Some properties of elementary particles or a determination of the lifetime of the neutral pi meson

Theoretical estimates of the lifetime of the neutral &pi; meson have indicated a value of the order of 10<sup>&minus;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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Bibliographic Details
Main Author: Evans, David Arthur
Published: University of Oxford 1963
Online Access:http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.734619
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Summary:Theoretical estimates of the lifetime of the neutral &pi; meson have indicated a value of the order of 10<sup>&minus;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>&pi;2</sub> mode (&pi;<sup>+</sup>&pi;<sup>0</sup>) provides a &pi;<sup>0</sup> of unique velocity and a direction directly opposite to that of the &pi;<sup>+</sup>; the latter being charged, leaves a track in the emulsion. The decay of the &pi;<sup>0</sup> is detected in emulsion if it takes place in the Dalitz mode:- &pi;<sup>0</sup> &gamma;+e<sup>+</sup>+e<sup>&minus;</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>&pi;2</sub> decays with the emission of a Dalitz pair. Other &pi;<sup>0</sup> producing decays of the K<sup>+</sup> (K<sub>&mu;3</sub>, K<sub>e3</sub>, &tau;&prime;) were at first indistinguishable from the desired K<sub>&pi;2</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 &tau;&prime; and 30% of the K<sub>&mu;3</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 &pi;<sup>0</sup> was defined as the intersection of the electron tracks with the line of flight of the &pi;<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 &pi;<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 &tau; decays of the K<sup>+</sup> (&pi;<sup>+</sup>&pi;<sup>+</sup>&pi;<sup>&minus;</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.