Year 12 PhysicsModule 8⏱ ~20 min5 MC · 2 Short AnswerLesson 15 of 17
Quarks and the Standard Model
You'll be able to determine quark content.
On 11 November 1974, Samuel Ting at Brookhaven National Laboratory and Burton Richter at SLAC simultaneously announced the discovery of the J/ψ meson, a particle with mass 3.097 GeV/c² composed of a charm–anticharm quark pair. This "November Revolution" confirmed Murray Gell-Mann's 1964 quark model and the predicted fourth (charm) quark. Ting and Richter shared the Nobel Prize in Physics in 1976. The Higgs boson, the final particle in the Standard Model, was confirmed at CERN on 4 July 2012 from a dataset of 5 × 10¹⁵ proton collisions.
Today's hook: On 11 November 1974, two independent teams, Samuel Ting at Brookhaven and Burton Richter at SLAC, simultaneously announced the discovery of a new particle, the J/ψ meson, at exactly 3.097 GeV/c². The particle was composed of a charm–anticharm quark pair, confirming Murray Gell-Mann's 1964 quark model. The Nobel Prize followed in 1976. Yet no experiment has ever detected a single free quark, try to pull two quarks apart and the energy you supply just creates new quark pairs instead. Why can quarks never be isolated?
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1
You're here
Orient and predict
Set up the vocabulary for quarks, colour charge and confinement, then predict why a free quark has never been seen.
Warm up first
Three quick questions from earlier lessons. Pulling old material back to mind before you learn something new makes the new material stick better, so this is not busywork.
Worksheets
Practise this lesson
Four printable worksheets that build from the foundations up to exam-style questions, start at whatever level suits you.
Before quarks were discovered, physicists knew protons and neutrons were not fundamental because they participated in many different particle reactions.
Before reading on, answer:
What evidence suggested protons and neutrons had internal structure?
Why do we never observe isolated quarks in nature?
How many different quarks are needed to explain all known hadrons?
Warm-up: A proton has charge $+1$. Its quark composition $uud$ gives charge:
Learning Intentions
goals
Know, Quark Properties
Six flavours: u, d, s, c, b, t
Charges: $+2/3e$ or $-1/3e$
Colour charge and confinement
Understand, Standard Model
Fermions: quarks and leptons
Bosons: force carriers
Higgs boson and mass
Can Do, Particle Analysis
Determine quark content
Verify conservation laws
Predict interaction outcomes
Scan these before reading
vocab
QuarkFundamental spin-$\frac{1}{2}$ fermion with fractional charge; six flavours exist in three generations.
ConfinementQuarks are never observed in isolation; they exist only in colour-neutral combinations (hadrons).
Colour chargeProperty of quarks analogous to electric charge; three colours: red, green, blue. Hadrons must be colour-neutral.
GluonMassless spin-1 boson that mediates the strong force between quarks; carries colour charge itself.
Higgs bosonSpin-0 particle discovered 2012 at CERN; gives mass to $W$, $Z$ bosons and fermions via the Higgs mechanism.
Cross-lesson links: L16 introduced antimatter. L17 builds the full Standard Model, 6 quarks, 6 leptons, 4 force carrier bosons. The Standard Model predicts every particle interaction in L18 and L19; understanding which particles are fundamental and which are composite is the conceptual organiser for all of particle physics.
Core Content
2
Read the quark table
Learn the six flavours and their fractional charges, then use colour charge to explain why quarks stay confined inside hadrons.
1
The Six Quarks
+5 XP
Flavours, charges, and colour confinement
When the J/ψ meson was discovered simultaneously at Brookhaven (Ting) and SLAC (Richter) on 11 November 1974 at mass 3.097 GeV/c², particle physicists recognised it as a charm–anticharm quark pair, the first direct evidence for the charm quark that Glashow, Iliopoulos, and Maiani had predicted in 1970. The quark model proposed by Murray Gell-Mann at Caltech in 1964 explained all known hadrons as combinations of quarks, fundamental spin-$\frac{1}{2}$ fermions with fractional electric charge. There are six flavours, grouped into three generations. Each flavour has a corresponding antiquark carrying opposite charge and quantum numbers.
