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15.3 Lasers, Nuclear Reactors, Radiation Detectors, Dosimetry & Elementary Particles

Key Takeaways

  • A laser needs stimulated emission, a population inversion and an optical resonator; metastable states (lifetimes around 10−3 s10^{-3}\text{ s} instead of about 10−8 s10^{-8}\text{ s}) make the inversion possible, and the helium–neon laser emits red light at 632.8 nm.

  • A thermal-neutron fission reactor uses enriched uranium fuel, a moderator (graphite or heavy water) to slow neutrons, control rods (cadmium or boron) to absorb them, and a coolant to carry heat to the turbines.

  • Alpha particles ionise most strongly but are stopped by paper; beta particles are stopped by a few millimetres of aluminium; gamma rays are only reduced by thick lead or concrete.

  • Absorbed dose is measured in gray (1 Gy=1 J/kg1\text{ Gy} = 1\text{ J/kg}); equivalent dose in sievert multiplies by the radiation's weighting factor (about 20 for alpha, 1 for beta and gamma); activity is measured in becquerel (decays per second).

  • Hadrons (baryons and mesons) are made of quarks: a proton is uud and a neutron udd, with up-quark charge +23e+\frac{2}{3}e and down-quark charge −13e-\frac{1}{3}e; leptons such as the electron and neutrino are not made of quarks.

Last updated: October 2026

Lasers, Nuclear Reactors, Radiation Detectors, Dosimetry & Elementary Particles

Section 15.2 covered photons, atomic spectra, X-rays, radioactive decay, fission and fusion. This section completes the atomic and nuclear chapters with lasers, the practical side of nuclear physics, and the modern picture of what matter is made of.


1. Lasers

LASER stands for Light Amplification by Stimulated Emission of Radiation.

Three Ways Atoms Interact with Light

ProcessWhat happens
Induced absorptionA photon of energy hf=E2−E1hf = E_2 - E_1 raises an atom from E1E_1 to E2E_2
Spontaneous emissionAn excited atom drops to a lower level on its own, emitting a photon in a random direction and phase
Stimulated emissionA passing photon of energy E2−E1E_2 - E_1 triggers an excited atom to emit an identical photon, with the same frequency, phase, direction and polarisation

Stimulated emission amplifies light, but normally most atoms are in the lower level, so absorption wins. A laser therefore needs:

  1. Population inversion: more atoms in the upper level than in the lower level, produced by pumping energy in (electrical discharge, flash lamp or another laser).
  2. A metastable state: an excited level with a long lifetime (around 10−3 s10^{-3}\text{ s}, compared with about 10−8 s10^{-8}\text{ s} for ordinary excited states), so atoms accumulate there.
  3. An optical resonator: two parallel mirrors, one fully reflecting and one partially transmitting, so photons pass back and forth through the medium many times and the beam builds up.

The Helium–Neon Laser

A glass tube contains a mixture of about 85% helium and 15% neon. An electrical discharge excites helium atoms to a metastable level whose energy almost matches an excited level of neon. Collisions transfer the energy to neon atoms, creating a population inversion in neon, which then lases at 632.8 nm (red light).

Properties and Uses of Laser Light

  • Monochromatic (a very narrow band of wavelengths), coherent (constant phase relation), directional (very little spreading) and intense.
  • Uses: eye surgery (reattaching retinas), cutting and welding, barcode scanners, optical-fibre communication, measuring distances, holography (three-dimensional images recorded by interference), and destroying kidney stones and tumours.

2. Interaction of Nuclear Radiation with Matter

Radiation loses energy mainly by ionising the atoms it passes.

RadiationNatureIonising powerPenetrationStopped by
Alpha (α\alpha)Helium nucleus, charge +2e+2eHighest (thousands of ion pairs per cm in air)A few cm of airA sheet of paper
Beta (β\beta)Fast electron, charge −e-eModerateUp to about a metre of airA few mm of aluminium
Gamma (γ\gamma)High-energy photon, no chargeLowestVery penetrating; intensity falls graduallyOnly reduced by thick lead or concrete

Gamma rays are not "stopped" at a fixed range; their intensity falls roughly exponentially with thickness, so shielding is described by the half-value thickness.


3. Radiation Detectors

DetectorPrincipleNotes
Wilson cloud chamberSupersaturated vapour condenses on ions left by a passing particle, making a visible trackAlpha tracks are thick and straight; beta tracks are thin and twisted; gamma rays leave faint scattered tracks
Geiger–Muller (GM) counterA gas-filled tube with a central wire anode at high voltage; each ionising particle triggers an avalanche of ions and a pulse that is countedA quenching gas stops the discharge; the dead time (about 10−4 s10^{-4}\text{ s}) limits the maximum count rate
Solid-state detectorA reverse-biased p-n junction; radiation creates electron–hole pairs that give a current pulseFast and compact; the pulse size is proportional to the particle's energy, so it can measure energies

A counter always records a small background count from cosmic rays and natural radioactivity, which must be subtracted from measurements.


