Chapter 11: Problem 24
Describe the balloon analogy for cosmological expansion. Explain why it only appears that we are at the center of expansion of the universe.
Chapter 11: Problem 24
Describe the balloon analogy for cosmological expansion. Explain why it only appears that we are at the center of expansion of the universe.
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Get started for freeDraw a Feynman diagram to represents annihilation of an electron and positron into a photon.
Electrons and positrons are collided in a circular accelerator. Derive the expression for the center-of-mass energy of the particle.
Which of the following decays cannot occur because the law of conservation of lepton number is violated? (a) \(\mathrm{n} \rightarrow \mathrm{p}+\mathrm{e}^{-}\) (b) \(\mu^{+} \rightarrow \mathrm{e}^{+}+v_{\mathrm{e}}\) (c) \(\pi^{+} \rightarrow \mathrm{e}^{+}+v_{\mathrm{e}}+\bar{v}_{\mu}\) (d) \(\mathrm{p} \rightarrow \mathrm{n}+\mathrm{e}^{+}+v_{\mathrm{e}}\) (e) \(\pi^{-} \rightarrow \mathrm{e}^{-}+\bar{v}_{\mathrm{e}}\) (f) \(\mu^{-} \rightarrow \mathrm{e}^{-}+\bar{v}_{\mathrm{e}}+v_{\mu}\) (g) \(\Lambda^{0} \rightarrow \pi^{-}+\mathrm{p}\) (h) \(\mathbf{K}^{+} \rightarrow \mu^{+}+v_{\mu}\)
When an electron and positron collide at the SLAC facility, they each have 50.0 -GeV kinetic energies. What is the total collision energy available, taking into account the annihilation energy? Note that the annihilation energy is insignificant, because the electrons are highly relativistic.
Which of the following reactions cannot because the law of conservation of strangeness is violated? (a) \(\mathrm{p}+\mathrm{n} \rightarrow \mathrm{p}+\mathrm{p}+\pi^{-}\) (b) \(\mathrm{p}+\mathrm{n} \rightarrow \mathrm{p}+\mathrm{p}+\mathrm{K}^{-}\) (c) \(\mathrm{K}^{-}+\mathrm{p} \rightarrow \mathrm{K}^{-}+\sum^{+}\) (d) \(\pi^{-}+\mathrm{p} \rightarrow \mathrm{K}^{+}+\sum^{-}\) (e) \(\mathrm{K}^{-}+\mathrm{p} \rightarrow \Xi^{0}+\mathrm{K}^{+}+\pi^{-}\) (f) \(\mathrm{K}^{-}+\mathrm{p} \rightarrow \Xi^{0}+\pi^{-}+\pi^{-}\) (g) \(\pi^{+}+\mathrm{p} \rightarrow \Sigma^{+}+\mathrm{K}^{+}\) (h) \(\pi^{-}+\mathrm{n} \rightarrow \mathrm{K}^{-}+\Lambda^{0}\)
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