Chapter 39: Problem 5
Why are we unlikely to observe an isolated quark?
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Chapter 39: Problem 5
Why are we unlikely to observe an isolated quark?
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(a) By what factor must the magnetic field in a proton synchrotron be increased as the proton energy increases by a factor of \(10 ?\) Assume the protons are highly relativistic, so \(\gamma \gg 1 .\) (b) By what factor must the diameter of the accelerator be increased to raise the energy by a factor of 10 without changing the magnetic field?
What's the role of gluons?
Pions are the lightest mesons, with mass some 270 times that of the electron. Charged pions decay typically into a muon and a neutrino or antineutrino. This makes pion beams useful for producing beams of neutrinos, which physicists use to study those elusive particles. In a medical application during the late 20 th century, accelerator centers installed "biomedical beam lines" to test pions for cancer therapy. In these experiments, pions attached themselves to atomic nuclei within cancer cells. The nuclei would literally explode, delivering a "pion star" of cancer-killing nuclear debris. Unfortunately, results were not as encouraging as hoped, and enthusiasm for this technique has waned. The negative pion usually decays into a negative muon and one other particle. The other particle could be a. a proton. b. an antineutrino. c. a neutrino. d. an up quark.
Why did Yukawa conclude that the particle mediating the strong force should have nonzero mass?
Both the neutral kaon and the neutral \(\rho\) meson can decay to a pion- antipion pair. Which of these decays is mediated by the weak force? How can you tell?
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