup>0</sup> producing decays of the K<sup>+</sup> (K<sub>μ3</sub>, K<sub>e3</sub>, τ′) were at first indistinguishable from the desired K<sub>π2</sub> decays. In order to reduce this contamination, grain density measurements were made on the charged secondary from the K<sup>+</sup> decay. By rejecting events in which g* was greater than 1.3 all τ′ and 30% of the K<sub>μ3</sub> events were rejected. A correction factor was calculated to account for the remaining decays. The co-ordinates of the grains composing the events were measured relative to axes fixed in the field of view. A bifilar micrometer eyepiece was used which has the motions of the cross-wires digitised to enable rapid measurement. The co-ordinates were automatically punched out on to tape ready for input to the computer. The tracks of the particles were obtained by fitting straight lines to the measured co-ordinates. The decay point of the π<sup>0</sup> was defined as the intersection of the electron tracks with the line of flight of the π<sup>+</sup>. The point of production was taken as the foot of the perpendicular from the measured position of the K<sup>+</sup> on to the π<sup>+</sup> trajectory. The effects of errors due to measurement, "grain noise" and grain size were thoroughly investigated. Use was made of co-ordinate measurements on τ decays of the K<sup>+</sup> (π<sup>+</sup>π<sup>+</sup>π<sup>−</sup>) where it is known that the three tracks converge on the point of decay of the K<sup>+</sup>. An estimation of the lifetime was made using a likelihood calculation. It was discovered that the presence of events giving anomalous flight distances affected the estimate considerably. A suitable cutoff criterion was applied to reject these events.University of Oxfordhttp://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.734619https://ora.ox.ac.uk/objects/uuid:9c9972ee-d45e-49cb-906a-0363b6d7443dElectronic Thesis or Dissertation |
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Theoretical estimates of the lifetime of the neutral π meson have indicated a value of the order of 10<sup>−17</sup> secs. In order to determine the lifetime by flight distance measurements a method employing very fine resolution is required. Nuclear emulsions provide a medium for resolution of distances of the order of a micron. This experiment uses the same principle as that first tried by Harris et al.(1957). The decay at rest of the K<sup>+</sup> meson in the K<sub>π2</sub> mode (π<sup>+</sup>π<sup>0</sup>) provides a π<sup>0</sup> of unique velocity and a direction directly opposite to that of the π<sup>+</sup>; the latter being charged, leaves a track in the emulsion. The decay of the π<sup>0</sup> is detected in emulsion if it takes place in the Dalitz mode:- π<sup>0</sup> γ+e<sup>+</sup>+e<sup>−</sup> (br. ratio 1.2%). Detection is possible because of the emission of charged particles. A stack of Ilford L4 emulsions was exposed to a beam of stopping K mesons. After processing, the stack was scanned for K<sub>π2</sub> decays with the emission of a Dalitz pair. Other π<sup>0</sup> producing decays of the K<sup>+</sup> (K<sub>μ3</sub>, K<sub>e3</sub>, τ′) were at first indistinguishable from the desired K<sub>π2</sub> decays. In order to reduce this contamination, grain density measurements were made on the charged secondary from the K<sup>+</sup> decay. By rejecting events in which g* was greater than 1.3 all τ′ and 30% of the K<sub>μ3</sub> events were rejected. A correction factor was calculated to account for the remaining decays. The co-ordinates of the grains composing the events were measured relative to axes fixed in the field of view. A bifilar micrometer eyepiece was used which has the motions of the cross-wires digitised to enable rapid measurement. The co-ordinates were automatically punched out on to tape ready for input to the computer. The tracks of the particles were obtained by fitting straight lines to the measured co-ordinates. The decay point of the π<sup>0</sup> was defined as the intersection of the electron tracks with the line of flight of the π<sup>+</sup>. The point of production was taken as the foot of the perpendicular from the measured position of the K<sup>+</sup> on to the π<sup>+</sup> trajectory. The effects of errors due to measurement, "grain noise" and grain size were thoroughly investigated. Use was made of co-ordinate measurements on τ decays of the K<sup>+</sup> (π<sup>+</sup>π<sup>+</sup>π<sup>−</sup>) where it is known that the three tracks converge on the point of decay of the K<sup>+</sup>. An estimation of the lifetime was made using a likelihood calculation. It was discovered that the presence of events giving anomalous flight distances affected the estimate considerably. A suitable cutoff criterion was applied to reject these events. |
author |
Evans, David Arthur |
spellingShingle |
Evans, David Arthur Some properties of elementary particles or a determination of the lifetime of the neutral pi meson |
author_facet |
Evans, David Arthur |
author_sort |
Evans, David Arthur |
title |
Some properties of elementary particles or a determination of the lifetime of the neutral pi meson |
title_short |
Some properties of elementary particles or a determination of the lifetime of the neutral pi meson |
title_full |
Some properties of elementary particles or a determination of the lifetime of the neutral pi meson |
title_fullStr |
Some properties of elementary particles or a determination of the lifetime of the neutral pi meson |
title_full_unstemmed |
Some properties of elementary particles or a determination of the lifetime of the neutral pi meson |
title_sort |
some properties of elementary particles or a determination of the lifetime of the neutral pi meson |
publisher |
University of Oxford |
publishDate |
1963 |
url |
http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.734619 |
work_keys_str_mv |
AT evansdavidarthur somepropertiesofelementaryparticlesoradeterminationofthelifetimeoftheneutralpimeson |
_version_ |
1718636405599502336 |