Chapter 33: Q15CQ (page 1211)
Explain how the weak force can change strangeness by changing quark flavor.
Short Answer
Weak force can change strangeness by decay path \[s \to u + {W^ - }.\]
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Chapter 33: Q15CQ (page 1211)
Explain how the weak force can change strangeness by changing quark flavor.
Weak force can change strangeness by decay path \[s \to u + {W^ - }.\]
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What are the advantages of colliding-beam accelerators? What are the disadvantages?
There are particles called \({\rm{D}}\)-mesons. One of them is the \({{\rm{D}}^{\rm{ + }}}\) meson, which has a single positive charge and a baryon number of zero, also the value of its strangeness, topness, and bottomness. It has a charm of \({\rm{ + 1}}\). What is its quark configuration?
(a) Is the decay \({{\rm{\Lambda }}^{\rm{0}}} \to {\rm{n + }}{{\rm{\pi }}^{\rm{0}}}\) possible considering the appropriate conservation laws? State why or why not.
(b) Write the decay in terms of the quark constituents of the particles.
What lifetime do you expect for an antineutron isolated from normal matter?
Suppose a \[{{\rm{W}}^{\rm{ - }}}\]created in a bubble chamber lives for \[{\rm{5}}{\rm{.00 \times 1}}{{\rm{0}}^{{\rm{ - 25}}}}{\rm{\;s}}\]. What distance does it move in this time if it is traveling at \[{\rm{0}}{\rm{.900c}}\]? Since this distance is too short to make a track, the presence of the \[{{\rm{W}}^{\rm{ - }}}\]must be inferred from its decay products. Note that the time is longer than the given \[{{\rm{W}}^{\rm{ - }}}\]lifetime, which can be due to the statistical nature of decay or time dilation.
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