Quarks have been mentioned at various points in this text as fundamental building blocks and members of the exclusive club of truly elementary particles. Note that an elementary or fundamental particle has no substructure (it is not made of other particles) and has no finite size other than its wavelength. This does not mean that fundamental particles are stable—some decay, while others do not. Keep in mind that all leptons seem to be fundamental, whereasno hadrons are fundamental. There is strong evidence that quarks are the fundamental building blocks of hadrons as seen in [link]. Quarks are the second group of fundamental particles (leptons are the first). The third and perhaps final group of fundamental particles is the carrier particles for the four basic forces. Leptons, quarks, and carrier particles may be all there is. In this module we will discuss the quark substructure of hadrons and its relationship to forces as well as indicate some remaining questions and problems.
Conception of Quarks
Quarks were first proposed independently by American physicists Murray GellMann and George Zweig in 1963. Their quaint name was taken by GellMann from a James Joyce novel—GellMann was also largely responsible for the concept and name of strangeness. (Whimsical names are common in particle physics, reflecting the personalities of modern physicists.) Originally, three quark types—or flavors—were proposed to account for the thenknown mesons and baryons. These quark flavors are named up (u), down (d), and strange (s). All quarks have halfintegral spin and are thus fermions. All mesons have integral spin while all baryons have halfintegral spin. Therefore, mesons should be made up of an even number of quarks while baryons need to be made up of an odd number of quarks. [link] shows the quark substructure of the proton, neutron, and two pions. The most radical proposal by GellMann and Zweig is the fractional charges of quarks, which are $\pm \left(\frac{2}{3}\right){q}_{e}$ and $\left(\frac{1}{3}\right){q}_{e}$, whereas all directly observed particles have charges that are integral multiples of ${q}_{e}$. Note that the fractional value of the quark does not violate the fact that the e is the smallest unit of charge that is observed, because a free quark cannot exist. [link] lists characteristics of the six quark flavors that are now thought to exist. Discoveries made since 1963 have required extra quark flavors, which are divided into three families quite analogous to leptons.
How Does it Work?
To understand how these quark substructures work, let us specifically examine the proton, neutron, and the two pions pictured in [link] before moving on to more general considerations. First, the proton p is composed of the three quarks uud, so that its total charge is $+\left(\frac{2}{3}\right){q}_{e}+\left(\frac{2}{3}\right){q}_{e}\left(\frac{1}{3}\right){q}_{e}={q}_{e}$, as expected. With the spins aligned as in the figure, the proton’s intrinsic spin is $+\left(\frac{1}{2}\right)+\left(\frac{1}{2}\right)\left(\frac{1}{2}\right)=\left(\frac{1}{2}\right)$, also as expected. Note that the spins of the up quarks are aligned, so that they would be in the same state except that they have different colors (another quantum number to be elaborated upon a little later). Quarks obey the Pauli exclusion principle. Similar comments apply to the neutron n, which is composed of the three quarks udd. Note also that the neutron is made of charges that add to zero but move internally, producing its wellknown magnetic moment. When the neutron ${\beta}^{}$ decays, it does so by changing the flavor of one of its quarks. Writing neutron ${\beta}^{}$ decay in terms of quarks,
We see that this is equivalent to a down quark changing flavor to become an up quark:
Name  Symbol  Antiparticle  Spin  Charge 
$$B$$
$B$ is baryon number, S is strangeness, $c$ is charm, $b$ is bottomness, $t$ is topness.

$$S$$  $$c$$  $$b$$  $$t$$ 
Mass $(\text{GeV}/{c}^{2})$ Values are approximate, are not directly observable, and vary with model.

