Spelling suggestions: "subject:"buclear emulsions"" "subject:"anuclear emulsions""
1 
Investigation of mesonic interaction processes in nuclear emulsionsGoodhead, Dudley T. January 1965 (has links)
No description available.

2 
An investigation of the spurious scattering of high energy particles in nuclear emulsionJones, James Jordan, 1938 January 1963 (has links)
No description available.

3 
The mass spectrum of cosmic ray primariesGoldberg, Harvey Jay. January 1966 (has links)
Call number: LD2668 .T4 1966 G618 / Master of Science

4 
The search for a unit magnetic pole in nuclear emulsionsParnell, Darrell Ray. January 1959 (has links)
Call number: LD2668 .T4 1959 P38

5 
Nuclear decay scheme studies of some tantalum and terbium isotopesFaler, Kenneth T. January 1959 (has links)
ThesisUniversity of California, Berkeley, 1959. / Includes bibliographical references (p. 8184).

6 
Interactions of 200 GeV protons with emulsion nuclei.Hartner, Gerd F. January 1973 (has links)
No description available.

7 
Interactions of 200 GeV protons with emulsion nuclei.Hartner, Gerd F. January 1973 (has links)
No description available.

8 
A rangeionization method to identify stopping Kaons in ILFord G.5 nuclear emulsionElkadi, Sadiq Mohamed 03 June 2011 (has links)
The identification of stopping charged particles in G.5 nuclear emulsion by using a residual range ionization method has been investigated in this experiment using a large stack of ILFord, G.5 nuclear emulsion pellicles exposed to 450 and 435 Me V/c K ˉ mesons at the Berkeley Bevatron.The restricted rate of energy loss vs kinetic energy for protons has been calculated theoretically, and given in Barkas(9). Then for given values of B , we calculated the restricted rate of energy loss vs the kinetic energy of muon, pion, kaon, and sigma particles.The measurement of the residual range and the counting of blobs in each residual range segment were carried out for four known stopping pions tracks. A second degree polynomial computer fit program was used to interpret the plot of residual range vs blobs/100 μ m. Then a particular point on the plot was chosen as a reference for normalizing the relative grain density (g*), theoretically and experimentally. Next, theoretical tables of residual range (R) vs relative grain density (g*theo) were calculated for muons, pions, kaons, protons, and sigmas. Those portions of the latter tables, for which (g*theo) was less than  2, were used for the above mentioned theoretical plot of residual range (R) vs relative grain density (g* theo). The theoretically predicted curves were then tested by experimentally measuring the residual range and counting the blobs of each range segment of two selected stopping particle (primary) tracks which we suspected to be stopping kaon tracks. Then the second degree polynomial computer fit to the plotted data of the measured residual range vs blobs/l00 μm was carried out for each of the two suspected stopping kaon particles. Three points from each curve were picked and superimposed on the theoretical curves. The results were good but showed that it is necessary to measure a sufficiently long residual range, and more than one segment of blobcounts should be used along the measured residual range for accurate identification of the given particle.Ball State UniversityMuncie, IN 47306

9 
The impact of TeV nucleusnucleus simulations on JACEE results /Zager, Eric Louis, January 2002 (has links)
Thesis (Ph. D.)University of Washington, 2002. / Vita. Includes bibliographical references (p. 7176).

Page generated in 0.0601 seconds