Category
page 1Standard Model
Higgs boson
elementary particle transmitting the Higgs field giving particles mass
Standard Model
theory of particle physics based on Yang–Mills theory with gauge group SU(3)×SU(2)×U(1) and spontaneous symmetry breaking
top quark
the heaviest of the six known flavors of quarks
W or Z boson
massive gauge bosons that mediate the weak nuclear interaction
baryon number
one third of the difference between the number of quarks and antiquarks in a system
flavour
type of elementary particles occurring in the Standard Model
spontaneous symmetry breaking
physical phenomenon in which the vacuum expectation value of a field is not invariant under a symmetry of the action, so that a symmetry present at high temperatures is broken at low temperatures
neutrino oscillation
phenomenon in which a neutrino changes lepton flavor as it travels
Higgs mechanism
mechanism in quantum field theory in which spontaneous symmetry breaking causes gauge bosons to acquire mass
hypercharge
In particle physics, the hypercharge (a portmanteau of hyperonic and charge) Y of a particle is a quantum number conserved under the strong interaction. The concept of hypercharge provides a single charge operator that accounts for properties of isospin, electric charge, and flavour. The hypercharge is useful to classify hadrons; the similarly named weak hypercharge has an analogous role in the electroweak interaction.
weak isospin
quantum number of elementary particles
weak hypercharge
quantum number relating the electric charge and the third component of weak isospin
hierarchy problem
why is gravity weaker, compared to other fundamental forces
Cabibbo–Kobayashi–Maskawa matrix
3×3 unitary matrix relating the mass eigenbasis of the three generations of quarks to the basis under which the weak interactions diagonalize
quark model
Classification scheme of hadrons
Pontecorvo–Maki–Nakagawa–Sakata matrix
3×3 unitary mixing matrix that relates the flavor basis of the neutrinos to the mass eigenbasis
symmetry breaking
effect or phenomenon that is not invariant under a presumed or approximate symmetry of a physical system
anomalous magnetic dipole moment
quantum field-theoretic differences of magnetic properties than expected from classical theories
Yukawa interaction
interaction in particle physics
Gell-Mann–Nishijima formula
An Exceptionally Simple Theory of Everything
preprint

vacuum expectation value
expectation value of a local operator at a vacuum of a quantum field theory, whose nonzero value may effect the Higgs mechanism
G-parity
In particle physics, G-parity is a multiplicative quantum number that results from the generalization of C-parity to multiplets of particles.
neutrinoless double beta decay
nuclear physics process that has not been observed yet
X
term in particle physics
neutral particle oscillation
quantum mechanical transmutation of neutral particles
GIM mechanism
mechanism in the standard model through which flavour-changing neutral currents are suppressed in loop diagrams
flavor-changing neutral current
interactions between elementary particles that change a particle’s flavor without changing its electric charge