Up  $$u$$  $$\stackrel{}{u}$$  1/2  $$\pm \frac{2}{3}{q}_{e}$$  $$\pm \frac{1}{3}$$  0  0  0  0  0.005 
Down  $$d$$  $$\stackrel{}{d}$$  1/2  $$\mp \frac{1}{3}{q}_{e}$$  $$\pm \frac{1}{3}$$  0  0  0  0  0.008 
Strange  $$s$$  $$\stackrel{}{s}$$  1/2  $$\mp \frac{1}{3}{q}_{e}$$  $$\pm \frac{1}{3}$$  $$\mp 1$$  0  0  0  0.50 
Charmed  $$c$$  $$\stackrel{}{c}$$  1/2  $$\pm \frac{2}{3}{q}_{e}$$  $$\pm \frac{1}{3}$$  0  $$\pm 1$$  0  0  1.6 
Bottom  $$b$$  $$\stackrel{}{b}$$  1/2  $$\mp \frac{1}{3}{q}_{e}$$  $$\pm \frac{1}{3}$$  0  0  $$\mp 1$$  0  5 
Top  $$t$$  $$\stackrel{}{t}$$  1/2  $$\pm \frac{2}{3}{q}_{e}$$  $$\pm \frac{1}{3}$$  0  0  0  $$\pm 1$$  173 
Particle  Quark Composition 
Mesons  
$${\pi}^{+}$$  $$u\stackrel{}{d}$$ 
$${\pi}^{}$$  $$\stackrel{}{u}d$$ 
$${\pi}^{0}$$  $$u\stackrel{}{u}$$, $$d\stackrel{}{d}$$ mixture These two mesons are different mixtures, but each is its own antiparticle, as indicated by its quark composition. 
$${\eta}^{0}$$  $$u\stackrel{}{u}$$, $$d\stackrel{}{d}$$ mixture These two mesons are different mixtures, but each is its own antiparticle, as indicated by its quark composition. 
$${K}^{0}$$  $$d\stackrel{}{s}$$ 
$${\stackrel{}{K}}^{0}$$  $$\stackrel{}{d}s$$ 
$${K}^{+}$$  $$u\stackrel{}{s}$$ 
$${K}^{}$$  $$\stackrel{}{u}s$$ 
$$J/\psi $$  $$c\stackrel{}{c}$$ 
$\Upsilon $  $$b\stackrel{}{b}$$ 
Baryons Antibaryons have the antiquarks of their counterparts. The antiproton $\stackrel{}{p}$ is $\stackrel{}{u}\stackrel{}{u}\stackrel{}{d}$, for example. ,Baryons composed of the same quarks are different states of the same particle. For example, the ${\text{\Delta}}^{+}$ is an excited state of the proton.


$$p$$  $$\text{uud}$$ 
$$n$$  $$\text{udd}$$ 
$${\text{\Delta}}^{0}$$  $$\text{udd}$$ 
$${\text{\Delta}}^{+}$$  $$\text{uud}$$ 
$${\text{\Delta}}^{}$$  $$\text{ddd}$$ 
$${\text{\Delta}}^{\text{++}}$$  $$\text{uuu}$$ 
$${\text{\Lambda}}^{0}$$  $$\text{uds}$$ 
$${\text{\Sigma}}^{0}$$  $$\text{uds}$$ 
$${\text{\Sigma}}^{+}$$  $$\text{uus}$$ 
$${\text{\Sigma}}^{}$$  $$\text{dds}$$ 
$${\text{\Xi}}^{0}$$  $$\text{uss}$$ 
$${\text{\Xi}}^{}$$  $$\text{dss}$$ 
$${\Omega}^{}$$  $$\text{sss}$$ 
This is an example of the general fact that the weak nuclear force can change the flavor of a quark. By general, we mean that any quark can be converted to any other (change flavor) by the weak nuclear force. Not only can we get $d\to u$, we can also get $u\to d$. Furthermore, the strange quark can be changed by the weak force, too, making $s\to u$ and $s\to d$ possible. This explains the violation of the conservation of strangeness by the weak force noted in the preceding section. Another general fact is that the strong nuclear force cannot change the flavor of a quark.
Again, from [link], we see that the ${\pi}^{+}$ meson (one of the three pions) is composed of an up quark plus an antidown quark, or $u\stackrel{}{d}$. Its total charge is thus $+\left(\frac{2}{3}\right){q}_{e}+\left(\frac{1}{3}\right){q}_{e}={q}_{e}$, as expected. Its baryon number is 0, since it has a quark and an antiquark with baryon numbers $+\left(\frac{1}{3}\right)\left(\frac{1}{3}\right)=0$. The ${\pi}^{+}$ halflife is relatively long since, although it is composed of matter and antimatter, the quarks are different flavors and the weak force should cause the decay by changing the flavor of one into that of the other. The spins of the $u$ and $\stackrel{}{d}$ quarks are antiparallel, enabling the pion to have spin zero, as observed experimentally. Finally, the ${\pi}^{}$ meson shown in [link] is the antiparticle of the ${\pi}^{+}$ meson, and it is composed of the corresponding quark antiparticles. That is, the ${\pi}^{+}$ meson is $u\stackrel{}{d}$, while the ${\pi}^{}$ meson is $\stackrel{}{u}d$. These two pions annihilate each other quickly, because their constituent quarks are each other’s antiparticles.
