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The reaction \({{\rm{\pi }}^{\rm{ + }}}{\rm{ + p}} \to {{\rm{\Delta }}^{{\rm{ + + }}}}\) (described in the preceding problem) takes place via the strong force.

(a) What is the baryon number of the \({{\rm{\Delta }}^{{\rm{ + + }}}}\)particle?

(b) Draw a Feynman diagram of the reaction showing the individual quarks involved.

Short Answer

Expert verified

a. The baryon number of \({{\rm{\Delta }}^{{\rm{ + + }}}}\)particle is\({\rm{ + 1}}\).

b. The Feynman diagram for the reaction \({\pi ^ + } + p \to {\Delta ^{ + + }}\) is drawn.

Step by step solution

01

Definition of Concept

A graphical representation of the reactions that represent the interactions between elementary particles and the product formed in the reaction is called Feynman diagram. They are named after the famous scientist Richard Feynman.

02

Find the baryon number of the \({{\rm{\Delta }}^{{\rm{ +  + }}}}\) particle

(a)

The baryon number of\({{\rm{\pi }}^{\rm{ + }}}\)is 0

the baryon number of a proton is\({\rm{ + 1}}\).

Let the baryon number of\({{\rm{\Delta }}^{{\rm{ + + }}}}\)is\(b\).

for the given reaction-

\({\pi ^ + } + p \to {\Delta ^{ + + }}\)

\({\rm{Baryon number}}:0 + 1 \to b\)

In order to conserve baryon number for the given reaction, the baryon number on both sides of the reaction must be same. So, baryon number of the\({{\rm{\Delta }}^{{\rm{ + + }}}}\)particle should be equal to\({\rm{ + 1}}\).

Also, based on the quark structure,\({\Delta ^{ + + }} = uuu\)

The baryon number of a u quark is\({\rm{ + }}\frac{{\rm{1}}}{{\rm{3}}}\).

As a result, the baryon number is given as-

\(\begin{array}{c}B = \frac{1}{3} + \frac{1}{3} + \frac{1}{3}\\ = 1\end{array}\).

Therefore, the requiredbaryon number of\({{\rm{\Delta }}^{{\rm{ + + }}}}\)particle is\({\rm{ + 1}}\).

03

Draw a Feynman diagram of the reaction

(b)

Below is a Feynman diagram for the reaction \({\pi ^ + } + p \to {\Delta ^{ + + }}\).

Therefore, the Feynman diagram for the reaction \({\pi ^ + } + p \to {\Delta ^{ + + }}\) is drawn.

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Most popular questions from this chapter

(a) Calculate the relativistic quantity \(\gamma {\rm{ = }}\frac{{\rm{1}}}{{\sqrt {{\rm{1 - }}{{\rm{v}}^{\rm{2}}}{\rm{/}}{{\rm{c}}^{\rm{2}}}} }}\) for \({\rm{1}}{\rm{.00 - TeV}}\) protons produced at Fermilab.

(b) If such a proton created a \({\pi ^{\rm{ + }}}\) having the same speed, how long would its life be in the laboratory?

(c) How far could it travel in this time?

What length track does a \[{{\rm{\pi }}^{\rm{ + }}}\]traveling at 0.100c leave in a bubble chamber if it is created there and lives for \[{\rm{2}}{\rm{.60 \times 1}}{{\rm{0}}^{{\rm{ - 8}}}}{\rm{\;s}}\]? (Those moving faster or living longer may escape the detector before decaying.)

One decay mode for the eta-zero meson is\({{\rm{\eta }}^{\rm{0}}} \to {\rm{\gamma + \gamma }}\).

(a) Find the energy released.

(b) What is the uncertainty in the energy due to the short lifetime?

(c) Write the decay in terms of the constituent quarks.

(d) Verify that baryon number, lepton numbers, and charge are conserved.

The decay mode of the positive tau is\({{\bf{\tau }}^ + } \to {\rm{ }}{{\bf{\mu }}^ + }{\rm{ }} + {\rm{ }}{{\bf{\nu }}_{\bf{\mu }}}{\rm{ }} + {\rm{ }}{{\bf{\bar \nu }}_{\bf{\tau }}}\).

(a) What energy is released?

(b) Verify that charge and lepton family numbers are conserved.

(c) The \({\tau ^ + }\)is the antiparticle of the \({\tau ^ - }\). Verify that all the decay products of the \({\tau ^ + }\)are the antiparticles of those in the decay of the \({\tau ^ - }\) given in the text.

(a) Show that the conjectured decay of the proton, \({\rm{p}} \to {\pi ^{\rm{0}}}{\rm{ + }}{{\rm{e}}^{\rm{ + }}}\), violates conservation of baryon number and conservation of lepton number.

(b) What is the analogous decay process for the antiproton?

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