Gap measurement as a method of analysing cosmic ray stars in photographic emulsions

Author(s):  
P.E. Hodgson
1950 ◽  
Vol 28a (6) ◽  
pp. 616-627 ◽  
Author(s):  
E. Pickup ◽  
L. Voyvodic

One of the more interesting features of cosmic ray stars is that [Formula: see text] nuclei are ejected occasionally in the nuclear disintegrations. Such nuclei are characterized by the fact that, at the end of their range, they suffer radioactive decay (τ = 0.9 sec.) into [Formula: see text], which immediately splits up into two oppositely directed α-particles, giving what is usually referred to as a hammer track. In this investigation numerous examples have been observed of the emission of such nuclei in stars in photographic emulsions, the stars having from 2 to 60 prongs. In particular, it has been shown that the energy spectrum of the α-particles forming the hammer tracks is in good agreement with that observed by other workers, and also with experiments made, using the cloud chamber technique, indicating that the [Formula: see text] in this disintegration is formed in the excited state. When an electron sensitive emulsion is used it is shown that the hammer track is accompanied by the [Formula: see text] disintegration electron. The energy spectrum of the [Formula: see text] nuclei is plotted, and the mechanism of the formation is discussed for both large and small stars.


1957 ◽  
Vol 4 ◽  
pp. 29-38 ◽  
Author(s):  
I.A. Ivanovskaya ◽  
D.S. Chernavsky

1954 ◽  
Vol 9 (2) ◽  
pp. 147-149 ◽  
Author(s):  
Shin-ichi Kaneko ◽  
Tadayoshi Kubozoe ◽  
Masaomi Takahata

1952 ◽  
Vol 86 (5) ◽  
pp. 796-797 ◽  
Author(s):  
J. Y. Mei ◽  
E. Pickup

1951 ◽  
Vol 29 (4) ◽  
pp. 263-273 ◽  
Author(s):  
E. Pickup ◽  
L. Voyvodic

It has been found that a certain proportion of the fragments emitted in cosmic ray stars formed at about 85,000 ft. consists of radioactive nuclei, i.e., in electron sensitive photographic emulsions, tracks of electrons with energies of several mega electron volts can be seen originating at the end of the track of the fragment. Details of such events are given, together with energy measurements for the disintegration electrons made by the multiple Coulomb scattering method. The significance of the results, and possible identification of the fragments, are discussed.


The masses of the secondary particles emitted from disintegrations produced by cosmic-ray protons of energy greater than 2 GeV have been determined by observations on the grain density and scattering of their tracks in photographic emulsions. It has thus been possible to determine the yield of the heavy charged mesons with mass between 900 and 1400 m e , as a function of the energy of the primary particles. Among 325 secondary particles which produce tracks with grain density between 1⋅07 and 2⋅0 times the minimum value, twenty heavy mesons have been identified. The statistical distribution in the measured values of their mass is consistent with a unique value of 1210±40 m e . The total observed proper time of flight of these particles is 2⋅9 x 10 -10 s; no example of decay 'in flight’ has yet been observed. The rate of production of these heavy mesons, referred to as K -particles, has been compared with the frequency with which heavy mesons are observed to decay at rest; the ratio is consistent with the estimated lifetime of the K -particles. In the disintegrations produced by primary particles of energy greater than ~ 20 GeV, approximately equal energy goes into production of π-and K -particles. The yield of K -particles at a primary energy of 2 to 3 GeV is estimated to be a few per cent per primary interaction. The results suggest th at not only π-mesons but also K -mesons are ‘heavy quanta’ associated with the nuclear field. If charged mesons of mass between 276 and 900 m e are created directly in showers, they occur with a frequency < 1 % of the π-particles.


1952 ◽  
Vol 30 (5) ◽  
pp. 453-458 ◽  
Author(s):  
J. Y. Mei

In an analysis of cosmic ray stars found in Ilford G5 emulsions exposed at about 85,000 ft. the star-size distribution curve shows a change in slope at a prong number of about 8.5. A similar effect is shown for emulsions exposed at airplane altitudes, and it is assumed that the effect is mainly due to the composition of the emulsions. While the primary particles producing the stars at about 85,000 ft. are mostly protons, about 50% of the low energy stars are produced by nonionizing radiation, presumably neutrons. a-Particles and heavier nuclei produce about 30% of the larger energetic stars. The absolute frequency of star production is given.


1951 ◽  
Vol 82 (2) ◽  
pp. 265-265 ◽  
Author(s):  
E. Pickup ◽  
L. Voyvodic

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