Two general rules for combining quarks to form hadrons are:
 Baryons are composed of three quarks, and antibaryons are composed of three antiquarks.
 Mesons are combinations of a quark and an antiquark.
One of the clever things about this scheme is that only integral charges result, even though the quarks have fractional charge.
All Combinations are Possible
All quark combinations are possible. [link] lists some of these combinations. When GellMann and Zweig proposed the original three quark flavors, particles corresponding to all combinations of those three had not been observed. The pattern was there, but it was incomplete—much as had been the case in the periodic table of the elements and the chart of nuclides. The ${\Omega}^{}$ particle, in particular, had not been discovered but was predicted by quark theory. Its combination of three strange quarks, $\text{sss}$, gives it a strangeness of $3$ (see [link]) and other predictable characteristics, such as spin, charge, approximate mass, and lifetime. If the quark picture is complete, the ${\Omega}^{}$ should exist. It was first observed in 1964 at Brookhaven National Laboratory and had the predicted characteristics as seen in [link]. The discovery of the ${\Omega}^{}$ was convincing indirect evidence for the existence of the three original quark flavors and boosted theoretical and experimental efforts to further explore particle physics in terms of quarks.
Verify the quantum numbers given for the ${\text{\Xi}}^{0}$ particle in [link] by adding the quantum numbers for its quark composition as given in [link].
Strategy
The composition of the ${\text{\Xi}}^{0}$ is given as $\text{uss}$ in [link]. The quantum numbers for the constituent quarks are given in [link]. We will not consider spin, because that is not given for the ${\text{\Xi}}^{0}$. But we can check on charge and the other quantum numbers given for the quarks.
Solution
The total charge of uss is $+\left(\frac{2}{3}\right){q}_{e}\left(\frac{1}{3}\right){q}_{e}\left(\frac{1}{3}\right){q}_{e}=0$, which is correct for the ${\text{\Xi}}^{0}$. The baryon number is $+\left(\frac{1}{3}\right)+\left(\frac{1}{3}\right)+\left(\frac{1}{3}\right)=1$, also correct since the ${\text{\Xi}}^{0}$ is a matter baryon and has $B=1$, as listed in [link]. Its strangeness is $S=011=2$, also as expected from [link]. Its charm, bottomness, and topness are 0, as are its lepton family numbers (it is not a lepton).
Discussion
This procedure is similar to what the inventors of the quark hypothesis did when checking to see if their solution to the puzzle of particle patterns was correct. They also checked to see if all combinations were known, thereby predicting the previously unobserved ${\Omega}^{}$ as the completion of a pattern.
Now, Let Us Talk About Direct Evidence
At first, physicists expected that, with sufficient energy, we should be able to free quarks and observe them directly. This has not proved possible. There is still no direct observation of a fractional charge or any isolated quark. When large energies are put into collisions, other particles are created—but no quarks emerge. There is nearly direct evidence for quarks that is quite compelling. By 1967, experiments at SLAC scattering 20GeV electrons from protons had produced results like Rutherford had obtained for the nucleus nearly 60 years earlier. The SLAC scattering experiments showed unambiguously that there were three pointlike (meaning they had sizes considerably smaller than the probe’s wavelength) charges inside the proton as seen in [link]. This evidence made all but the most skeptical admit that there was validity to the quark substructure of hadrons.
More recent and higherenergy experiments have produced jets of particles in collisions, highly suggestive of three quarks in a nucleon. Since the quarks are very tightly bound, energy put into separating them pulls them only so far apart before it starts being converted into other particles. More energy produces more particles, not a separation of quarks. Conservation of momentum requires that the particles come out in jets along the three paths in which the quarks were being pulled. Note that there are only three jets, and that other characteristics of the particles are consistent with the threequark substructure.