Generation
Quark
Symbol
Charge
Mass (MeV/c²)
1
Up
u
$+2/3$
~2.2
1
Down
d
$-1/3$
~4.7
2
Charm
c
$+2/3$
~1,275
2
Strange
s
$-1/3$
~95
3
Top
t
$+2/3$
~173,000
3
Bottom
b
$-1/3$
~4,180
Ordinary matter contains only up and down quarks. Heavier quarks are produced in high-energy collisions and decay rapidly to lighter quarks via the weak force.
Each quark carries one of three colour charges: red, green, or blue. Antiquarks carry anticolours. Hadrons must always be colour-neutral (white):
Baryons: three quarks, one of each colour (red + green + blue = white). Example: proton $= uud$.
Quark confinement: quarks are never observed in isolation. Pulling quarks apart requires so much energy that the strong-force field creates new quark-antiquark pairs rather than freeing the originals. This is why only colour-neutral hadrons are seen.
Figure 1, Quark composition of the proton ($uud$, charge $= +\frac{2}{3}+\frac{2}{3}-\frac{1}{3}=+1$) and neutron ($udd$, charge $= +\frac{2}{3}-\frac{1}{3}-\frac{1}{3}=0$). Quarks are held together by gluon exchange; colours (red, green, blue) combine to give colour-neutral (white) baryons.Text description
Proton: two up quarks (+⅔ each) and one down quark (−⅓): total charge +1.
Neutron: one up quark (+⅔) and two down quarks (−⅓ each): total charge 0.
In each, the quarks are held together by gluon exchange (dashed), and their three colour charges, red, green and blue, combine to make the particle colour-neutral.
Stop and check
A $\Sigma^+$ baryon has charge $+1$ and contains one strange quark. What are its other two quarks? Verify the total charge.
Six quarks in 3 generations: Gen 1 u(+⅔)/d(−⅓); Gen 2 c(+⅔)/s(−⅓); Gen 3 t(+⅔)/b(−⅓). Ordinary matter is only u and d. Colour charge (red/green/blue): hadrons must be colour-neutral. Confinement: quarks are never free, separating them creates new pairs. Proton = uud (+1); neutron = udd (0).
Record the six quarks, their charges and generations, you'll be asked to verify hadron charge from quark composition.
Up-type quarks (u, c, t) have charge $+\frac{2}{3}$, while down-type quarks (d, s, b) have charge $-\frac{1}{3}$.
An isolated quark with charge $+\frac{2}{3}$ can be detected if enough energy is supplied to break the hadron apart.
A neutron has quark composition $udd$ and total charge $0$.
3
Assemble the Standard Model
Place the twelve matter fermions and the force-carrying bosons, and see which force each boson mediates.
Beyond the syllabus. Quarks, proton and neutron composition, hadrons and leptons are explicit core. Colour charge, confinement mechanisms, memorising all three generations and the Higgs mechanism are extension — the exam asks for the Standard Model's core picture.
2
The Standard Model
+5 XP
Particles and forces
We just saw the six quarks and the rule of colour confinement. That raises a question: where do quarks and leptons fit within the complete picture of known particles? This card answers it → the Standard Model organises all 12 matter particles (6 quarks + 6 leptons), the 4 force-carrier bosons and the Higgs boson into a single coherent framework, the most successful theory in physics.
The Standard Model is a quantum field theory that describes all known fundamental particles and three of the four fundamental forces (electromagnetic, weak, and strong). It organises particles into two groups: matter particles (fermions) and force carriers (bosons).
Matter particles, fermions (spin-½):
Quarks (6): u, d, c, s, t, b, experience strong, weak, and electromagnetic forces.
Leptons (6): $e^-$, $\mu^-$, $\tau^-$, $\nu_e$, $\nu_\mu$, $\nu_\tau$, experience weak and electromagnetic forces; neutrinos interact only via weak force and gravity.
Gluons ($g$, 8 types): mediate the strong force. Massless but confined (short effective range due to confinement).
$W^+$, $W^-$, $Z^0$: mediate the weak force. Massive (~80–90 GeV/c²); range $\sim 10^{-18}$ m.
Higgs boson ($H$, spin-0): Discovered in 2012 at CERN. Gives mass to the $W$ and $Z$ bosons and to the fundamental fermions via the Higgs mechanism, coupling to each in proportion to its mass. It does not give mass to the photon or the gluon, and it accounts for only a small fraction of the mass of ordinary matter: most of a proton's mass is the energy of its internal gluon field. Without the Higgs field, the $W$ and $Z$ bosons would be massless and the weak force would have infinite range.
