← Index
Glossary
Symbols
$A(n)$
,
$\d_x$
,
$E\otimes F$
,
$\wh f$
,
$\Gl(E)$
,
$\Gl(n)$
,
$\Hom(E,F)$
,
$\Hom_G(\Psi,\Phi)$
,
$\Hom_G(\Psi)$
,
$L_2(G)$
,
$\bar\Q$
,
$\OO(n)$
,
$\Q(\z)$
,
$\R_1^{n+1}$
,
$S^1$
,
$S(n)$
,
$\SO(n)$
,
$\SU(n)$
,
$T_xM$
,
$\TT$
,
$\UU(E)$
,
$\UU(n)$
,
$\bar\Z$
,
A
abelianization
,
adjacency matrix
,
algebra
,
algebraic integer
,
algebraic number
,
alternating group
,
angular momentum operator
,
angular momentum operator
,
angular momentum quantum number
,
atomic orbital
,
B
baryon
,
baryon number
,
bipartite graph
,
C
Cayley graph
,
Cayley table
,
character
,
charge
,
class function
,
commutative Lie-algebra
,
commutator
,
commutator
,
compact symplectic group
,
companion matrix
,
complete vector field
,
complex differentiable
,
complexification
,
complex structure
,
compound character
,
configuration space
,
conjugacy class
,
connected manifold
,
contragredient representation
,
center of a group
,
contravariant tensor
,
convolution algebra
,
coordinate-function
,
coordinate transformation
,
covariant tensor
,
critical
,
cyclotomic field
,
D
diagonalizable
,
diffeomorphism
,
dihedral group
,
direct sum of representations
,
Dirac operator
,
dual basis
,
dual of a group
,
dual representation
,
E
eigen-frequency
,
eigen-space
,
eigen-state
,
energy-momentum tensor field
,
equivalent representations
,
Euler-Lagrange equations
,
Euler-Lagrange field equation
,
exchange operator
,
F
faithful representation
,
finitely generated abelian group
,
first integral
,
first quantum number
,
flow of a vector field
,
flow of a vector field
,
Fourier coefficient
,
Fourier transform
,
G
generator
,
generator of a one parameter group
,
ground state
,
group algebra
,
group of symmetries
,
group operation on a space
,
H
hadron
,
Heisenberg group
,
highest weight cyclic representation
,
holomorphic
,
homomorphism
,
hypercharge
,
I
ideal
,
improper rotation
,
induced character
,
induced representation
,
inner product
,
intertwining operator
,
invariant measure
,
invariant subspace
,
irreducible representation
,
irreducible representation
,
irreducible subspace
,
isomorphism
,
isospin
,
isotypic component
,
J
K
L
ladder operator
,
Lagrange density
,
Lagrangian
,
left invariant vectorfield
,
left-regular representation
,
Lie-algebra
,
linear group
,
Lorentz group
,
Lorentz transformation
,
M
magnetic quantum number
,
matrix Lie-group
,
mean value of an abservable
,
meson
,
Minkowski space
,
multipliticity of a representation
,
N
non-singular form
,
normal operator
,
O
observable
,
one-parameter group
,
orbit
,
orbit space
,
P
partial trace
,
partition
,
partition function
,
Pauli spin matrices
,
positive linear operator
,
probability current
,
proper rotation
,
Q
R
related vector fields
,
representation
,
representation of a Lie-algebra
root
root vector
S
SALC
,
self-adjoint operator
,
semisimple Lie-algebra
,
simple algebra
,
simple Lie-algebra
,
simple eigen-value
,
simply connected
,
simultaneously diagonalizable
,
site representation of a molecule
,
skew symmetric operator
,
special orthogonal group
,
special unitary group
,
spin addition
,
spin exchange operator
,
spin $l/2$ representation
,
spherical harmonic
,
square of angular momentum
,
stable state
,
state
,
submanifold
,
subrepresentation
,
symmetric group
,
symplectic form
,
symplectic group
,
symplectic space
,
T
tangent space
,
tensor product of representations
,
time-dependent Schrödinger equation
,
transitive action
,
transposition
,
U
unitary group
,
unitary representation
,
universal property
,
V
variance of an observable
,
variation
,
vector field
,
vector field
,
vector field
,
W
weight
,
weight vector
,
Wirtinger operators
,
X
Y
Z
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Last modified: Thu Sep 1 11:06:37 CEST 2022