Quarks Have Their Ups and Downs
The quark model actually lost some of its early popularity because the original model with three quarks had to be modified. The up and down quarks seemed to compose normal matter as seen in [link], while the single strange quark explained strangeness. Why didn’t it have a counterpart? A fourth quark flavor called charm (c) was proposed as the counterpart of the strange quark to make things symmetric—there would be two normal quarks (u and d) and two exotic quarks (s and c). Furthermore, at that time only four leptons were known, two normal and two exotic. It was attractive that there would be four quarks and four leptons. The problem was that no known particles contained a charmed quark. Suddenly, in November of 1974, two groups (one headed by C. C. Ting at Brookhaven National Laboratory and the other by Burton Richter at SLAC) independently and nearly simultaneously discovered a new meson with characteristics that made it clear that its substructure is $c\stackrel{}{c}$. It was called J by one group and psi ($\psi $) by the other and now is known as the $J/\psi $ meson. Since then, numerous particles have been discovered containing the charmed quark, consistent in every way with the quark model. The discovery of the $J/\psi $ meson had such a rejuvenating effect on quark theory that it is now called the November Revolution. Ting and Richter shared the 1976 Nobel Prize.
History quickly repeated itself. In 1975, the tau ($\tau $) was discovered, and a third family of leptons emerged as seen in [link]). Theorists quickly proposed two more quark flavors called top (t) or truth and bottom (b) or beauty to keep the number of quarks the same as the number of leptons. And in 1976, the upsilon ($\Upsilon $) meson was discovered and shown to be composed of a bottom and an antibottom quark or $b\stackrel{}{b}$, quite analogous to the $J/\psi $ being $c\stackrel{}{c}$ as seen in [link]. Being a single flavor, these mesons are sometimes called bare charm and bare bottom and reveal the characteristics of their quarks most clearly. Other mesons containing bottom quarks have since been observed. In 1995, two groups at Fermilab confirmed the top quark’s existence, completing the picture of six quarks listed in [link]. Each successive quark discovery—first $c$, then $b$, and finally $t$ —has required higher energy because each has higher mass. Quark masses in [link] are only approximately known, because they are not directly observed. They must be inferred from the masses of the particles they combine to form.
What’s Color got to do with it?—A Whiter Shade of Pale
As mentioned and shown in [link], quarks carry another quantum number, which we call color. Of course, it is not the color we sense with visible light, but its properties are analogous to those of three primary and three secondary colors. Specifically, a quark can have one of three color values we call red ($R$), green ($G$), and blue ($B$) in analogy to those primary visible colors. Antiquarks have three values we call antired or cyan$\left(\stackrel{}{R}\right)$, antigreen or magenta$\left(\stackrel{}{G}\right)$, and antiblue or yellow$\left(\stackrel{}{B}\right)$ in analogy to those secondary visible colors. The reason for these names is that when certain visual colors are combined, the eye sees white. The analogy of the colors combining to white is used to explain why baryons are made of three quarks, why mesons are a quark and an antiquark, and why we cannot isolate a single quark. The force between the quarks is such that their combined colors produce white. This is illustrated in [link]. A baryon must have one of each primary color or RGB, which produces white. A meson must have a primary color and its anticolor, also producing white.
Why must hadrons be white? The color scheme is intentionally devised to explain why baryons have three quarks and mesons have a quark and an antiquark. Quark color is thought to be similar to charge, but with more values. An ion, by analogy, exerts much stronger forces than a neutral molecule. When the color of a combination of quarks is white, it is like a neutral atom. The forces a white particle exerts are like the polarization forces in molecules, but in hadrons these leftovers are the strong nuclear force. When a combination of quarks has color other than white, it exerts extremely large forces—even larger than the strong force—and perhaps cannot be stable or permanently separated. This is part of the theory of quark confinement, which explains how quarks can exist and yet never be isolated or directly observed. Finally, an extra quantum number with three values (like those we assign to color) is necessary for quarks to obey the Pauli exclusion principle. Particles such as the ${\Omega}^{}$, which is composed of three strange quarks, $\text{sss}$, and the ${\text{\Delta}}^{\text{++}}$, which is three up quarks, uuu, can exist because the quarks have different colors and do not have the same quantum numbers. Color is consistent with all observations and is now widely accepted. Quark theory including color is called quantum chromodynamics (QCD), also named by GellMann.