Gravity is not included. General relativity describes gravity classically; unifying it with the Standard Model quantum framework remains one of the greatest unsolved problems in physics.
Figure 2, Structure of the Standard Model. Top: 12 matter particles (fermions), 6 quarks and 6 leptons in three generations. Bottom: the 4 force carriers, photon ($\gamma$), 8 gluons ($g$), $W^\pm$ and $Z^0$ bosons (weak), plus the Higgs boson ($H$), which gives particles mass rather than mediating a force. Gravity is not included.Text description
Quarks, in generations 1 to 3: up, charm, top (+⅔); down, strange, bottom (−⅓).
Leptons: electron, muon, tau (−1); electron-, muon- and tau-neutrinos (0).
Force carriers: the photon (electromagnetic, massless), 8 gluons (strong, massless), and the W± (about 80 GeV) and Z⁰ (about 91 GeV) bosons (weak).
The Higgs boson (spin 0) gives particles mass rather than carrying a force. Gravity (a possible graviton) is not part of the Standard Model.
Standard Model Summary
Quarks (6): u, d, c, s, t, b, constituents of hadrons
Photon ($\gamma$), electromagnetic force carrier (massless)
Gluons ($g$, 8 types), strong force carrier (massless; confined)
$W^\pm$, $Z^0$, weak force carriers (~80–91 GeV/c²)
Higgs ($H$), gives mass to $W$, $Z$, and fermions via Higgs mechanism
Stop and check
Why does the weak force have such a short range compared to electromagnetism? What role does the Higgs boson play in explaining this?
Standard Model: 12 matter fermions (6 quarks + 6 leptons, 3 generations) + 5 boson types. Photon (γ, EM, massless, infinite range); gluons (strong, massless, confined); W±/Z⁰ (weak, ~80–91 GeV, range ~10⁻¹⁸ m); Higgs (spin-0, found 2012, gives mass). Gravity is NOT in the Standard Model.
Write the particle table with force carriers and their ranges, knowing which boson mediates which force is tested directly.
Three of these are force-carrying bosons in the Standard Model. Pick the odd one out.
4
Clear the misconceptions
Correct the three traps: freeing a quark, what the Higgs actually gives mass to, and whether gravity is in the model.
Misconceptions, Final Check
HSC Tip, Quark Composition
Memorise the quark content of common particles: proton $= uud$ (charge $+\frac{2}{3}+\frac{2}{3}-\frac{1}{3}=+1$), neutron $= udd$ (charge $+\frac{2}{3}-\frac{1}{3}-\frac{1}{3}=0$), $\pi^+ = u\bar{d}$, $\pi^- = d\bar{u}$, $K^+ = u\bar{s}$. A common trap: forgetting that antiquarks have opposite charge. So $\bar{u}$ has charge $-\frac{2}{3}$ and $\bar{d}$ has charge $+\frac{1}{3}$. When checking particle interactions, verify conservation of charge, baryon number, and lepton number.
Wrong: "Quarks can be freed if you use enough energy."
Right: The strong force increases with separation, pumping in more energy creates new quark-antiquark pairs (jet production) rather than freeing isolated quarks. This is quark confinement.
Wrong: "The Higgs boson gives every particle its mass."
Right: The Higgs mechanism gives mass to $W^\pm$, $Z^0$ bosons and the fundamental fermions (quarks and leptons). It does NOT give mass to the photon or gluon (which remain massless), nor does it account for most of the proton's mass (which comes mainly from gluon field energy).
Wrong: "Gravity is part of the Standard Model."
Right: Gravity is described by Einstein's general relativity, a classical field theory. The Standard Model has no quantum description of gravity, unifying the two is an open problem (quantum gravity).
The quark composition of the pion $\pi^-$ is:
5
Verify quark composition and charge
Sum fractional quark charges to reproduce the observed charge of each hadron, and sort particles into quarks, leptons and bosons.
Activities
Activity 1, Quark Composition and Charge
ApplyBand 4
Determine quark content and verify charges of common particles
State the quark composition of a proton and verify its charge of $+1$ by summing quark charges.
State the quark composition of a neutron and verify its charge of $0$.
The kaon $K^+$ has quark composition $u\bar{s}$. Calculate its charge (recall $\bar{s}$ has charge $+\frac{1}{3}$). Is the $K^+$ a baryon or a meson?
A particle has composition $uss$. Calculate its electric charge and its baryon number, then state whether it is a baryon or a meson.
