Chapter 39: Problem 3
How are baryons fundamentally different from leptons?
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Chapter 39: Problem 3
How are baryons fundamentally different from leptons?
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Is it possible for a charged particle to be its own antiparticle?
What forces are unified in the electroweak theory?
Is the interaction \(p+p \rightarrow p+\pi^{+}\) allowed? If not, what conservation law does it violate?
The \(\Sigma^{+}\) and \(\Sigma^{-}\) have quark compositions uus and \(d d s\), respectively. Are the \(\Sigma^{+}\) and \(\Sigma^{-}\) each other's antiparticles? If not, give the quark compositions of their antiparticles.
Your roommate is writing a science-fiction novel set very far in the future, 60 Gy after the Big Bang. One of the characters is a cosmologist, and your roommate wants to know what the cosmologist will measure for the Hubble constant. What's your answer, assuming a steady expansion rate?
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