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fundamental interactions and elementary-particle families

Learning objectives

  • Outcome

    List the four fundamental interactions, stating for each its mediator, relative strength, and range.

  • Outcome

    Classify a given particle as a fermion or boson and assign it to a family (quark, lepton, gauge boson, scalar).

  • Outcome

    Compute the electric charge of a hadron from its quark content and name the interaction that binds it.

  • Outcome

    Decide from a lifetime and a reaction type which fundamental interaction governs it.

Understand the idea

Fundamental Interactions and Elementary-Particle Families

Text

In modern physics the whole variety of interactions reduces to four fundamental ones: gravitational, electromagnetic, strong, and weak. Each is carried by the exchange of mediator particles — gauge bosons: the photon γ\gamma for the electromagnetic, gluons gg for the strong, the W±W^\pm and ZZ bosons for the weak, while gravity is carried by tensor perturbations of the metric (the hypothetical graviton GG). The relative strengths are conveniently remembered as strong:electromagnetic:weak:gravitational≈1:10−2:10−6:10−39\text{strong} : \text{electromagnetic} : \text{weak} : \text{gravitational} \approx 1 : 10^{-2} : 10^{-6} : 10^{-39} at typical energies of order a GeV. The range of the strong interaction is ∼10−15\sim 10^{-15} m and of the weak interaction ∼10−18\sim 10^{-18} m, whereas the electromagnetic and gravitational interactions have unlimited range and fall off as 1/r21/r^2. By spin, particles divide into fermions (half-integer spin, obeying the Pauli principle), which make up matter — quarks and leptons — and bosons (integer spin), which carry interactions or give mass (the Higgs boson HH). The quarks u,d,s,c,b,tu, d, s, c, b, t have fractional charges +2/3+2/3 and −1/3-1/3, are never observed in isolation (confinement), and form hadrons: baryons made of three quarks (for example p=uudp = uud) and mesons made of a quark–antiquark pair (for example π+=udˉ\pi^+ = u\bar d).

Worked examples

Direct

Problem

The proton consists of the quarks uuduud, the neutron of uddudd. Compute the charge of each particle in units of ee and state which family they belong to and which interaction holds them together.

Solution

Quark charges: qu=+2/3q_u = +2/3, qd=−1/3q_d = -1/3.

  • Proton: qp=23+23−13=+1q_p = \tfrac{2}{3} + \tfrac{2}{3} - \tfrac{1}{3} = +1.
  • Neutron: qn=23−13−13=0q_n = \tfrac{2}{3} - \tfrac{1}{3} - \tfrac{1}{3} = 0.

Both contain three quarks, hence baryon number B=1B = 1 and spin 1/21/2 — they are fermions (baryons). The binding is provided by the strong interaction through gluon exchange; confinement prevents knocking out a single quark.

Application

Problem

The muon decays as μ−→e−+νˉe+νμ\mu^- \to e^- + \bar\nu_e + \nu_\mu with a lifetime of 2.2×10−62.2\times10^{-6} s, while the neutral pion decays as π0→γγ\pi^0 \to \gamma\gamma with a lifetime of 8×10−178\times10^{-17} s. Determine which interactions are responsible, name the mediators, and explain the difference in lifetimes.

Solution
  1. In the muon decay the lepton flavour changes (μ→e\mu \to e), and neutrinos participate only in the weak interaction, so this is a weak process; the mediator is the W−W^- boson.
  2. In the π0=uuˉ\pi^0 = u\bar u decay a quark and an antiquark annihilate into two photons; flavour does not change and charge is conserved, so the mediator is the photon, that is, the electromagnetic interaction.
  3. Comparison: τμ/τπ0≈2.2×10−6/8×10−17≈3×1010\tau_\mu / \tau_{\pi^0} \approx 2.2\times10^{-6} / 8\times10^{-17} \approx 3\times10^{10}. The weak interaction is strongly suppressed by its small coupling constant and by the propagator of the heavy WW boson, so weak decays are many orders of magnitude slower than electromagnetic ones.

Transfer

Problem

Estimate the range of the weak interaction from the WW-boson mass mWc2=80m_W c^2 = 80 GeV using R≈ℏc/(mc2)R \approx \hbar c / (m c^2) with ℏc=197\hbar c = 197 MeV·fm. Compare it with the range of the strong interaction estimated from the pion mass mπc2=140m_\pi c^2 = 140 MeV, and explain why a neutrino with an energy of order 1 MeV hardly interacts with matter.

Solution
  1. Weak interaction: RW≈ℏcmWc2=197 MeV⋅fm8.0×104 MeV≈2.5×10−3 fm=2.5×10−18 m.R_W \approx \frac{\hbar c}{m_W c^2} = \frac{197\ \text{MeV·fm}}{8.0\times10^{4}\ \text{MeV}} \approx 2.5\times10^{-3}\ \text{fm} = 2.5\times10^{-18}\ \text{m}.
  2. Strong interaction: Rπ≈197 MeV⋅fm140 MeV≈1.4 fm=1.4×10−15 m.R_\pi \approx \frac{197\ \text{MeV·fm}}{140\ \text{MeV}} \approx 1.4\ \text{fm} = 1.4\times10^{-15}\ \text{m}.
  3. The ratio Rπ/RW≈560R_\pi / R_W \approx 560: the weak interaction is "pointlike" on the scale of a nucleus and a nucleon.
  4. A neutrino participates only in the weak interaction, so the cross section of the reaction ν+n→p+e−\nu + n \to p + e^- is of order σ∼GF2E2\sigma \sim G_F^2 E^2 and at E∼1E \sim 1 MeV is extremely small: a neutrino travels through enormous thicknesses of matter without collisions.

