(a) Show that all combinations of three quarks produce integral charges. Thus, baryons must have integral charge.

(b) Show that all combinations of a quark and an antiquark produce only integral charges. Thus, mesons must have integral charge.

Short Answer

Expert verified

(a) There are four combinations of the three quarks that lead to the result - baryons must have integral charge.

(b) There are four combinations of the quarks and antiquarks that lead to the result - mesons must have integral charge.

Step by step solution

01

Concept Introduction

A baryon is a type of composite subatomic particle in particle physics category which contains an odd number of valence quarks.

A quark is defined as the basic ingredient of matter and a sort of elementary particle.

Antiquarks are defined as the antiparticles that correspond to each flavour of quark.

02

Baryons having Integral Charge

(a)

Since baryons are formed by combinations of \({\rm{3}}\) quarks, and since there are only two charges for the quarks: \(\frac{{{\rm{ - 1}}}}{{\rm{3}}}\) and \(\frac{{\rm{2}}}{{\rm{3}}}\), then there would be \(4\) combinations of those quarks such that –

First combination;

\(\frac{{ - 1}}{3} + \frac{{ - 1}}{3} + \frac{{ - 1}}{3} = - 1\)

Second combination;

\(\frac{{ - 1}}{3} + \frac{{ - 1}}{3} + \frac{2}{3} = 0\)

Third combination;

\(\frac{2}{3} + \frac{2}{3} + \frac{2}{3} = 2\)

Fourth combination;

\(\frac{{ - 1}}{3} + \frac{2}{3} + \frac{2}{3} = 1\)

As here all the combination of three quarks produce integral charges. This leads to the fact that baryons must have integral charge.

Therefore, baryons have integral charge.

03

Mesons having Integral Charge

(b)

Since mesons are formed by combinations of one quark and one antiquark, and since there are only two charges for the quarks: \(\frac{{{\rm{ - 1}}}}{{\rm{3}}}\) and \(\frac{{\rm{2}}}{{\rm{3}}}\), and only two charges for the antiquarks: \(\frac{{\rm{1}}}{{\rm{3}}}\) and \(\frac{{{\rm{ - 2}}}}{{\rm{3}}}\) then there would be \(4\) forms of those mesons given by –

First combination;

\(\frac{2}{3} + \frac{1}{3} = 1\)

Second combination;

\(\frac{2}{3} - \frac{1}{3} = 0\)

Third combination;

\(\frac{{ - 1}}{3} + \frac{1}{3} = 0\)

Fourth combination;

\(\frac{{ - 1}}{3} - \frac{2}{3} = - 1\)

As here all the combination of quarks produce integral charges. This leads to the fact that mesons must have integral charge.

Therefore, mesons have integral charge.

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Most popular questions from this chapter

(a) How much energy would be released if the proton did decay via the conjectured reaction \({\rm{p}} \to {\pi ^{\rm{0}}}{\rm{ + }}{{\rm{e}}^{\rm{ + }}}\)?

(b) Given that the \({\pi ^{\rm{0}}}\) decays to two \(\gamma {\rm{ s}}\) and that the \({{\rm{e}}^{\rm{ + }}}\) will find an electron to annihilate, what total energy is ultimately produced in proton decay?

(c) Why is this energy greater than the proton’s total mass (converted to energy)?

(a) What is the uncertainty in the energy released in the decay of a \(\tau {\rm{ }} - \)due to its short lifetime?

(b) Is the uncertainty in this energy greater than or less than the uncertainty in the mass of the tau neutrino? Discuss the source of the uncertainty.

What evidence is cited to support the contention that the gluon force between quarks is greater than the strong nuclear force between hadrons? How is this related to color? Is it also related to quark confinement?

(a) Verify from its quark composition that the \({\rm{\Delta + }}\)particle could be an excited state of the proton.

(b) There is a spread of about \({\rm{100 MeV}}\) in the decay energy of the \({\rm{\Delta + }}\), interpreted as uncertainty due to its short lifetime. What is its approximate lifetime?

(c) Does its decay proceed via the strong or weak force?

(a) What is the uncertainty in the energy released in the decay of a \({{\rm{\pi }}^{\rm{0}}}\)due to its short lifetime?

(b) What fraction of the decay energy is this, noting that the decay mode is \({{\bf{\pi }}^{\bf{0}}} \to {\bf{\gamma }}{\rm{ }} + {\rm{ }}{\bf{\gamma }}\) (so that all the \({\rm{\pi ^0}}\)mass is destroyed)?

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