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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?

Short Answer

Expert verified

The quark"s theory confinement that explains why quarks will be exist but can not be observed and isolated.

Step by step solution

01

Definition of Concept

The interplay of physical forces, such as electromagnetism and maybe even gravity, is controlled by bosons, which are sometimes referred to as force particles.

02

Find two major limitations prevent us from building high-energy accelerators

The nuclear force that binds the proton and neutron is between 1 and 3 fm, whereas the force that binds quarks with is a proton, neutron, and hadron is less than 1fm. As a result, the gluon force between quarks is greater than the strong nuclear force between hadrons, despite the fact that the quark force of small value can hold the particles strongly as compared to the nuclear force. Additionally, gluons are made up of bosons, which carry both colour and anticolor quarks and bind the hadron while changing its colour. The colour force is what we call it. This phenomenon of colour energy is related to quark confinement because the colour characteristics of quark and anti-quark movement are involved in it.

Therefore, the confinement of the quark theory explains why quarks exist but cannot be observed or isolated.

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Most popular questions from this chapter

Why is it easier to see the properties of the c, b, and t quarks in mesons having composition Wโˆ’ or t rather than in baryons having a mixture of quarks, such as udb?

Suppose a \[{{\rm{W}}^{\rm{ - }}}\]created in a bubble chamber lives for \[{\rm{5}}{\rm{.00 \times 1}}{{\rm{0}}^{{\rm{ - 25}}}}{\rm{\;s}}\]. What distance does it move in this time if it is traveling at \[{\rm{0}}{\rm{.900c}}\]? Since this distance is too short to make a track, the presence of the \[{{\rm{W}}^{\rm{ - }}}\]must be inferred from its decay products. Note that the time is longer than the given \[{{\rm{W}}^{\rm{ - }}}\]lifetime, which can be due to the statistical nature of decay or time dilation.

The primary decay mode for the negative pion is \[{\pi ^ - } \to {\mu ^ - } + {\bar \nu _\mu }\]. What is the energy release in MeV in this decay?

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.

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(a) What would the relativistic quantity \(\gamma {\rm{ = }}\frac{{\rm{1}}}{{\sqrt {{\rm{1 - }}{{{{\rm{\nu }}^{\rm{2}}}} \mathord{\left/{\vphantom {{{{\rm{\nu }}^{\rm{2}}}} {{{\rm{c}}^{\rm{2}}}}}} \right. \\} {{{\rm{c}}^{\rm{2}}}}}} }}\) be for these particles?

(b) How long would their average lifetime be in the laboratory?

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