The Three Families
Fundamental particles are thought to be one of three types—leptons, quarks, or carrier particles. Each of those three types is further divided into three analogous families as illustrated in [link]. We have examined leptons and quarks in some detail. Each has six members (and their six antiparticles) divided into three analogous families. The first family is normal matter, of which most things are composed. The second is exotic, and the third more exotic and more massive than the second. The only stable particles are in the first family, which also has unstable members.
Always searching for symmetry and similarity, physicists have also divided the carrier particles into three families, omitting the graviton. Gravity is special among the four forces in that it affects the space and time in which the other forces exist and is proving most difficult to include in a Theory of Everything or TOE (to stub the pretension of such a theory). Gravity is thus often set apart. It is not certain that there is meaning in the groupings shown in [link], but the analogies are tempting. In the past, we have been able to make significant advances by looking for analogies and patterns, and this is an example of one under current scrutiny. There are connections between the families of leptons, in that the $\tau $ decays into the $\mu $ and the $\mu $ into the e. Similarly for quarks, the higher families eventually decay into the lowest, leaving only u and d quarks. We have long sought connections between the forces in nature. Since these are carried by particles, we will explore connections between gluons, ${W}^{\pm}$ and ${Z}^{0}$, and photons as part of the search for unification of forces discussed in GUTs: The Unification of Forces..
Summary
 Hadrons are thought to be composed of quarks, with baryons having three quarks and mesons having a quark and an antiquark.
 The characteristics of the six quarks and their antiquark counterparts are given in [link], and the quark compositions of certain hadrons are given in [link].
 Indirect evidence for quarks is very strong, explaining all known hadrons and their quantum numbers, such as strangeness, charm, topness, and bottomness.
 Quarks come in six flavors and three colors and occur only in combinations that produce white.
 Fundamental particles have no further substructure, not even a size beyond their de Broglie wavelength.
 There are three types of fundamental particles—leptons, quarks, and carrier particles. Each type is divided into three analogous families as indicated in [link].
Conceptual Questions
The quark flavor change $d\to u$ takes place in ${\beta}^{}$ decay. Does this mean that the reverse quark flavor change $u\to d$ takes place in ${\beta}^{+}$ decay? Justify your response by writing the decay in terms of the quark constituents, noting that it looks as if a proton is converted into a neutron in ${\beta}^{+}$ decay.
Explain how the weak force can change strangeness by changing quark flavor.
Beta decay is caused by the weak force, as are all reactions in which strangeness changes. Does this imply that the weak force can change quark flavor? Explain.
Why is it easier to see the properties of the c, b, and t quarks in mesons having composition ${W}^{}$ or $t\stackrel{}{t}$ rather than in baryons having a mixture of quarks, such as udb?
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.
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?
Discuss how we know that $\pi \text{mesons}$ (${\pi}^{+},\pi ,{\pi}^{0}$) are not fundamental particles and are not the basic carriers of the strong force.
An antibaryon has three antiquarks with colors $\stackrel{}{R}\stackrel{}{G}\stackrel{}{B}$. What is its color?
Suppose leptons are created in a reaction. Does this imply the weak force is acting? (for example, consider $\beta $ decay.)
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?
(a) Do all particles having strangeness also have at least one strange quark in them?
(b) Do all hadrons with a strange quark also have nonzero strangeness?
The sigmazero particle decays mostly via the reaction ${\text{\Sigma}}^{0}\to {\text{\Lambda}}^{0}+\gamma $. Explain how this decay and the respective quark compositions imply that the ${\text{\Sigma}}^{0}$ is an excited state of the ${\text{\Lambda}}^{0}$.
What do the quark compositions and other quantum numbers imply about the relationships between the ${\text{\Delta}}^{+}$ and the proton? The ${\text{\Delta}}^{0}$ and the neutron?
Discuss the similarities and differences between the photon and the ${Z}^{0}$ in terms of particle properties, including forces felt.
Identify evidence for electroweak unification.
The quarks in a particle are confined, meaning individual quarks cannot be directly observed. Are gluons confined as well? Explain
Problems & Exercises
(a) Verify from its quark composition that the ${\text{\Delta}}^{+}$ particle could be an excited state of the proton.
