theorem 12.75 The canonical commutation relation admits no bounded solution
open in the book ·
parts/02-mathematical-methods/10-hilbert-spaces.tex:2047
· p. 435
Rests on
-
depends_on
definition 12.35
Bounded operator; operator norm
¶
-
depends_on
definition 5.37
Linear transformation
¶
-
depends_on
definition 4.33
Vector space
¶
-
depends_on
definition 4.8
Commutativity; abelian structure
¶
- depends_on definition 4.4 Internal binary operation; magma ¶
- depends_on definition 4.32 Field ¶
- depends_on definition 4.31 Module ¶
-
depends_on
definition 4.8
Commutativity; abelian structure
¶
-
depends_on
definition 4.33
Vector space
¶
-
depends_on
definition 5.19
Norm
¶
- depends_on definition 4.33 Vector space ¶ ↺
-
depends_on
definition 5.37
Linear transformation
¶
-
depends_on
proposition 12.37
$\mathcal{B}(\mathcal{H})$ is a Banach algebra
¶
- depends_on definition 12.35 Bounded operator; operator norm ¶ ↺
-
depends_on
proposition 12.8
Absolutely convergent series test
¶
- depends_on definition 5.19 Norm ¶ ↺
- depends_on definition 6.27 Convergence; Cauchy sequence; completeness ¶
- proves proof ch:10-hilbert-spaces@proof-4 ¶
- proves proof ch:10-hilbert-spaces@proof-19 ¶
- proves proof ch:10-hilbert-spaces@proof-37 ¶
Supports
- depends_on corollary 12.76 Position and momentum are unbounded, and cannot be everywhere defined ¶
- depends_on corollary 25.30 The relation cannot be realized by matrices ¶
-
depends_on
definition 12.109
Weyl system
¶
- depends_on corollary 12.112 Commutator of the momentum with a function of the position ¶
-
depends_on
definition A.580
Weyl operator
¶
-
depends_on
definition A.585
The Gaussian average of the Weyl operators
¶
-
depends_on
theorem A.587
The Gaussian average is a non-zero projector that
absorbs the Weyl operators
¶
- depends_on lemma A.590 The Gram matrix is universal ¶
- depends_on proposition A.589 Cyclic subspaces and the rank of the average ¶
- depends_on proposition A.592 The vacuum of the Schrödinger system ¶
-
depends_on
theorem A.587
The Gaussian average is a non-zero projector that
absorbs the Weyl operators
¶
-
depends_on
lemma A.581
Composition law
¶
-
depends_on
lemma A.582
Joint strong continuity
¶
- depends_on lemma A.583 Absolutely convergent operator-valued integrals ¶
- depends_on lemma A.590 The Gram matrix is universal ¶ ↺
-
depends_on
lemma A.582
Joint strong continuity
¶
-
depends_on
definition A.585
The Gaussian average of the Weyl operators
¶
-
depends_on
example 12.110
The Schrödinger system
¶
- depends_on proposition A.592 The vacuum of the Schrödinger system ¶ ↺
- depends_on theorem A.579 Stone–von Neumann ¶
-
depends_on
proposition 12.111
The Weyl relation is a covariance statement
¶
- depends_on corollary 12.112 Commutator of the momentum with a function of the position ¶ ↺
- depends_on theorem A.579 Stone–von Neumann ¶ ↺
- depends_on theorem 12.114 Stone–von Neumann ¶
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 |
→ | Bounded operator; operator norm | declared | parts/02-mathematical-methods/10-hilbert-spaces.tex:2055 |
depends_on |
→ | $\mathcal{B}(\mathcal{H})$ is a Banach algebra | declared | parts/02-mathematical-methods/10-hilbert-spaces.tex:2055 |
depends_on |
← | Position and momentum are unbounded, and cannot be everywhere defined | declared | parts/02-mathematical-methods/10-hilbert-spaces.tex:2091 |
depends_on |
← | The relation cannot be realized by matrices | declared | parts/03-classical-mechanics/08-poisson-quantum-bridge.tex:1117 |
depends_on |
← | Weyl system | declared | parts/02-mathematical-methods/10-hilbert-spaces.tex:3009 |
proves |
← | ch:10-hilbert-spaces@proof-37 | declared | parts/02-mathematical-methods/10-hilbert-spaces.tex:2058 |