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Determine the electric charge, baryon number, strangeness quantum number, and charm quantum number for the following quark combinations: (a) uus, (b) \(c \bar{s},\) (c) \(\overline{d d} \bar{u},\) and \((\) d) \(\bar{c} b\).

Short Answer

Expert verified
The properties for the given quark combinations are: uus - charge +1, baryon number 1, strangeness -1, charm 0; \(c \overline{s}\) - charge +1, baryon number 0, strangeness +1, charm +1; \(\overline{d} \overline{d} \overline{u}\) - charge -1, baryon number -1, strangeness 0, charm 0; \(d \overline{c} b\) - charge 0, baryon number 1/3, strangeness 0, charm +1

Step by step solution

01

Identify the quark values

First identify the types and properties of the quarks in each combination. Use these quark properties: up quark (u) - charge +2/3, baryon number 1/3, strangeness 0, charm 0; down quark (d) - charge -1/3, baryon number 1/3, strangeness 0, charm 0; strange quark (s) - charge -1/3, baryon number 1/3, strangeness -1, charm 0; charm quark (c) - charge +2/3, baryon number 1/3, strangeness 0, charm +1; bottom quark (b) - charge -1/3, baryon number 1/3, strangeness 0, charm 0; anti-quarks, denoted by the over-line, have opposite values to their corresponding quarks
02

Calculate properties for uus

For uus, add the properties: charge = +2/3 + 2/3 -1/3 = +1, baryon number = 1/3 + 1/3 + 1/3 = 1, strangeness = 0 + 0 -1 = -1, charm = 0
03

Calculate properties for \(c \overline{s}\)

For \(c \overline{s}\), add the properties: charge = +2/3 -(-1/3) = +1, baryon number = 1/3 -1/3 = 0, strangeness = 0 -(-1) = +1, charm = +1 -0 = +1
04

Calculate properties for \(\overline{d} \overline{d} \overline{u}\)

For \(\overline{d} \overline{d} \overline{u}\), add the properties: charge = -(-1/3) -(-1/3) -(+2/3) = -1, baryon number = -1/3 -1/3 -1/3 = -1, strangeness = 0, charm = 0
05

Calculate properties for \(d \overline{c} b\)

For \(d \overline{c} b\), add the properties: charge = -1/3 -(-2/3) -1/3 = 0, baryon number = 1/3 -1/3 + 1/3 = 1/3, strangeness = 0, charm = 0 -(-1) + 0 = +1

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Electric Charge of Quarks
Quarks are fundamental particles that combine to form composite particles such as protons and neutrons, which are the components of atomic nuclei.
Each type of quark has a specific electric charge, which is a crucial property influencing how quarks combine and interact with each other through the electromagnetic force.

The up (u), charm (c), and top (not mentioned here) quarks carry an electric charge of +2/3, while the down (d), strange (s), and bottom (b) quarks have a charge of -1/3. It's important to note that their corresponding anti-quarks carry the opposite charge.

To determine the total electric charge of a quark combination, such as in the given example of uus or \(c \overline{s},\) one simply needs to add up the charge of each individual quark. The properties of the anti-quarks must reflect their opposite charge, and therefore, they contribute a negative value to the total charge when calculating combinations that include them.
Baryon Number
The baryon number is a quantum number representing the number of baryons in a system. Baryons are particles composed of three quarks, like protons and neutrons.

Quarks are assigned a baryon number of +1/3, while anti-quarks have a baryon number of -1/3. The baryon number is conserved in most reactions, meaning the sum of baryon numbers before and after a reaction is the same. When quarks combine to form a particle, the sum of their baryon numbers gives the baryon number of that particle.

In the calculation of baryon numbers for different quark combinations, one must consider both quarks and anti-quarks. For example, in a quark combination like \(c \overline{s},\) the baryon number cancels out to zero since the baryon number from the charm quark is negated by the anti-strange quark, indicating that the combination is not a baryon but a meson.
Strangeness Quantum Number
The strangeness quantum number is associated with the presence of strange quarks within a particle, reflecting a property conserved under the strong nuclear force but not the weak force.

A strange quark has a strangeness of -1, mainly due to its heavier mass compared to the up and down quarks. When calculating the strangeness of a quark combination, it is essential to pay attention to whether the strange quark is a particle or an anti-particle, as this will affect the sign of the strangeness number.

For the given combination \(c \overline{s},\) the strangeness would be +1, which is the negative of the strangeness quantum number for a strange quark, because we are dealing with an anti-strange quark. Therefore, the presence of an anti-strange quark will increase the total strangeness quantum number of the particle.
Charm Quantum Number
Charm is another quantum number associated with the presence of charm quarks in a particle. The charm quark, being one of the heavier quarks, carries a charm quantum number of +1.

Just like other quantum numbers, the charm quantum number helps in identifying and classifying particles. It is important to note that anti-charm quarks have a charm number of -1.

In the practice of calculating for quark combinations, when an anti-charm quark is present, its contribution will be subtracted from the total charm quantum number. As an example, in the quark combination \(d \overline{c} b\), the anti-charm reverses its charm value, resulting in a positive charm quantum number when summed with the other quarks that have a charm number of zero. This concept is integral to understanding the composition and characteristics of hadrons, which are particles made up of quarks.

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Most popular questions from this chapter

In which of the following decays are the three lepton numbers conserved? In each case, explain your reasoning. (a) \(\mu^{-} \rightarrow \mathrm{e}^{-}+v_{e}+\bar{v}_{\mu}\) (b) \(\tau^{-} \rightarrow \mathrm{e}^{-}+\bar{\nu}_{e}+\nu_{\tau}\) (c) \(\pi^{+} \rightarrow \mathrm{e}^{+}+\gamma_{i}\) (d) \(\mathrm{n} \rightarrow \mathrm{p}+\mathrm{e}^{-}+\bar{\nu}_{e}\)

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