Practice

Text

A safe self-study activity based on databases (no measurements with radiation sources are performed).

  1. Open the online resource PDG Live (pdg.lbl.gov) or an interactive particle table and an open particle-physics simulation (for example, a detector event display).
  2. Fill in a table for the particles pp, nn, π+\pi^+, K−K^-, e−e^-, μ−\mu^-, νe\nu_e, γ\gamma, W−W^-, HH: type (fermion/boson), family (quark, lepton, gauge boson, scalar), charge in units of ee, baryon and lepton numbers, spin.
  3. Check the conservation of charge, baryon number, and lepton number in the reactions n→p+e−+νˉen \to p + e^- + \bar\nu_e and π+→μ++νμ\pi^+ \to \mu^+ + \nu_\mu.
  4. For each interaction, state its mediator, relative strength, and range, and then explain in one sentence which interaction dominates in each of the reactions you checked.

Visual reference

Purpose

To show that the four fundamental interactions differ in mediator, relative strength, and range, and that elementary particles divide by spin into matter fermions (quarks, leptons) and mediator bosons (plus the Higgs scalar).

Representation

Two coordinated diagrams on a single sheet.

(a) Interaction table. Rows — gravitational, electromagnetic, strong, weak; columns — mediator (mass, spin), relative strength, range, example process. Inside the cells, the symbols GG, γ\gamma, gg, W±/ZW^\pm/Z and the numbers 1:10−2:10−6:10−391 : 10^{-2} : 10^{-6} : 10^{-39}.

(b) Particle "tree". On the left the fermion branch with spin 1/21/2: quarks u,d,s,c,b,tu, d, s, c, b, t with charges +2/3+2/3 and −1/3-1/3; leptons e,μ,τ,νe,νμ,ντe, \mu, \tau, \nu_e, \nu_\mu, \nu_\tau. On the right the boson branch: gauge gg, γ\gamma, W±W^\pm, ZZ (spin 1) and the scalar HH (spin 0). Arrows from the quarks show composite hadrons: p=uudp = uud, n=uddn = udd, π+=udˉ\pi^+ = u\bar d.

Real-world examples

Basketball bounce: gravity and electromagnetic contact

Scenario

A basketball of mass m=0,62 kgm = 0{,}62\ \mathrm{kg} falls from a height h=1,5 mh = 1{,}5\ \mathrm{m}. Earth pulls it with a force Fg=mg≈6,1 NF_g = mg \approx 6{,}1\ \mathrm{N}. Just before impact the speed is v=2gh≈5,4 m/sv = \sqrt{2gh} \approx 5{,}4\ \mathrm{m/s} and the momentum is p=mv≈3,4 kg⋅m/sp = mv \approx 3{,}4\ \mathrm{kg\cdot m/s}. If the ball stops in Δt=0,02 s\Delta t = 0{,}02\ \mathrm{s}, the floor exerts an average force F=ΔpΔt≈1,7×102 NF = \frac{\Delta p}{\Delta t} \approx 1{,}7\times10^{2}\ \mathrm{N} — 28 times its weight.

Connection

The scenario uses two fundamental interactions. The gravitational interaction acts on the ball's mass and sets Fg=mgF_g = mg. The contact force comes from the electromagnetic interaction: electron shells of atoms in the ball and floor repel, preventing the bodies from passing through each other. The atoms themselves are made of quarks (inside protons and neutrons) and leptons (electrons).

Phone touchscreen: electromagnetic sensing

Scenario

A smartphone's glass screen contains transparent electrodes. Each electrode has a capacitance of about C=10 pFC = 10\ \mathrm{pF} at a voltage V=1,8 VV = 1{,}8\ \mathrm{V}. The charge on such an electrode is Q=CV≈1,8×10−11 CQ = CV \approx 1{,}8\times10^{-11}\ \mathrm{C}, which corresponds to about N=Q/e≈1,1×108N = Q/e \approx 1{,}1\times10^{8} electrons. When a finger — full of water and mobile ions — comes within fractions of a millimetre, the capacitance changes by about 1 pF1\ \mathrm{pF} (roughly 10%10\%), and the controller registers a touch.

Connection

The sensor's operation is purely the electromagnetic interaction. Its carrier is the photon — the gauge boson of the electromagnetic field. Charges in the electrodes and in the finger interact at a distance, changing the capacitance. The electrons that create the charge and current in the sensor belong to the lepton family.

The Sun as a fusion reactor: strong and weak interactions

Scenario

The Sun radiates a power L=3,8×1026 WL = 3{,}8\times10^{26}\ \mathrm{W}. By E=mc2E = mc^2, this means a mass m=Lc2≈4,2×109 kgm = \frac{L}{c^2} \approx 4{,}2\times10^{9}\ \mathrm{kg} is converted into energy every second. Since fusing four protons into a helium nucleus converts about 0,66%0{,}66\% of the mass into energy, the Sun consumes roughly 6×1011 kg6\times10^{11}\ \mathrm{kg} of hydrogen per second. The reaction begins with a proton turning into a neutron: p+p→d+e++νep + p \rightarrow d + e^+ + \nu_e, where dd is a deuteron, e+e^+ a positron, and νe\nu_e an electron neutrino.

Connection

Two short-range interactions are at work here. The weak interaction turns a proton into a neutron by emitting a WW boson; without it the pppp chain would not start. The strong interaction, carried by gluons, binds quarks inside protons and neutrons and glues them into a deuteron and helium, overcoming the electric repulsion of protons. The neutrino and positron are leptons, while protons and neutrons are baryons built from quarks.