I* + p+r* + p Width 100 MeV 200 400 600 800 KE of r (MeV) Figure 33.26 This graph shows the probability of an interaction between a n and a proton as a function of energy. The bump is interpreted as Number of interactions

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Accelerators such as the Triangle Universities Meson Facility (TRIUMF) in British Columbia produce secondary beams of pions by having an intense primary proton beam strike a target. Such “meson factories” have been used for many years to study the interaction of pions with nuclei and,
hence, the strong nuclear force. One reaction that occurs is
π+ + p → Δ++π+ + p , where the Δ++ is a very short-lived particle. The graph shows the probability of this reaction as a function of energy. The width of the bump is the uncertainty in energy due to the short lifetime of the Δ++ .
(a) Find this lifetime.
(b) Verify from the quark composition of the particles that this
reaction annihilates and then re-creates a d quark and a d 
antiquark by writing the reaction and decay in terms of
quarks.
(c) Draw a Feynman diagram of the production and decay of
the Δ++ showing the individual quarks involved.

I* + p+r* + p
Width 100 MeV
200
400
600
800
KE of r (MeV)
Figure 33.26 This graph shows the probability of an interaction between
a n and a proton as a function of energy. The bump is interpreted as
Number of interactions
Transcribed Image Text:I* + p+r* + p Width 100 MeV 200 400 600 800 KE of r (MeV) Figure 33.26 This graph shows the probability of an interaction between a n and a proton as a function of energy. The bump is interpreted as Number of interactions
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