Identify whether each of the following is a quark, lepton, or boson: (a) electron neutrino; (b) gluon; (c) top quark; (d) muon; (e) $Z^0$.
6
Analyse decays and force ranges
Track beta decay down to the quark level, link boson mass to force range, and separate baryons from mesons.
Activity 2, The Standard Model and Conservation Laws
AnalyseBand 5
Analyse particle interactions using Standard Model principles
In beta-minus decay, a neutron becomes a proton: $n \rightarrow p + e^- + \bar{\nu}_e$. (a) Identify the quark-level change (which quark flavour changes and to what). (b) Which force mediates this decay and which boson is the intermediate carrier?
Explain why the $W$ and $Z$ bosons have a much shorter range than the photon, even though they carry the same type of force interaction (gauge bosons). What property of the $W/Z$ is responsible?
A student claims a $\Delta^{++}$ baryon (charge $+2$) is made of $uuu$. Verify this claim by calculating the total charge. What colour combination do the three quarks carry?
Explain the difference between a baryon and a meson in terms of (a) quark content, (b) baryon number, and (c) whether the particle can exist as a stable isolated particle in principle.
Analyse6 marks
Analyse how the quark model accounts for the observed charge and composition of the proton and the neutron, and for the existence of other hadrons. (6 marks)
1
State the assignment the model makes
The model is a set of assignments. Give the two that matter here.
The quark model assigns fractional electric charges: an up quark carries $+2/3$ of the elementary charge and a down quark $-1/3$.
Fractional charge is the model's boldest claim and the source of everything that follows. Both values are required.
2
Derive the proton and neutron charges
Show the arithmetic rather than asserting the result.
A proton is two up quarks and one down quark, giving a total charge of $+2/3 + 2/3 - 1/3 = +1$. A neutron is one up quark and two down quarks, giving $+2/3 - 1/3 - 1/3 = 0$.
Two observed charges reproduced from one assignment, with no adjustment between them, is the model's primary quantitative success.
3
Point out that the success is constrained, not fitted
This is the analytical step: the model could have failed here and did not.
This is a genuine constraint rather than a fitted result, because the same two charge values must reproduce both nucleons simultaneously, and no other assignment of three quarks from these two types gives $+1$ and $0$ for those combinations.
Distinguishing a prediction from a fit is what makes this analysis rather than description, and it is the reason the fractional charges are believed.
4
Extend to other hadrons by recombination
The question's second half is about generalisation.
Other hadrons are accounted for as different combinations of quarks. Baryons, including the proton and neutron, are combinations of three quarks; mesons are a quark paired with an antiquark. Including the heavier quark types generates the large number of observed hadrons from a small set of constituents.
The baryon/meson distinction by quark count is Core. It explains the hadron families as combinatorics rather than as an unexplained list.
5
Show the model constrains what can exist
A model that permits everything explains nothing. Say what is forbidden.
The model also restricts which hadrons can exist, since every observed combination must produce an integer total charge, and the observed hadron charges are indeed always integer multiples of the elementary charge despite the fractional charges of the constituents.
Integer totals from fractional parts is the resolution of the obvious objection to fractional charge, and it is a real predictive success.
6
Draw the conclusion at the right level
Close on what the model achieves.
The model therefore accounts for the nucleons' charges quantitatively, for the existence of hadron families as combinations of a few constituents, and for the fact that no hadron has been observed with fractional charge.
Three distinct achievements, each established earlier in the answer. Note the card needs nothing about colour charge or confinement, both Extension in this lesson.
7
The full-mark answer
Assignment, the two derivations, why it is a constraint, generalisation, what is forbidden, conclusion.
The quark model assigns fractional electric charges, an up quark carrying $+2/3$ of the elementary charge and a down quark $-1/3$. A proton is two up quarks and one down quark, giving $+2/3 + 2/3 - 1/3 = +1$, and a neutron is one up and two down quarks, giving $+2/3 - 1/3 - 1/3 = 0$. This is a genuine constraint rather than a fitted result, since the same two charge values must reproduce both nucleons at once and no other three-quark assignment from these two types does so. Other hadrons follow as different combinations: baryons, including the nucleons, are three quarks, while mesons are a quark paired with an antiquark, and including the heavier quark types generates the large number of observed hadrons from a small set of constituents. The model also restricts what can exist, since every allowed combination must give an integer total charge, and observed hadron charges are always integer multiples of the elementary charge despite their constituents' fractional charges. The model therefore accounts quantitatively for the nucleons' charges, for the hadron families as combinations of a few constituents, and for the absence of any observed fractionally charged hadron.
