11. Particle physics AS

Syllabus
9702–2028–2029
Section
11
Level
AS

11.1 Atoms, nuclei and radiation

Syllabus
9702–2028–2029
Topic
11.1
Level
AS

Alpha scattering showed that atoms contain a tiny dense positive nucleus

Most alpha particles passed through thin foil, but a small fraction were deflected through large angles; this implies most atomic volume is empty with mass and positive charge concentrated in a tiny nucleus.

Use the scattering observations as evidence and distinguish the nuclear model from the older diffuse-charge model.

A near head-on deflection is rare because the nucleus occupies a tiny cross-section, yet it reveals strong repulsion from concentrated positive charge.

The experiment did not show electrons orbiting like planets; it established nuclear concentration, not a complete modern atom model.

The nuclear atom contains protons and neutrons in a small nucleus with electrons outside it

A simple nuclear model places positively charged protons and neutral neutrons in a tiny nucleus, with negatively charged electrons occupying the surrounding region.

Mass is concentrated mainly in nucleons while atomic size is set by the electron region. This is a model, not a literal set of classical orbits.

Changing the number of electrons can make an ion without changing the nucleus or the element identity.

Electrons are not inside the nucleus in this model, and a neutral atom does not mean it contains no charged particles.

Proton number identifies the element, while nucleon number counts protons plus neutrons

Proton number Z is the number of protons; nucleon number A is total protons plus neutrons, so neutron number is A−Z.

Z determines chemical identity. A can vary between isotopes while Z remains fixed.

A nuclide with A=23 and Z=11 contains 11 protons and 12 neutrons.

Nucleon number is not the number of electrons, and changing A alone does not create a new element.

Isotopes are atoms of the same element with different neutron numbers

Isotopes have the same proton number but different numbers of neutrons, so they share chemical identity but differ in mass and nuclear properties.

Compare Z first, then A. Isotopic abundance affects relative atomic mass without changing the element symbol.

Carbon-12 and carbon-14 both have Z=6; carbon-14 has two more neutrons and is radioactive.

Isotopes are not different elements, and isotope differences are not caused by different electron counts in neutral atoms.

Read nuclide notation and count particles in atoms and ions

⁽(A)Z)X:A=nucleonnumber,Z=protonnumber,X=elementsymbol⁽ᴬ⁾₍Z₎X: A = nucleon number, Z = proton number, X = element symbol

Quantity Count
protons Z
neutrons A − Z
electrons in a neutral atom Z
electrons in an ion of charge +ne Z − n
electrons in an ion of charge −ne Z + n

For ²³⁹₉₄Pu⁺, protons = 94, neutrons = 239 − 94 = 145 and electrons = 94 − 1 = 93. The + sign means one electron has been removed; it does not change the nucleus.

To write a nuclide symbol, use the periodic-table identity to select X and Z, then place total protons plus neutrons as A at upper left and Z at lower left.

Do not swap A and Z. A is not neutron number, and an ionic charge changes electron count only; it does not change A, Z or the isotope.

Balance nucleon number and electric charge separately

ΣAbefore=ΣAafterandΣ(q/e)before=Σ(q/e)afterΣA_before = ΣA_after and Σ(q/e)_before = Σ(q/e)_after

Emitted object nucleon number A charge number q/e
α particle 4 +2
β⁻ electron 0 −1
β⁺ positron 0 +1
γ photon or (anti)neutrino 0 0

Write every reactant and product, then total the upper numbers for nucleon number and the signed lower charge numbers independently. A missing particle or wrong daughter is exposed when either ledger fails.

Alpha decay conserves A through A = (A − 4) + 4 and charge through Z = (Z − 2) + 2. In beta-minus decay, the daughter's nuclear proton number rises by one, but total charge still balances: Z = (Z + 1) + (−1).

Proton number and neutron number are not each separately conserved in beta decay: one nucleon changes type. The conserved quantities here are total nucleon number and total electric charge across all products.

Compare alpha, beta-minus, beta-plus and gamma radiation

Radiation Composition Rest mass Charge
α helium nucleus: 2 protons + 2 neutrons about 4 u +2e
β⁻ electron 9.11 × 10⁻³¹ kg ≈ 5.49 × 10⁻⁴ u −e
β⁺ positron same as electron +e
γ electromagnetic photon 0 0

Identify radiation from all three requested properties. Positive charge alone is insufficient: both α and β⁺ are positive, but α has charge magnitude 2e and a mass thousands of times larger.