(b) There is a spread of about 100 MeV in the decay energy of the ${\text{\Delta}}^{+}$, 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) The $\text{uud}$ composition is the same as for a proton.
(b) $3\text{.}3\times {\text{10}}^{\text{24}}\phantom{\rule{0.25em}{0ex}}\text{s}$
(c) Strong (short lifetime)
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 ${\pi}^{+}+p\to {\text{\Delta}}^{\text{++}}\to {\pi}^{+}+p$, where the ${\text{\Delta}}^{\text{++}}$ is a very shortlived particle. The graph in [link] 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 ${\text{\Delta}}^{\text{++}}$.
(a) Find this lifetime.
(b) Verify from the quark composition of the particles that this reaction annihilates and then recreates a d quark and a $\stackrel{}{d}$ antiquark by writing the reaction and decay in terms of quarks.
(c) Draw a Feynman diagram of the production and decay of the ${\text{\Delta}}^{\text{++}}$ showing the individual quarks involved.
The reaction ${\pi}^{+}+p\to {\text{\Delta}}^{\text{++}}$ (described in the preceding problem) takes place via the strong force. (a) What is the baryon number of the ${\text{\Delta}}^{\text{++}}$ particle?
(b) Draw a Feynman diagram of the reaction showing the individual quarks involved.
a) ${\text{\Delta}}^{\text{++}}(\text{uuu});\phantom{\rule{0.25em}{0ex}}B=\frac{1}{3}+\frac{1}{3}+\frac{1}{3}=1$
b)
One of the decay modes of the omega minus is ${\Omega}^{}\to {\text{\Xi}}^{0}+{\pi}^{}$.
(a) What is the change in strangeness?
(b) Verify that baryon number and charge are conserved, while lepton numbers are unaffected.
(c) Write the equation in terms of the constituent quarks, indicating that the weak force is responsible.
Repeat the previous problem for the decay mode ${\Omega}^{}\to {\text{\Lambda}}^{0}+{K}^{}.$
(a) $+1$
(b) $B=1=1+\mathrm{0,}Z==0+(1)$, all lepton numbers are 0 before and after
(c) $(\text{sss})\to (\text{uds})+\left(\stackrel{}{u}s\right)$
One decay mode for the etazero meson is ${\eta}^{0}\to \gamma +\mathrm{\gamma .}$
(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.
(d) Verify that baryon number, lepton numbers, and charge are conserved.
One decay mode for the etazero meson is ${\eta}^{0}\to {\pi}^{0}+{\pi}^{0}$.
(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 ${\pi}^{0}\to \gamma +\gamma $?
(a) $(u\stackrel{}{u}+d\overline{d})\to (u\stackrel{}{u}+d\overline{d})+(u\stackrel{}{u}+d\overline{d})$
(b) 277.9 MeV
(c) 547.9 MeV
Is the decay $n\to {e}^{+}+{e}^{}$ possible considering the appropriate conservation laws? State why or why not.
Is the decay ${\mu}^{}\to {e}^{}+{\nu}_{e}+{\nu}_{\mu}$ possible considering the appropriate conservation laws? State why or why not.
No. $\text{Charge}=1$ is conserved. ${L}_{{e}_{\text{i}}}=0\ne {L}_{{e}_{\text{f}}}=2$ is not conserved. ${L}_{\mu}=1$ is conserved.
(a) Is the decay ${\text{\Lambda}}^{0}\to n+{\pi}^{0}$ possible considering the appropriate conservation laws? State why or why not.
(b) Write the decay in terms of the quark constituents of the particles.
(a) Is the decay ${\text{\Sigma}}^{}\to n+{\pi}^{}$ possible considering the appropriate conservation laws? State why or why not. (b) Write the decay in terms of the quark constituents of the particles.
(a)Yes. $Z=1=0+(1)$, $B=1=1+0$, all lepton family numbers are 0 before and after, spontaneous since mass greater before reaction.
(b) $\text{dds}\to \text{udd}+\stackrel{}{u}d$
The only combination of quark colors that produces a white baryon is RGB. Identify all the color combinations that can produce a white meson.
(a) Three quarks form a baryon. How many combinations of the six known quarks are there if all combinations are possible?
(b) This number is less than the number of known baryons. Explain why.
