A Proposal to Search for Charmed Particles Originating from the Interactions of 400 GeV/c Protons in Emulsion Nuclei
Abstract
There has been much recent discussion of the possibility of the existence of 'charmed' particles, hadrons which possess non-zero values of 'charm', a further additive quantum number. These particles may be generated either in the three triplet model of Han and Nambu or by the postulate of a fourth, charm-bearing quark. On the assumption that charm, like strangeness, is conserved in strong and electromagnetic interactions (the opposite assumption would necessitate charmed particles coupling strongly to ordinary hadrons and the existence of yet undiscovered states, e.g. Z*s) but not conserved in weak interactions one might expect their production either singly in neutrino interactions or in pairs in associated production in high energy hadron collisions, to be followed by their subsequent, relatively slow, decay into 'uncharmed' particles. Various estimates as to mass, lifetime, production cross-sections and decay modes have been made for these particles. However their failure to appear as di-lepton events among the neutrino interactions of the Brookhaven A.G.S. and CERN P.S. experiments might suggest that their masses are in excess of 2 GeV/c{sup 2} the other hand, such particles would have been expected to have been observed directly in bubble chamber studies at FNAL had their lifetimes been greater thanmore »
- Authors:
- Publication Date:
- Research Org.:
- Fermi National Accelerator Lab. (FNAL), Batavia, IL (United States)
- Sponsoring Org.:
- USDOE
- OSTI Identifier:
- 910471
- Report Number(s):
- FERMILAB-PROPOSAL-0364
TRN: US200724%%180
- DOE Contract Number:
- AC02-07CH11359
- Resource Type:
- Technical Report
- Country of Publication:
- United States
- Language:
- English
- Subject:
- 72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS; BUBBLE CHAMBERS; CROSS SECTIONS; ELECTROMAGNETIC INTERACTIONS; NUCLEI; PAIR PRODUCTION; PRODUCTION; PROTON BEAMS; PROTONS; QUANTUM NUMBERS; SPATIAL RESOLUTION; WEAK INTERACTIONS; HADRONS
Citation Formats
Sacton, J. A Proposal to Search for Charmed Particles Originating from the Interactions of 400 GeV/c Protons in Emulsion Nuclei. United States: N. p., 1974.
Web. doi:10.2172/910471.
Sacton, J. A Proposal to Search for Charmed Particles Originating from the Interactions of 400 GeV/c Protons in Emulsion Nuclei. United States. doi:10.2172/910471.
Sacton, J. Fri .
"A Proposal to Search for Charmed Particles Originating from the Interactions of 400 GeV/c Protons in Emulsion Nuclei". United States.
doi:10.2172/910471. https://www.osti.gov/servlets/purl/910471.
@article{osti_910471,
title = {A Proposal to Search for Charmed Particles Originating from the Interactions of 400 GeV/c Protons in Emulsion Nuclei},
author = {Sacton, J.},
abstractNote = {There has been much recent discussion of the possibility of the existence of 'charmed' particles, hadrons which possess non-zero values of 'charm', a further additive quantum number. These particles may be generated either in the three triplet model of Han and Nambu or by the postulate of a fourth, charm-bearing quark. On the assumption that charm, like strangeness, is conserved in strong and electromagnetic interactions (the opposite assumption would necessitate charmed particles coupling strongly to ordinary hadrons and the existence of yet undiscovered states, e.g. Z*s) but not conserved in weak interactions one might expect their production either singly in neutrino interactions or in pairs in associated production in high energy hadron collisions, to be followed by their subsequent, relatively slow, decay into 'uncharmed' particles. Various estimates as to mass, lifetime, production cross-sections and decay modes have been made for these particles. However their failure to appear as di-lepton events among the neutrino interactions of the Brookhaven A.G.S. and CERN P.S. experiments might suggest that their masses are in excess of 2 GeV/c{sup 2} the other hand, such particles would have been expected to have been observed directly in bubble chamber studies at FNAL had their lifetimes been greater than 10{sup -11}s as suggested by some authors. This proposal, which may be thought of as complementary to that of Burhop et al, is for a straightforward exposure of a stack of emulsions to a 400 GeV/c proton beam to look for evidence of the pair production of charmed particles. The spatial resolution of the emulsion technique is about one micron with the consequence that the decays of particles of mean lives in the range 10{sup -11} to 10{sup -14} s should be readily observable.},
doi = {10.2172/910471},
journal = {},
number = ,
volume = ,
place = {United States},
year = {Fri Nov 01 00:00:00 EST 1974},
month = {Fri Nov 01 00:00:00 EST 1974}
}
-
A stack of nuclear emulsions was irradiated by 400 Gev/c protons at FNAL. In this work a search for the short-lived particles has been carried out by a new method that allowed to detect secondary events (including the narrow ones) on short distances from the parent star. By measuring angles, momenta and ionizations of the secondary particles they could identify electrons and distinguish them from hadrons. In search for the decays of charged of particles on n{sub s} {ge} 3 charged relativistic particles or of neutral ones on two or four charged particles the environments of the 1120 stars hasmore »
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Interactions of 400-GeV/c protons with emulsion nuclei. Multiplicity of charged particles
The principal characteristics of multiplicity distributions and correlations are presented and discussed for various types of secondary charged particles from inelastic interactions of 400-GeV protons with the nuclei of nuclear emulsions, and also their energy dependence in the energy region up to 400 GeV. -
MESON PRODUCTION IN THE INTERACTIONS OF 26.7 Gev/c PROTONS WITH EMULSION NUCLEI
One-hundred-thirty-three interactions initiated in nuclear emulsions by 26.7 Bev/c protons are studied. The events are subject to separation into two groups, one in which most of the shower particles are emitied in a single nucleon- nucleon coliision in the target nucleus, the other in which multiple collisions produce the particles. Experimental procedure, classification of events, identification of tracks, and various distributions are discussed. Graphs of distributions are included. (27 references.) (D.C.W.)