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1Meson resonance production in 15 GeV/c [pi symbol][superscript plus sign] interactions with liquid hydrogen

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“Meson resonance production in 15 GeV/c [pi symbol][superscript plus sign] interactions with liquid hydrogen” Metadata:

  • Title: ➤  Meson resonance production in 15 GeV/c [pi symbol][superscript plus sign] interactions with liquid hydrogen
  • Author:
  • Language: English
  • Number of Pages: Median: 184
  • Publisher: ➤  Nevis Laboratories, Columbia University, Physics Dept.
  • Publish Date:
  • Publish Location: Irvington-on-Hudson, N.Y

“Meson resonance production in 15 GeV/c [pi symbol][superscript plus sign] interactions with liquid hydrogen” Subjects and Themes:

Edition Identifiers:

Access and General Info:

  • First Year Published: 1975
  • Is Full Text Available: No
  • Is The Book Public: No
  • Access Status: No_ebook

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Nucleon

the strong interaction. (Before the discovery of quarks, the term "strong interaction" referred to just internucleon interactions.) Nucleons sit at the

Meson

antiquarks, usually one of each, bound together by the strong interaction. Because mesons are composed of quark subparticles, they have a meaningful physical

Nuclear force

The nuclear force (or nucleonnucleon interaction, residual strong force, or, historically, strong nuclear force) is a force that acts between hadrons

Strong interaction

massive, short lived mesons on this scale, the residual strong interaction obeys a distance-dependent behavior between nucleons that is quite different

Pion

pions, along with vector, rho and omega mesons, provides an explanation for the residual strong force between nucleons. Pions are not produced in radioactive

List of mesons

such as the nuclear interaction. Since mesons are composed of quarks, they participate in both the weak and strong interactions. Mesons with net electric

Kaon

violation in the weak interaction (most significantly, by the Wu experiment). Since the mesons decay through weak interactions, parity is not conserved

Muon

the more general term meson was adopted to refer to any such particle within the correct mass range between electrons and nucleons. Further, in order to

B meson

In particle physics, B mesons are mesons composed of a bottom antiquark and either an up (B+ ), down (B0 ), strange (B0 s) or charm quark (B+ c). The

Isospin

These considerations would also prove useful in the analysis of meson-nucleon interactions after the discovery of the pions in 1947. The three pions (π+