Axiom 1 (Local Algebras), curved spacetime #
This file formalises the blueprint declaration
def:local-algebras-in-curved-spacetime (Axiom 1 of the
Haag-Kastler axioms on a Lorentzian spacetime, Chapter 10
(sections/sec10/10-4_haag-kastler-axioms-in-curved-spacetime) of the
AQFT-in-Lean blueprint):
For any basis element
๐of the Alexandrov topology on a Lorentzian spacetimeM, i.e. any set of the formIโบ(p) โฉ Iโป(q), there is a corresponding abstract C*-algebra๐(๐), and when๐is the empty set,๐(โ ) = โ ยท 1.
Main definitions #
Physicslib4.AQFT.HaagKastlerCurved.LocalNet: astructurebundling the data of Axiom 1 over an abstractLorentzianSpacetimeM.
Modelling notes #
The shape is identical to the Minkowski LocalNet
(def:local-algebras), but with the fixed Minkowski carrier and
Alexandrov-basis predicate replaced by the abstract interface
M : LorentzianSpacetime. The empty-region normalisation
๐(โ
) = โ ยท 1 is encoded by a StarAlgEquiv between the fiber over
โ
and โ.
Axiom 1 (Local Algebras), curved spacetime. The data of a
Haag-Kastler local net on a Lorentzian spacetime M: an assignment,
for every subset B of M (thought of as an Alexandrov-basis set,
with the empty set covering the normalisation ๐(โ
) = โ ยท 1), of a
unital C*-algebra algebra B.
The ๐(โ
) = โ normalisation is captured by the field
emptyEquivComplex exhibiting a StarAlgEquiv between algebra โ
and โ.
Blueprint reference: def:local-algebras-in-curved-spacetime.
The C*-algebra
๐(B)assigned to a (would-be Alexandrov-basis) regionB.- instCStarAlgebra (B : Set M.Carrier) : CStarAlgebra (self.algebra B)
The
CStarAlgebrainstance on each fiber๐(B). Normalisation:
๐(โ ) = โ ยท 1, encoded as a*-algebra isomorphismalgebra โ โโโ[โ] โ.
Instances For
The empty-region algebra ๐(โ
) is commutative: it is
*-isomorphic to โ via emptyEquivComplex, so its multiplication
inherits commutativity from โ.
The empty-region algebra ๐(โ
) is one-dimensional over โ.