Six marks with no reference to colour charge or confinement, both of which are beyond the syllabus in this lesson despite appearing in its learning intentions.
Compare6 marks
Compare hadrons and leptons. (6 marks)
1
Distinguish them by composition first
A compare answer needs a primary respect. This is the one the classification is built on.
The fundamental difference is composition: hadrons are composite particles made of quarks, while leptons are themselves fundamental and have no known internal structure.
Composite versus fundamental is the defining distinction, and every other difference below follows from it or from the forces involved.
2
Compare them by the forces they experience
The second respect explains why the classification is useful.
They differ in the interactions they undergo. Hadrons experience the strong nuclear interaction, which is what binds their quarks together and binds nucleons in a nucleus; leptons do not experience the strong interaction at all.
This is the operational difference. Naming the strong interaction as the discriminator shows the classification reflects physics rather than convention.
3
Give examples on both sides
Concrete membership, and enough of it to show the range.
Hadrons include the proton and neutron, and mesons such as the pion. Leptons include the electron, the muon and the neutrinos.
Naming a meson as well as the nucleons shows hadrons are a family rather than a synonym for nucleons, and neutrinos extend the lepton examples usefully.
4
Note the internal structure of the hadron family
A comparison gains from noting that one side subdivides and the other does not in the same way.
The hadrons subdivide by quark content, into baryons of three quarks and mesons of a quark-antiquark pair. Leptons are not subdivided by composition, having none, but are grouped into generations with an associated neutrino for each charged lepton.
This shows the two families are organised on different principles, which is a genuine comparative point rather than an additional list.
5
State the similarities
A compare answer that finds only differences is incomplete.
They also have features in common: both include electrically charged and uncharged members, both have corresponding antiparticles, both participate in the weak interaction, and members of both are subject to gravity.
Four shared properties, briefly. This is where a comparison earns marks that a contrast alone does not.
6
Close on why the division matters
End on the use of the classification.
The division is therefore not merely descriptive: whether a particle is a hadron or a lepton determines which interactions can govern its behaviour, and separate conservation rules apply to baryon number and to lepton number when deciding whether a reaction is possible.
The conservation-law consequence is the payoff, and it connects the classification to the reaction analysis the module uses elsewhere.
7
The full-mark answer
Composition, forces, examples, internal organisation, similarities, then the use.
The fundamental difference is composition: hadrons are composite particles built from quarks, whereas leptons are themselves fundamental with no known internal structure. They differ correspondingly in their interactions, since hadrons experience the strong nuclear interaction, which binds their quarks and binds nucleons within a nucleus, while leptons do not experience it at all. Hadrons include the proton, the neutron and mesons such as the pion; leptons include the electron, the muon and the neutrinos. The two families are also organised on different principles: hadrons subdivide by quark content into baryons of three quarks and mesons of a quark-antiquark pair, while leptons, having no composition to subdivide, are grouped into generations with a neutrino associated with each charged lepton. They nonetheless share several features: both include charged and uncharged members, both have corresponding antiparticles, both take part in the weak interaction, and members of both are subject to gravity. The division is therefore not merely descriptive, since whether a particle is a hadron or a lepton determines which interactions can govern it, and separate conservation rules for baryon number and lepton number apply when judging whether a reaction can occur.
Six marks, held on four respects with similarities included. Colour charge, confinement and all-generation memorisation are Extension here and none appears.
7
Independent practice
Show what you can do without prompts
Complete a shuffled question-bank set, then write full Standard Model responses in HSC style.
Quick recall, quarks, Standard Model and conservation laws
+5 XP
A fresh five-question set drawn from this lesson's bank, feedback shown immediately. +5 XP per correct · +25 XP all correct
Pick your answer, then rate your confidence, that tells the system what to drill next.
Short Answer, 8 marks
+5 XP
ApplyBand 4(3 marks) 1. (a) State the quark composition of a proton and a neutron. (b) Calculate the electric charge of each using quark charges. (c) Explain why quarks are never observed as isolated free particles.