α=24He,β−=−10e,β+=+10e,γ=00γα = ⁴₂He, β⁻ = ⁰₋₁e, β⁺ = ⁰₊₁e, γ = ⁰₀γ

Gamma radiation is electromagnetic radiation, not a neutral nucleon. A beta particle has the electron/positron rest mass; its high speed does not make its rest mass zero.

An antiparticle has equal mass and opposite charge

The antiparticle corresponding to a particle has the same rest mass and electric charge of equal magnitude but opposite sign.

Particle Antiparticle Mass relation Charge relation
electron e⁻ positron e⁺ equal −e and +e
proton p antiproton p̄ equal +e and −e

If a top quark has charge +(2/3)e, its antiquark has the same mass and charge −(2/3)e. Reverse the sign; do not change the magnitude or mass.

A positron is specifically the electron's antiparticle. It is not a proton: both carry +e, but their masses and particle identities are different.

Beta-minus emits an antineutrino; beta-plus emits a neutrino

Decay Nucleon change Charged beta particle Neutral lepton
β⁻ neutron → proton electron e⁻ electron antineutrino ν̄ₑ
β⁺ proton → neutron positron e⁺ electron neutrino νₑ

n→p+e−+νˉep→n+e++νen → p + e⁻ + ν̄ₑ p → n + e⁺ + νₑ

Match the beta sign first: β⁻ is the electron and therefore accompanies the antineutrino; β⁺ is the positron and accompanies the neutrino. Both (anti)neutrinos have zero charge and zero nucleon number.

The (anti)neutrino is an additional emitted particle, not another name for the beta particle. Omitting it makes a beta-decay equation incomplete for this syllabus.

Alpha particles have discrete energies, whereas beta particles have a continuous energy spectrum

Alpha decay between quantised nuclear levels gives particles with characteristic discrete energies; beta decay shares energy with a neutrino, producing a continuous range.

Interpret line spectra and broad beta spectra as evidence about the number of bodies sharing decay energy.

A detector can show sharp alpha peaks but a broad beta distribution ending at a maximum energy.

A continuous beta spectrum does not mean beta particles are emitted with random violation of energy conservation; total energy is conserved event by event.

Write complete alpha, beta-minus and beta-plus decay equations

α:ZAX→−2A−4Y+24Heβ−:ZAX→+1AY+−10e+00νˉeβ+:ZAX→−1AY++10e+00νeα: ᴬ_ZX → ᴬ⁻⁴_Z₋₂Y + ⁴₂He β⁻: ᴬ_ZX → ᴬ_Z₊₁Y + ⁰₋₁e + ⁰₀ν̄ₑ β⁺: ᴬ_ZX → ᴬ_Z₋₁Y + ⁰₊₁e + ⁰₀νₑ

Identify the decay type, calculate the daughter A and Z, use Z to identify its element symbol, add every emitted particle, then check that upper numbers and signed lower numbers balance separately.

Decay Complete example Check
α ²³⁸₉₂U → ²³⁴₉₀Th + ⁴₂He 238 = 234 + 4; 92 = 90 + 2
β⁻ ³₁H → ³₂He + ⁰₋₁e + ⁰₀ν̄ₑ 3 = 3; 1 = 2 − 1
β⁺ ¹²₇N → ¹²₆C + ⁰₊₁e + ⁰₀νₑ 12 = 12; 7 = 6 + 1

A is unchanged in beta decay. The daughter Z rises for β⁻ and falls for β⁺, and the correct electron (anti)neutrino must be included even though it contributes 0 to both number checks.

Convert particle and nuclear masses using the unified atomic mass unit

One unified atomic mass unit, 1 u, is one twelfth of the mass of a neutral carbon-12 atom. Use 1 u = 1.66 × 10⁻²⁷ kg.

massinkg=massinu×1.66×10−27massinu=massinkg÷(1.66×10−27)mass in kg = mass in u × 1.66 × 10⁻²⁷ mass in u = mass in kg ÷ (1.66 × 10⁻²⁷)

A particle of mass 12.0 u has mass 12.0 × 1.66 × 10⁻²⁷ = 1.99 × 10⁻²⁶ kg.

A nucleus of mass 7.30 × 10⁻²⁶ kg has mass (7.30 × 10⁻²⁶)/(1.66 × 10⁻²⁷) = 44.0 u.

