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CERN · A Field Guide · No. 13

Particle Physics /

The zoo of fundamental things

From Thomson's electron to the Higgs — a hundred and twenty-five years of finding pieces of matter that refused to break further.

A 13-slide deck · 2026

02 · Pre-history

Before the Standard Model

1897

J. J. Thomson

Cathode-ray experiments at Cambridge reveal a particle ~1/1836 the mass of hydrogen — the electron. The atom is no longer indivisible.

1911

Ernest Rutherford

Alpha particles fired at gold foil bounce backward. Atoms are mostly empty space with a tiny dense nucleus. Plum-pudding is dead.

1932

Chadwick · Anderson

The neutron is found. The positron arrives — Dirac's prediction of antimatter is real.

1930s–50s

The particle zoo

Cosmic-ray cloud chambers and early accelerators produce muons, pions, kaons, lambdas. Dozens of "elementary" particles. Nobody is happy about this.

03 · Forces

Four ways things push

Strong

Gluons bind quarks into protons, neutrons. Confined to ~10-15 m. Strongest, shortest range.

EM

Photons. Infinite range. Light, chemistry, electricity, magnetism — all one thing since Maxwell.

Weak

W±, Z bosons. Beta decay. Massive carriers — that's why it's "weak" and short-range (~10-18 m).

Gravity

Hypothetical graviton. Infinite range, absurdly weak (10-39 of EM). Not in the Standard Model.

The Standard Model unifies the first three. The fourth still refuses to join.

04 · Cast

Fermions vs Bosons

FERMIONS · spin ½

Matter

The stuff that makes things. Obey Pauli exclusion — no two in the same quantum state. That's why atoms have shells, why solids are solid.

  • Quarks (build hadrons)
  • Leptons (electrons, neutrinos, ...)
BOSONS · integer spin

Force-carriers

Mediators. Pile up freely in the same state — that's why lasers and superconductors work. They exchange between fermions to make forces happen.

  • Gauge bosons (γ, g, W, Z)
  • Higgs (scalar, spin 0)

05 · 1964

The quark model

Murray Gell-Mann (and George Zweig, independently) propose: the particle zoo isn't a zoo of elementaries. The hadrons are composite, built from a small set of fractionally-charged constituents.

Three flavors at first — u, d, s — later expanded to six. Combinations:

  • Mesons: q q̄ — quark + antiquark (pion, kaon)
  • Baryons: q q q — three quarks (proton, neutron)

"Three quarks for Muster Mark." — Joyce, via Gell-Mann.

PROTON u u d PION (π⁺) u

06 · Leptons

The other half of matter

Leptons don't feel the strong force. Three charged leptons, three neutrinos — arranged in three generations, each heavier than the last.

GENERATION I

electron · e⁻

Mass 0.511 MeV. Stable. Builds every atom.

νe — electron neutrino. Nearly massless.

GENERATION II

muon · μ⁻

Mass 106 MeV. Lifetime 2.2 μs.

νμ — muon neutrino.

GENERATION III

tau · τ⁻

Mass 1.78 GeV. Heavier than a proton.

ντ — tau neutrino.

Rabi on the muon's discovery: "Who ordered that?"

07 · The chart

The Standard Model

u
UP
2.2 MeV
c
CHARM
1.27 GeV
t
TOP
173 GeV
γ
PHOTON
0
d
DOWN
4.7 MeV
s
STRANGE
95 MeV
b
BOTTOM
4.18 GeV
g
GLUON
0
e
ELECTRON
0.511 MeV
μ
MUON
106 MeV
τ
TAU
1.78 GeV
Z
Z BOSON
91.2 GeV
νe
e-NEUTRINO
< eV
νμ
μ-NEUTRINO
< eV
ντ
τ-NEUTRINO
< eV
H
HIGGS
125 GeV
Quarks (6) Leptons (6) Gauge bosons (4) Higgs (1)

08 · 1983

W and Z bosons

1968. Glashow, Weinberg, Salam unify electromagnetism and the weak force into electroweak theory. The theory predicts three new heavy bosons: W⁺, W⁻, Z⁰.

