definition 14.5 Universal enveloping algebra
open in the book ·
parts/02-mathematical-methods/12-lie-groups-fibre-bundles.tex:281
· p. 544
- ground object -- no derivation owed
Rests on
-
depends_on
equation 14.5
eq:lie-structconst
¶
-
step_from
equation 14.4
eq:lie-gengrlie
¶
- step_from equation 14.3 eq:lie-generators ¶
- step_from equation 14.2 eq:lie-varincor ¶
-
step_from
equation 14.4
eq:lie-gengrlie
¶
Supports
-
depends_on
definition A.320
Filtration by degree
¶
-
depends_on
definition A.325
Symmetric algebra and symbol
¶
- depends_on corollary A.328 The Casimir elements are not accidentally zero ¶
-
depends_on
definition A.326
Symmetrization
¶
-
depends_on
proposition A.327
Symmetrization is an isomorphism of
$\mathfrak{g}$-modules
¶
- depends_on proposition A.348 Symmetrization identifies the invariants ¶
-
depends_on
proposition A.327
Symmetrization is an isomorphism of
$\mathfrak{g}$-modules
¶
- depends_on lemma A.349 Lifting generators through the filtration ¶
- depends_on proposition A.327 Symmetrization is an isomorphism of $\mathfrak{g}$-modules ¶ ↺
- depends_on proposition A.348 Symmetrization identifies the invariants ¶ ↺
- depends_on lemma A.321 The ordered monomials span ¶
-
depends_on
definition A.325
Symmetric algebra and symbol
¶
- depends_on definition A.326 Symmetrization ¶ ↺
-
depends_on
definition 14.8
Casimir element
¶
-
depends_on
corollary 14.18
A Casimir acts as a number on an irreducible
representation
¶
-
depends_on
proposition 14.55
The fundamental, the antifundamental and the adjoint
¶
- depends_on corollary A.377 The adjoint representation is irreducible ¶
- depends_on example A.358 Rank two: $\mathfrak{su}(3)$ ¶
-
depends_on
theorem 14.57
$\vect{3}\otimes\bar{\vect{3}}
= \vect{1}\oplus\vect{8}$
¶
- depends_on proposition 102.6 Mesons are $q\bar{q}$, baryons are $qqq$ ¶
-
depends_on
theorem 102.12
Which quark combinations can be colour singlets
¶
- depends_on corollary 102.13 The selection rule of the eightfold way ¶
- depends_on theorem A.354 Harish-Chandra, quoted: the labels separate ¶
-
depends_on
proposition 14.55
The fundamental, the antifundamental and the adjoint
¶
-
depends_on
lemma A.347
Central is the same as invariant
¶
- depends_on proposition A.348 Symmetrization identifies the invariants ¶ ↺
- depends_on lemma 14.87 A rescaled Casimir stays central ¶
-
depends_on
proposition 14.60
The quadratic invariant
¶
- depends_on theorem 14.65 The two Casimir operators of the Poincaré algebra in $3+1$ dimensions ¶
-
depends_on
theorem A.346
Racah
¶
- depends_on example A.359 The Lorentz algebra ¶
- depends_on example A.357 Rank one: $\mathfrak{su}(2)$ ¶
- depends_on example A.358 Rank two: $\mathfrak{su}(3)$ ¶ ↺
- depends_on theorem A.354 Harish-Chandra, quoted: the labels separate ¶ ↺
-
depends_on
theorem 14.16
Invariant tensors give Casimir operators
¶
- depends_on corollary A.328 The Casimir elements are not accidentally zero ¶ ↺
-
depends_on
corollary 14.17
The quadratic Casimir
¶
-
depends_on
lemma 14.41
Ladder algebra
¶
- depends_on proposition 14.44 Existence: every allowed $j$ is realized ¶
- depends_on theorem 14.43 The irreducible representations of $\mathfrak{su}(2)$ ¶
-
depends_on
proposition 14.54
The two Casimir operators of $\mathfrak{su}(3)$
¶
- depends_on example A.358 Rank two: $\mathfrak{su}(3)$ ¶ ↺
-
depends_on
lemma 14.41
Ladder algebra
¶
- depends_on proposition 14.54 The two Casimir operators of $\mathfrak{su}(3)$ ¶ ↺
-
depends_on
theorem 14.21
Racah
¶
-
depends_on
proposition 14.22
The rank of $\mathfrak{so}(p,q)$
¶
-
depends_on
lemma 14.68
The algebra fixing a timelike momentum
¶
- depends_on definition A.384 The mass shell and the standard momentum ¶
- depends_on lemma A.386 The little group ¶
- depends_on theorem A.385 Labels of a massive representation ¶
-
depends_on
lemma 14.68
The algebra fixing a timelike momentum
¶
- depends_on proposition 14.54 The two Casimir operators of $\mathfrak{su}(3)$ ¶ ↺
- depends_on theorem A.385 Labels of a massive representation ¶ ↺
-
depends_on
proposition 14.22
The rank of $\mathfrak{so}(p,q)$
¶
-
depends_on
corollary 14.18
A Casimir acts as a number on an irreducible
representation
¶
- depends_on lemma A.347 Central is the same as invariant ¶ ↺
-
depends_on
theorem A.319
Poincaré–Birkhoff–Witt
¶
- depends_on corollary A.328 The Casimir elements are not accidentally zero ¶ ↺
- depends_on definition A.325 Symmetric algebra and symbol ¶ ↺
- depends_on proposition A.327 Symmetrization is an isomorphism of $\mathfrak{g}$-modules ¶ ↺
- depends_on theorem 14.16 Invariant tensors give Casimir operators ¶ ↺
-
depends_on
theorem 14.7
Poincaré–Birkhoff–Witt
¶
- depends_on lemma 14.87 A rescaled Casimir stays central ¶ ↺
Neighborhood
Every logical edge within two steps of this node.
- declared and complete
- partly declared
- a check failed
- not graded
- declared in the source
- inferred from structure
Edges
| type | direction | node | provenance | where |
|---|---|---|---|---|
depends_on |
→ | eq:lie-structconst | declared | parts/02-mathematical-methods/12-lie-groups-fibre-bundles.tex:297 |
depends_on |
← | Filtration by degree | declared | appendices/A-long-proofs.tex:15678 |
depends_on |
← | Symmetrization | declared | appendices/A-long-proofs.tex:16005 |
depends_on |
← | Casimir element | declared | parts/02-mathematical-methods/12-lie-groups-fibre-bundles.tex:339 |
depends_on |
← | Central is the same as invariant | declared | appendices/A-long-proofs.tex:16937 |
depends_on |
← | Poincaré–Birkhoff–Witt | declared | appendices/A-long-proofs.tex:15662 |
depends_on |
← | Invariant tensors give Casimir operators | declared | parts/02-mathematical-methods/12-lie-groups-fibre-bundles.tex:490 |
depends_on |
← | Poincaré–Birkhoff–Witt | declared | parts/02-mathematical-methods/12-lie-groups-fibre-bundles.tex:319 |