Nucleon number A is an integer count, not an exact nuclear mass in u. Binding energy causes the actual mass of a nucleus to differ from the simple sum of free nucleon masses.

11.2 Fundamental particles

Syllabus
9702–2028–2029
Topic
11.2
Level
AS

Quarks are fundamental particles with six flavours

A fundamental particle is not known to contain smaller constituent particles: it cannot be subdivided into a simpler internal structure. Quarks are fundamental particles.

Group for charge learning Quark flavours
up-type up (u), charm (c), top (t)
down-type down (d), strange (s), bottom (b)

The six flavour names are up, down, strange, charm, top and bottom. Each also has a corresponding antiquark flavour, so there are six antiquark flavours.

Meson, baryon, proton and neutron are not quark flavours; they are composite hadrons. For this syllabus, learn quark flavour and charge only—no other quark properties are required.

Use quark and antiquark charges to find composite charge

Flavours Quark charge Corresponding antiquark charge
u, c, t +(2/3)e −(2/3)e
d, s, b −(1/3)e +(1/3)e

Replace every constituent by its signed charge and add. An antiquark keeps the flavour family but reverses the charge sign.

Proton uud: +(2/3)e +(2/3)e −(1/3)e = +e. Neutron udd: +(2/3)e −(1/3)e −(1/3)e = 0. Antiproton ūūd̄: −(2/3)e −(2/3)e +(1/3)e = −e.

Do not reverse flavour when forming an antiquark: anti-up is still the antiparticle of up, but its charge is −(2/3)e. Fractional constituent charges can sum to an integer hadron charge.

Protons are uud and neutrons are udd

Nucleon Quark composition Charge sum
proton uud 2/3 + 2/3 − 1/3 = +1
neutron udd 2/3 − 1/3 − 1/3 = 0

Protons and neutrons are not fundamental because each is a composite baryon containing three quarks.

ForZprotonsandNneutrons:numberofu=2Z+N,numberofd=Z+2NFor Z protons and N neutrons: number of u = 2Z + N, number of d = Z + 2N

Tritium has Z = 1 and N = 2, so it contains 2(1)+2 = 4 up quarks and 1+2(2) = 5 down quarks. An alpha particle has two protons and two neutrons, giving 6 up and 6 down quarks.

A neutron is neutral because its fractional constituent charges sum to zero, not because it contains no charged quarks.

Hadrons are baryons or mesons according to constituent pattern

Hadron class Constituent pattern Examples
baryon three quarks proton uud, neutron udd
antibaryon three antiquarks antiproton ūūd̄
meson one quark + one antiquark pion

A hadron is a composite particle made from quarks. For the syllabus classification, hadrons are baryons or mesons; flavour combinations need not use identical quarks.

A neutral meson can pair a quark with its corresponding antiquark, such as uū: +(2/3)e −(2/3)e = 0. Charge validity must agree with the constituent signs.

Electrons, positrons, neutrinos and antineutrinos are leptons, not hadrons. A meson is not two baryons and does not contain two ordinary quarks.

Beta decay changes quark flavour while conserving total charge and nucleon number

In β− decay a down quark changes to an up quark, turning a neutron udd into a proton uud and emitting an electron and antineutrino; β+ reverses the quark change with a positron and neutrino.

Track the quark charge change and the emitted lepton charges together. The weak interaction mediates the flavour change.

A neutron’s d→u raises hadron charge by +e, balanced by the emitted electron’s −e in β− decay.

The beta electron is not an orbital electron released from the atom; it is created in the weak decay process.

Electrons and neutrinos are fundamental leptons

Leptons are fundamental particles: they are not made from quarks. In this syllabus, recognise electrons and neutrinos and their antiparticles as leptons.

Lepton Antiparticle Electric charge
electron e⁻ positron e⁺ −e; antiparticle +e
electron neutrino νₑ electron antineutrino ν̄ₑ 0; antiparticle 0
Fundamental leptons Composite hadrons (not leptons)
electron, positron, neutrino, antineutrino proton, neutron, baryon, meson

Beta-minus emission contains two leptons: an electron and an electron antineutrino. Beta-plus emission contains a positron and an electron neutrino.

A positron is a positively charged lepton, so it is false that every charged lepton has charge −e. A neutrino is not a neutral hadron or a photon.