Non-descriptive name |
Descriptive name(s) |
Explanation/comments |
Concept type |
Bolzano-Weierstrass Theorem |
Sequential compactness theorem, Lion-hunting theorem |
'Lion-hunting' is a reference to one of the ways of proving the theorem |
Theorem |
Rolle's theorem |
Hilltop theorem |
|
Theorem |
Picard-Lindelöf theorem |
Standard ODE theory, Existence and uniqueness theorem |
Lecturers seem to say 'by standard ODE theory there exists a
unique solution' anyway. |
Theorem |
Kakutani Fixed-Point Theorem |
|
I don't have a name for this but just wanted to include a funny name related anecdote. Kakutani
once asked another mathematician at a conference why so many economists attended his talk.
The mathematician replied it was probably because of the Kakutani fixed point theorem. Kakutani was
puzzled and replied "What is the Kakutani fixed point theorem?"
|
Theorem |
Cauchy sequence |
Diametrically shrinking sequence |
Define the Nth diameter to be DN=max{|xm-xn| : m, n > N}. Then
a sequence is Cauchy if DN→0. |
Non-descriptive name |
Descriptive name(s) |
Explanation/comments |
Minkowski metric/spacetime |
Flat metric/spacetime |
|
Levi-civita connection |
Metric connection |
Connection uniquely defined by metric |
Christoffel symbols |
Connection components, geodesic components |
Components appearing in connection/geodesic equation |
Lie derivative |
Fisherman's derivative, flow derivative |
|
Riemannian metric [tensor] |
Metric [tensor] |
|
Riemann curvature tensor |
Curvature tensor (for the frame bundle) |
|
Ricci tensor |
Contracted curvature tensor, metric distortion tensor |
Metric distortion: see Wikipedia page for Ricci tensor, direct geometric meaning |
Ricci scalar |
Scalar curvature |
Already used |
Einstein tensor |
Trace-reversed [Ricci tensor] |
Insert favourite name for [Ricci tensor] |
Bianchi identity |
Conservation of dual field strength/curvature |
|
Ricci identity |
Curvature as commutator of covariant derivatives |
|
Kretschmann scalar |
Quadratic curvature scalar, total curvature |
Total curvature as it is non-zero as long as curvature is non-zero: it is the Yang-Mills functional
term for the Levi-Civita connection.
|
Einstein's field equations |
Gravitational field equations |
|
Killing vector fields |
Isometry generating vector fields/isometry generators |
|
Killing's equation |
Isometry equation |
The equation satisfied by isometry generators |
Non-descriptive name |
Descriptive name(s) |
Explanation/comments |
Concept type |
[Time (in)dependent] Schrödinger equation |
Evolution equation for states, quantum equation of motion, wavefunction equation of motion |
|
Differential equation |
Boson |
Symmetron, Fungible particles |
Symmetric under transposition of particles. They are fungible, that is, any two bosons with the same wavefunction
are indistinguishable.
|
Physical object |
Fermion |
Signon, Non-fungible particles |
Permutations act on multiparticle systems in the sign representation.
|
Physical object |
Non-descriptive name |
Descriptive name(s) |
Explanation/comments |
Klein-Gordon Equation |
Free Field Equation (for a real scalar field) |
|
Scalar Yukawa Theory |
Scalar real/complex coupling |
|
Yukawa interactions |
Scalar-fermion coupling |
|
Second Quantisation |
Occupation representation |
Comes from the mistaken belief that
the solution to the
Dirac equation described a wavefunction, and so was a
'second quantisation' of an already quantum wavefunction. But
the current understanding is that a classical field is
quantised to give the Dirac fermion field, hence would be a
first quantisation of a field, written in terms of occupation
numbers of points of the field.
|
Non-linear sigma model |
Manifold model, coset model |
The sigma or σ comes from a field which emerges from the model but is not a feature of such
models that current research is interested in. The field takes values in a manifold which is often
a homogeneous space G/H.
|
Mandelstam variables |
Channel variables |
s, t and u correspond to different channels in 2-to-2 scattering.
|
Terminology from the Advanced Quantum Field Theory course in Part III.
Non-descriptive name |
Descriptive name(s) |
Explanation/comments |
Grassmann variable/Grassmann number |
Anticommuting number; supernumber; exterior element |
First two names are already in use according to wikipedia. Exterior element is own terminology, as
Grassmann variables are really associated to generators of an exterior algebra, that is, basis
vectors of a generating vector space.
|
Berezin integral |
Superintegral |
An integral over the odd or 'fermionic' part of superspace |
LSZ (Lehmann, Symanzik, Zimmermann) reduction formula |
S-matrix/correlator/vertex function correspondence |
The reduction formula makes precise why we are interested in calculating correlators |
Wavefunction renormalisation |
Field renormalisation |
Vestige from when physicists still thought quantum fields could be interpreted as wavefunctions,
which also gave notation like `second quantisation'.
|
Wick rotation |
Complex coordinate rotation |
|
Feynman diagrams |
Interaction diagrams |
|
Landau pole |
Coupling pole |
Scale at which coupling constant becomes infinite |
Callan-Symanzik equation |
Renormalisation differential equation (for correlators) |
|
Schwinger-Dyson equations |
QFT/functional EOM (equations of motion) |
QFT analogue of Euler-Lagrange equations |
Ward-Takahashi identity |
Correlator Noether identity |
Yes, yes, there is still a name, but Noether is so tied to this idea of symmetry-conservation
correspondence. Really we'd have to go back and rename Noether's theorem.
|
Yang-Mills Theory (Lagrangian) |
Curvature minimising; G-Electromagnetism (G for Lie Group, often G = SU(N)) |
G-Electromagnetism as Yang-Mills theory is a generalisation of electromagnetism,
from U(1) to a general smooth group G, although this is somewhat unsatisfying as Yang-Mills theory
is often qualitatively different, for example having self-interactions. 'Curvature minimising' as
least action is achieved when some notion of total curvature is minimised.
|
Wilson lines |
(Trace of the) holonomy |
This is already the used terminology in maths |
Faddeev-Popov ghosts (or procedure) |
Gauge ghosts, ghosting procedure |
|
BRST quantisation |
Ghost SUSY quantisation |
|
Non-descriptive name |
Descriptive name(s) |
Explanation/comments |
Baker-Campbell-Hausdorff (BCH) formula |
Exponential formula for [Lie algebras] |
|
Killing form |
(Adjoint) trace form |
An example of general trace forms, which can be defined on any representation ρ |
Chern-Simons forms |
Characteristic (class) forms |
This is their name in Chern and Simons original paper |
Cartan Sub-algebra |
Maximally ad-diagonalisable subalgebra |
Cartan-Weyl basis |
Charge-root basis |
|
Poincaré group |
ISO(p,q) |
Isometries of flat space with a metric of signature (p,q) |
(Generalised) Gell-Mann matrices/basis |
Standard real SU(N) basis |
The real is an important qualifier here: this basis preserves SU(N) as a real Lie algebra. As a
complexified Lie algebra a much more standard basis is the one of unit matrices
(with 1 in a single entry, 0 elsewhere).
|
Here we rename a concept after its creator, and see how disastrous the consequences are.