1983. Carlo Rubbia and Simon van der Meer at CERN's Super Proton Synchrotron see them at exactly the predicted masses.

  • W± : 80.4 GeV — charged-current weak decays
  • Z⁰ : 91.2 GeV — neutral-current weak decays
  • Nobel Prize, 1984

A theory makes a number. A machine measures the number. They agree to four decimals. That's the Standard Model working.

BETA DECAY · FEYNMAN d u W⁻ e⁻ ν̄ₑ d → u + W⁻ → u + e⁻ + ν̄ₑ

09 · 2012

The Higgs boson

The problem

Gauge symmetry says W, Z, and fermions should be massless. They aren't. W weighs as much as a silver atom.

The 1964 fix

Englert · Brout · Higgs propose a scalar field filling all space. Particles drag through it; the drag is mass. The field's quantum is a new boson.

The 2012 find

ATLAS and CMS at the LHC see a bump at 125 GeV, decaying as the theory predicted. announced 4 July 2012.

What it does

  • Gives mass to W, Z via electroweak symmetry breaking
  • Gives mass to fermions via Yukawa couplings
  • Last missing Standard Model particle

Nobel: Englert & Higgs, 2013.

10 · Beyond

What the Standard Model doesn't explain

Dark matter

Galaxies rotate as if there's ~5× more matter than we see. Standard Model has no candidate. WIMPs, axions, sterile neutrinos — none confirmed.

Neutrino mass

Neutrinos oscillate between flavors — therefore have mass. The Standard Model says they shouldn't. Where does the mass come from? Majorana? See-saw?

Hierarchy

Why is the Higgs 125 GeV and not 1019 GeV (the Planck scale)? Quantum corrections should drag it up. They don't. Why?

Matter–antimatter

The Big Bang should have made equal amounts. We see a universe of matter. CP violation in the SM is ~10⁹ too small to explain it.

Dark energy

The expansion is accelerating. About 68% of the universe is some unknown vacuum-energy-like thing. The SM offers nothing.

Gravity

Just absent. General relativity is classical; the SM is quantum. They don't combine without infinities.

11 · Machines

Where the work happens

LHC · CERN

27 km ring under France/Switzerland. Proton-proton at 13.6 TeV. Found the Higgs. Currently Run 3.

ATLAS

General-purpose detector at LHC. 7000 tonnes, 100M readout channels. One of two that found the Higgs.

CMS

Compact Muon Solenoid. The other Higgs-discovery detector. Different design, same answer — that's how you cross-check.

Fermilab

Illinois. Tevatron found the top quark (1995). Now hosts g-2 muon experiments — possible hints of new physics.

IceCube

A cubic kilometer of Antarctic ice instrumented for neutrinos. First detection of astrophysical neutrinos, 2013.

KATRIN · Super-K · DUNE

Neutrino mass and oscillation experiments. Patient, precise, low-background. The opposite of a hadron collider in style.

12 · Open

Unresolved · 2026

Quantum gravity

String theory and loop quantum gravity remain mathematically rich, experimentally untested. Energies of 1019 GeV are roughly 1015× beyond the LHC.

Supersymmetry

Predicted superpartners would solve the hierarchy problem and offer a dark-matter candidate. The LHC has not found them at expected masses. Minimal SUSY is in trouble; weaker variants survive.

The next collider

Three serious proposals: FCC-ee/hh (CERN, 91 km), CEPC (China, ~100 km), muon collider (Fermilab concept). Decades and tens of billions either way.

Anomalies to chase

Muon g-2 tension, lepton-flavor universality hints in B mesons, the W-mass measurement controversy. Each is small. Each could be the crack.

13 · End

Read further · watch further

References

  • Griffiths · Introduction to Elementary Particles (2nd ed.)
  • Peskin & Schroeder · An Introduction to QFT
  • Frank Close · The Infinity Puzzle
  • Sean Carroll · The Particle at the End of the Universe
  • home.cern · CERN public site
  • particleadventure.org · LBNL primer
  • pdg.lbl.gov · Particle Data Group

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"The history of physics is a history of finding the next layer down. There is no reason to think we're near the bottom."