4. Nuclear Reactors

Each fission of uranium-235 by a slow neutron releases about 200 MeV and two or three neutrons (Section 15.2). If at least one of these neutrons causes another fission, a chain reaction continues. The minimum mass needed for a self-sustaining chain reaction is the critical mass.

ComponentFunctionTypical material
FuelUndergoes fissionUranium enriched to about 3% uranium-235 (natural uranium is about 0.7%)
ModeratorSlows fast neutrons to thermal speeds so they cause fission efficientlyGraphite, heavy water, ordinary water
Control rodsAbsorb neutrons to keep the reaction steady or shut it downCadmium or boron
CoolantCarries heat from the core to a heat exchangerWater, heavy water, carbon dioxide gas
ShieldingProtects workers from radiationThick concrete

The heat produces steam that drives turbines and generators, as in a conventional power station. In a fast breeder reactor, uranium-238 absorbs neutrons and is converted into fissile plutonium-239, producing more fuel than it consumes.


5. Radiation Dose and Biological Effects

QuantityUnitMeaning
Activitybecquerel (Bq) = 1 decay/s; older unit curie (Ci) = 3.7×1010 Bq3.7 \times 10^{10}\text{ Bq}Rate of decay of a source
Absorbed dosegray (Gy) = 1 J/kgEnergy absorbed per kilogram of tissue
Equivalent dosesievert (Sv)Absorbed dose × radiation weighting factor (RBE)

The weighting factor is about 1 for beta and gamma radiation and about 20 for alpha particles, so 1 mGy of alpha radiation inside the body is roughly as harmful as 20 mGy of gamma radiation.

  • Somatic effects damage the exposed person (burns, radiation sickness, cancer, cataracts).
  • Genetic effects damage reproductive cells and can be passed to future generations.
  • Typical natural background dose is a few millisieverts per year. Protection relies on time (minimise exposure), distance (intensity falls with the square of distance from a point source) and shielding.

Uses of Radioisotopes

  • Medical tracers: iodine-131 to study the thyroid; technetium-99m for imaging.
  • Radiotherapy: gamma rays from cobalt-60 to destroy cancer cells.
  • Carbon dating: carbon-14 (half-life about 5730 years) dates once-living material up to tens of thousands of years old.
  • Industry and agriculture: thickness gauging, leak detection in pipes, sterilising medical equipment, and tracing fertiliser uptake by plants.

6. Basic Forces and Building Blocks of Matter

ForceRelative strengthRangeActs on
Strong nuclearStrongestAbout 10−15 m10^{-15}\text{ m}Quarks and hadrons
ElectromagneticAbout 10−210^{-2} of strongInfiniteCharged particles
Weak nuclearMuch weakerLess than 10−17 m10^{-17}\text{ m}All leptons and quarks; causes beta decay
GravitationalWeakest by farInfiniteAll masses

Particles are grouped as:

  • Hadrons, which feel the strong force and are built from quarks: baryons (three quarks, such as protons and neutrons) and mesons (a quark and an antiquark, such as pions).
  • Leptons, which do not feel the strong force and are not made of quarks: the electron, muon, tau and their neutrinos.
QuarkCharge
Up (u)+23e+\frac{2}{3}e
Down (d)−13e-\frac{1}{3}e

A proton is uuduud: charge 23+23−13=+1\frac{2}{3} + \frac{2}{3} - \frac{1}{3} = +1. A neutron is uddudd: charge 23−13−13=0\frac{2}{3} - \frac{1}{3} - \frac{1}{3} = 0. In beta-minus decay a down quark changes into an up quark, turning a neutron into a proton and emitting an electron and an antineutrino.

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Three Conditions for Laser Action
Test Your Knowledge

Which component of a thermal nuclear reactor slows down fast neutrons so that they can cause further fission of uranium-235?

A

The control rods made of cadmium

B

The concrete shielding

C

The moderator, such as graphite or heavy water

D

The coolant in the heat exchanger

Test Your Knowledge

A tissue sample absorbs 2 mGy from alpha particles. Taking the radiation weighting factor of alpha particles as 20, what is the equivalent dose?

A

2 mSv

B

10 mSv

C

0.1 mSv

D

40 mSv

Test Your Knowledge

Which combination of quarks forms a neutron?

A

up, down, down

B

up, up, down

C

up and anti-down

D

down, down, down

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