(a) 216
(b) There are more baryons observed because we have the 6 antiquarks and various mixtures of quarks (as for the πmeson) as well.
(a) Show that the conjectured decay of the proton, $p\to {\pi}^{0}+{e}^{+}$, violates conservation of baryon number and conservation of lepton number.
(b) What is the analogous decay process for the antiproton?
Verify the quantum numbers given for the ${\Omega}^{+}$ in [link] by adding the quantum numbers for its quark constituents as inferred from [link].
$\begin{array}{l}{\Omega}^{+}(\stackrel{}{s}\stackrel{}{s}\stackrel{}{s})\\ B=\frac{1}{3}\frac{1}{3}\frac{1}{3}=\mathrm{1,}\\ {L}_{e},\phantom{\rule{0.25em}{0ex}}\mu ,\phantom{\rule{0.25em}{0ex}}\tau =0+0+0=\mathrm{0,}\\ Q=\frac{1}{3}+\frac{1}{3}+\frac{1}{3}=\mathrm{1,}\\ S=1+1+1=3\text{.}\end{array}$
(a) How much energy would be released if the proton did decay via the conjectured reaction $p\to {\pi}^{0}+{e}^{+}$?
(b) Given that the ${\pi}^{0}$ decays to two $\gamma $ s and that the ${e}^{+}$ 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)803 MeV
(b) 938.8 MeV
(c) The annihilation energy of an extra electron is included in the total energy.
(a) Find the charge, baryon number, strangeness, charm, and bottomness of the $J/\Psi $ particle from its quark composition.
(b) Do the same for the $\Upsilon $ particle.
There are particles called Dmesons. One of them is the ${D}^{+}$ 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 $+1.$ What is its quark configuration?
$c\overline{d}$
There are particles called bottom mesons or Bmesons. One of them is the ${B}^{}$ meson, which has a single negative charge; its baryon number is zero, as are its strangeness, charm, and topness. It has a bottomness of $1$. What is its quark configuration?
(a) What particle has the quark composition $\stackrel{}{u}\stackrel{}{u}\stackrel{}{d}$?
(b) What should its decay mode be?
a)The antiproton
b) $\stackrel{}{p}\to {\pi}^{0}+{e}^{}$
(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.
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 College Physics
 Preface
 Introduction: The Nature of Science and Physics
 Kinematics
 Introduction to OneDimensional Kinematics
 Displacement
 Vectors, Scalars, and Coordinate Systems
 Time, Velocity, and Speed
 Acceleration
 Motion Equations for Constant Acceleration in One Dimension
 ProblemSolving Basics for OneDimensional Kinematics
 Falling Objects
 Graphical Analysis of OneDimensional Motion
 TwoDimensional Kinematics
 Dynamics: Force and Newton's Laws of Motion
 Introduction to Dynamics: Newton’s Laws of Motion
 Development of Force Concept
 Newton’s First Law of Motion: Inertia
 Newton’s Second Law of Motion: Concept of a System
 Newton’s Third Law of Motion: Symmetry in Forces
 Normal, Tension, and Other Examples of Forces
 ProblemSolving Strategies
 Further Applications of Newton’s Laws of Motion
 Extended Topic: The Four Basic Forces—An Introduction
 Further Applications of Newton's Laws: Friction, Drag, and Elasticity
 Uniform Circular Motion and Gravitation
 Work, Energy, and Energy Resources
 Linear Momentum and Collisions
 Statics and Torque
 Rotational Motion and Angular Momentum
 Introduction to Rotational Motion and Angular Momentum
 Angular Acceleration
 Kinematics of Rotational Motion
 Dynamics of Rotational Motion: Rotational Inertia
 Rotational Kinetic Energy: Work and Energy Revisited
 Angular Momentum and Its Conservation
 Collisions of Extended Bodies in Two Dimensions
 Gyroscopic Effects: Vector Aspects of Angular Momentum
 Fluid Statics
 Fluid Dynamics and Its Biological and Medical Applications
 Introduction to Fluid Dynamics and Its Biological and Medical Applications
 Flow Rate and Its Relation to Velocity
 Bernoulli’s Equation
 The Most General Applications of Bernoulli’s Equation
 Viscosity and Laminar Flow; Poiseuille’s Law
