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(a) Is the decay \({\sum ^{\rm{ - }}} \to {\rm{n + }}{\pi ^{\rm{ - }}}\) possible considering the appropriate conservation laws? State why or why not.

(b) Write the decay in terms of the quark constituents of the particles.

Short Answer

Expert verified

(a) The decay\({\sum ^{\rm{ - }}} \to {\rm{n + }}{\pi ^{\rm{ - }}}\)is possible considering the appropriate conservation laws as all quantities are conserved.

(b) The decay in terms of the quark constituents of the particles is \(\left( {{\rm{dds}}} \right) \to \left( {{\rm{udd}}} \right){\rm{ + }}\left( {{\rm{\bar ud}}} \right)\).

Step by step solution

01

Concept Introduction

The sum of the baryon numbers of all entering particles equals the sum of the baryon numbers of all particles produced by the reaction, according to the rule of conservation of baryon number.

Conservation of Lepton says that when a lepton of a given generation is formed or destroyed in a reaction, a matching antilepton of the same generation must also be created or destroyed.

The concept of conservation of charge states that in an isolated system, the total electric charge never changes. The net quantity of electric charge in the cosmos, which is equal to the amount of positive charge minus the amount of negative charge, is constantly preserved.

02

Decay of \({\sum ^{\rm{ - }}} \to {\rm{n + }}{\pi ^{\rm{ - }}}\)

(a)

Check the conservation laws and if the reaction violates one of them it won't occur. The conservation laws are as follows –

  • Conservation of Baryon number.
  • Conservation of Charge.
  • Conservation of Lepton numbers.

Now, the equation is written as –

\({\sum ^{\rm{ - }}} \to {\rm{n + }}{\pi ^{\rm{ - }}}\)

Before

After

\({\rm{B}}\)

\({\rm{1}}\)

\({\rm{1 + 0 = 1}}\)

\({\rm{Q}}\)

\({\rm{ - 1}}\)

\({\rm{0 + ( - 1) = - 1}}\)

\({{\rm{L}}_{\rm{e}}}\)

\({\rm{0}}\)

\({\rm{0}}\)

\({{\rm{L}}_{\rm{\mu }}}\)

\({\rm{0}}\)

\({\rm{0}}\)

\({{\rm{L}}_{\rm{\tau }}}\)

\({\rm{0}}\)

\({\rm{0}}\)

Therefore, the reaction is allowed.

03

Decay in terms of quark compositions

(b)

According to table \({\rm{33}}{\rm{.4}}\), the quark composition for each particle is –

\(\begin{aligned}{c}{\sum ^{\rm{ - }}}{\rm{ = }}\left( {{\rm{dds}}} \right)\\{\rm{n = }}\left( {{\rm{udd}}} \right)\\{\pi ^{\rm{ - }}}{\rm{ = }}\left( {{\rm{\bar ud}}} \right)\end{aligned}\)

Substituting the values in the reaction –

\(\left( {{\rm{dds}}} \right) \to \left( {{\rm{udd}}} \right){\rm{ + }}\left( {{\rm{\bar ud}}} \right)\)

Therefore, the decay is written as \(\left( {{\rm{dds}}} \right) \to \left( {{\rm{udd}}} \right){\rm{ + }}\left( {{\rm{\bar ud}}} \right)\).

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Most popular questions from this chapter

Suppose you are designing a proton decay experiment and you can detect \({\rm{50}}\) percent of the proton decays in a tank of water.

(a) How many kilograms of water would you need to see one decay per month, assuming a lifetime of \({\rm{1}}{{\rm{0}}^{{\rm{31}}}}{\rm{ y}}\)?

(b) How many cubic meters of water is this?

(c) If the actual lifetime is \({\rm{1}}{{\rm{0}}^{{\rm{33}}}}{\rm{ y}}\), how long would you have to wait on an average to see a single proton decay?

The mass of a theoretical particle that may be associated with the unification of the electroweak and strong forces is\[{\rm{1}}{{\rm{0}}^{{\rm{14}}}}{\rm{ GeV/}}{{\rm{c}}^{\rm{2}}}\]. (a) How many proton masses is this? (b) How many electron masses is this? (This indicates how extremely relativistic the accelerator would have to be in order to make the particle, and how large the relativistic quantity γ would have to be.)

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

(a) Write the decay in terms of the quark constituents.

(b) How much energy is released?

(c) What is the ultimate release of energy, given the decay mode for the pi zero is\({{\rm{\pi }}^{\rm{0}}} \to {\rm{\gamma + \gamma }}\)?

Explain how conservation of baryon number is responsible for conservation of total atomic mass (total number of nucleons) in nuclear decay and reactions.

How can the lifetime of a particle indicate that its decay is caused by the strong nuclear force? How can a change in strangeness imply which force is responsible for a reaction? What does a change in quark flavor imply about the force that is responsible?

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