AnalyseBand 6(5 marks) 2. (a) List the six quark flavours and state their electric charges. (b) Distinguish between baryons and mesons in terms of quark content and baryon number. (c) Identify the force carrier for each of the three forces included in the Standard Model, and compare their masses and ranges. (d) Explain the significance of the Higgs boson, including what it gives mass to and what the consequence would be if the Higgs field did not exist. (e) State one limitation of the Standard Model.
1 mark: six quarks and charges · 1 mark: baryon/meson distinction · 1 mark: force carriers and properties · 1 mark: Higgs mechanism and consequence · 1 mark: valid limitation (no gravity, dark matter, etc.)
Show all answers
Multiple choice
MC answers and full explanations are shown inline as you complete each question. Use the retry button to attempt a fresh set drawn from the lesson bank.
Short Answer, Model Answers
Q1 (3 marks): (a) Proton $= uud$; Neutron $= udd$ (1 mark). (b) Proton: $+\frac{2}{3}+\frac{2}{3}-\frac{1}{3} = +1$; Neutron: $+\frac{2}{3}-\frac{1}{3}-\frac{1}{3} = 0$ (1 mark). (c) The strong force between quarks increases with separation rather than decreasing. When enough energy is added to separate quarks, the field energy creates a new quark-antiquark pair rather than releasing an isolated quark, so only colour-neutral hadrons are ever observed (1 mark).
Q2 (5 marks): (a) Up (u, $+\frac{2}{3}$), Down (d, $-\frac{1}{3}$), Charm (c, $+\frac{2}{3}$), Strange (s, $-\frac{1}{3}$), Top (t, $+\frac{2}{3}$), Bottom (b, $-\frac{1}{3}$) (1 mark). (b) Baryons are made of three quarks (e.g. proton $= uud$) and have baryon number $B = +1$. Mesons are made of a quark-antiquark pair (e.g. $\pi^+ = u\bar{d}$) and have baryon number $B = 0$ (1 mark). (c) Electromagnetic force: photon (massless, infinite range). Strong force: gluon (massless, but short effective range due to confinement). Weak force: $W^\pm$ and $Z^0$ bosons (~80–91 GeV/c², range $\sim 10^{-18}$ m, the large mass of the $W/Z$ gives the weak force its extremely short range) (1 mark). (d) The Higgs boson is the quantum of the Higgs field. It gives mass to the $W^\pm$, $Z^0$ bosons and the fundamental fermions via the Higgs mechanism. Without the Higgs field, the $W$ and $Z$ would be massless, making the weak force have infinite range, inconsistent with observation that the weak force is extremely short-ranged (1 mark). (e) Valid limitations include: the Standard Model does not include gravity; it does not account for dark matter or dark energy; it cannot explain the matter-antimatter asymmetry in the Universe; the Higgs mass requires fine-tuning (hierarchy problem); neutrino masses are not fully explained in the original formulation (1 mark).
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Final step
Retrieve, reflect and finish
Check what stuck, revisit your opening confinement prediction and record the quark table you will reuse.
Check what actually stuck
How did your thinking change?
At the start you were asked about the "November Revolution" of 11 November 1974, when Samuel Ting at Brookhaven and Burton Richter at SLAC independently discovered the J/ψ meson at 3.097 GeV/c², confirming Gell-Mann's 1964 quark model and the existence of the charm quark. Review your predictions:
Did you predict evidence for internal quark structure came from deep inelastic scattering experiments at SLAC (1967) showing point-like constituents inside protons? Correct, high-energy electron scattering revealed hard scattering centres inconsistent with a uniform charge distribution, exactly as quark confinement predicts.
Did you predict quarks are never isolated because of colour confinement, the strong force energy increases with separation until new quark pairs are created? Correct, the J/ψ discovery confirmed that mesons are quark–antiquark pairs confined by colour charge.
Did you predict six quarks are needed? Correct, the six-quark model (three generations) explains all observed hadrons, CP violation, and the CKM quark mixing matrix, with the top quark discovered in 1995 completing the set.
Extend: (a) The omega-minus baryon $\Omega^-$ has quark composition $sss$ and charge $-1$. Verify the charge. What is its baryon number? (b) Explain why the discovery of the Higgs boson in 2012 was considered the completion of the Standard Model. (c) A muon ($\mu^-$) has the same charge as an electron but is ~207 times heavier. Is it a quark, lepton, or boson? In what sense is it "unstable" and what does it decay into?
Take the full module quiz
quiz
A full module quiz covering every lesson in this module, not just this one. Set aside a decent block of time and treat it like a real assessment.