 The Onset of Turbulence
 Motion of an Object in a Viscous Fluid
 Molecular Transport Phenomena: Diffusion, Osmosis, and Related Processes
 Temperature, Kinetic Theory, and the Gas Laws
 Heat and Heat Transfer Methods
 Thermodynamics
 Introduction to Thermodynamics
 The First Law of Thermodynamics
 The First Law of Thermodynamics and Some Simple Processes
 Introduction to the Second Law of Thermodynamics: Heat Engines and Their Efficiency
 Carnot’s Perfect Heat Engine: The Second Law of Thermodynamics Restated
 Applications of Thermodynamics: Heat Pumps and Refrigerators
 Entropy and the Second Law of Thermodynamics: Disorder and the Unavailability of Energy
 Statistical Interpretation of Entropy and the Second Law of Thermodynamics: The Underlying Explanation
 Oscillatory Motion and Waves
 Introduction to Oscillatory Motion and Waves
 Hooke’s Law: Stress and Strain Revisited
 Period and Frequency in Oscillations
 Simple Harmonic Motion: A Special Periodic Motion
 The Simple Pendulum
 Energy and the Simple Harmonic Oscillator
 Uniform Circular Motion and Simple Harmonic Motion
 Damped Harmonic Motion
 Forced Oscillations and Resonance
 Waves
 Superposition and Interference
 Energy in Waves: Intensity
 Physics of Hearing
 Electric Charge and Electric Field
 Introduction to Electric Charge and Electric Field
 Static Electricity and Charge: Conservation of Charge
 Conductors and Insulators
 Coulomb’s Law
 Electric Field: Concept of a Field Revisited
 Electric Field Lines: Multiple Charges
 Electric Forces in Biology
 Conductors and Electric Fields in Static Equilibrium
 Applications of Electrostatics
 Electric Potential and Electric Field
 Electric Current, Resistance, and Ohm's Law
 Circuits, Bioelectricity, and DC Instruments
 Magnetism
 Introduction to Magnetism
 Magnets
 Ferromagnets and Electromagnets
 Magnetic Fields and Magnetic Field Lines
 Magnetic Field Strength: Force on a Moving Charge in a Magnetic Field
 Force on a Moving Charge in a Magnetic Field: Examples and Applications
 The Hall Effect
 Magnetic Force on a CurrentCarrying Conductor
 Torque on a Current Loop: Motors and Meters
 Magnetic Fields Produced by Currents: Ampere’s Law
 Magnetic Force between Two Parallel Conductors
 More Applications of Magnetism
 Electromagnetic Induction, AC Circuits, and Electrical Technologies
 Introduction to Electromagnetic Induction, AC Circuits and Electrical Technologies
 Induced Emf and Magnetic Flux
 Faraday’s Law of Induction: Lenz’s Law
 Motional Emf
 Eddy Currents and Magnetic Damping
 Electric Generators
 Back Emf
 Transformers
 Electrical Safety: Systems and Devices
 Inductance
 RL Circuits
 Reactance, Inductive and Capacitive
 RLC Series AC Circuits
 Electromagnetic Waves
 Geometric Optics
 Vision and Optical Instruments
 Wave Optics
 Introduction to Wave Optics
 The Wave Aspect of Light: Interference
 Huygens's Principle: Diffraction
 Young’s Double Slit Experiment
 Multiple Slit Diffraction
 Single Slit Diffraction
 Limits of Resolution: The Rayleigh Criterion
 Thin Film Interference
 Polarization
 *Extended Topic* Microscopy Enhanced by the Wave Characteristics of Light
 Special Relativity
 Introduction to Quantum Physics
 Atomic Physics
 Introduction to Atomic Physics
 Discovery of the Atom
 Discovery of the Parts of the Atom: Electrons and Nuclei
 Bohr’s Theory of the Hydrogen Atom
 X Rays: Atomic Origins and Applications
 Applications of Atomic Excitations and DeExcitations
 The Wave Nature of Matter Causes Quantization
 Patterns in Spectra Reveal More Quantization
 Quantum Numbers and Rules
 The Pauli Exclusion Principle
 Radioactivity and Nuclear Physics
 Medical Applications of Nuclear Physics
 Particle Physics
 Frontiers of Physics
 Atomic Masses
 Selected Radioactive Isotopes
 Useful Information
 Glossary of Key Symbols and Notation