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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?

Short Answer

Expert verified

The quark configuration of the\({\rm{D - }}\)meson particle is\({D^ + } = \left( {c\bar d} \right)\).

Step by step solution

01

Concept Introduction

Mesons are hadronic subatomic particles made up of an equal number of quarks and antiquarks, generally one of each, and linked together by strong interactions in particle physics.

A quark is a basic matter ingredient and an elementary particle.

Anti-quarks are the antiparticles that correspond to each flavour of quark.

02

Quantum numbers for \({{\rm{D}}^{\rm{ + }}}\)

Find the quark compositions for\({{\rm{D}}^{\rm{ + }}}\)given that all its quantum numbers as follows –

\({\rm{B}}\)

\({\rm{Q}}\)

\({\rm{S}}\)

\({\rm{t}}\)

\({\rm{b}}\)

\({\rm{c}}\)

\({{\rm{D}}^{\rm{ + }}}\)

\({\rm{0}}\)

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

\({\rm{0}}\)

\({\rm{0}}\)

\({\rm{0}}\)

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

03

Quark configuration for \({{\rm{D}}^{\rm{ + }}}\)

Now, find its quark configuration –

Since \({{\rm{D}}^{\rm{ + }}}\) is a meson. Thus, it consists of quark and anti-quark.

\({D^ + } = \left( {q\bar q} \right)\)

Since it has a charm of \(c = + 1\). Therefore, the quark is the charmed \({\rm{c}}\).

\({D^ + } = \left( {c\bar q} \right)\)

Since its charge is \({\rm{ + 1}}\) and the charge of the charm quark is \({\rm{ + 2/3}}\). Thus, an anti-quark with charge \({\rm{ + 1/3}}\) is needed. The options available are – \({\rm{\bar d,\bar s,}}\) and \({\rm{\mathord{\buildrel{\lower3pt\hbox{$\scriptscriptstyle\leftarrow$}} \over b} }}\).

Since its strangeness and bottomness are zero. Therefore,\({\rm{\bar s,}}\)and \({\rm{\mathord{\buildrel{\lower3pt\hbox{$\scriptscriptstyle\leftarrow$}} \over b} }}\) cannot be considered.

Hence, the quark configuration for the \({\rm{D}}\)-meson \({{\rm{D}}^{\rm{ + }}}\) is –

\({D^ + } = \left( {c\bar d} \right)\)

Therefore, the quark configuration is obtained as \({D^ + } = \left( {c\bar d} \right)\).

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Most popular questions from this chapter

(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.

Calculate the mass in \[{\rm{GeV/}}{{\rm{c}}^{\rm{2}}}\]of a virtual carrier particle that has a range limited to \[{\rm{1}}{{\rm{0}}^{{\rm{ - 30}}}}{\rm{\;m}}\]by the Heisenberg uncertainty principle. Such a particle might be involved in the unification of the strong and electroweak forces.

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\({{\rm{\pi }}^{\rm{ + }}}{\rm{ + p}} \to {{\rm{\Delta }}^{{\rm{ + + }}}} \to {{\rm{\pi }}^{\rm{ + }}}{\rm{ + p}}\), where the \({{\rm{\Delta }}^{{\rm{ + + }}}}\)is a very short-lived particle. The graph in Figure \({\rm{33}}{\rm{.26}}\)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\({{\rm{\Delta }}^{{\rm{ + + }}}}\).

(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 \({\rm{\bar d}}\)antiquark by writing the reaction and decay in terms of quarks.

(c) Draw a Feynman diagram of the production and decay of the \({{\rm{\Delta }}^{{\rm{ + + }}}}\)showing the individual quarks involved.

How can quarks, which are fermions, combine to form bosons? Why must an even number combine to form a boson? Give one example by stating the quark substructure of a boson.

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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