Documentation

QuantumInfo.Finite.ResourceTheory.ResourceTheory

class ResourceTheory (ι : Type u_1) extends FreeStateTheory ι :
Type (max u_1 (u_2 + 1))

A quantum resource theory extends a FreeStateTheory with a collection of free operations. It is required that any state we can always prepare for free must be free, and this is all then the resource theory is "minimal", but we can have a more restricted set of operations.

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    Given a FreeStateTheory, there is a maximal set of free operations compatible with the free states. That is the set of all operations that don't generate non-free states from free states. We call this the maximal resource theory.

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      A resource theory IsMaximal if it includes all non-generating operations.

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        A resource theory IsTensorial if it includes tensor products of operations, creating free states, and discarding. This implies that includes a unit object.

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          def ResourceTheory.mk_of_ops {ι : Type u_1} [ResourcePretheory ι] (O : (i j : ι) → Set (CPTPMap (ResourcePretheory.H i) (ResourcePretheory.H j))) (h_id : ∀ (i : ι), CPTPMap.id O i i) (h_comp : ∀ {i j k : ι} (Y : (O j k)) (X : (O i j)), (↑Y).compose X O i k) (h_closed : ∀ {i j : ι}, IsClosed (O i j)) (h_convex : ∀ {i j : ι}, Convex (CPTPMap.choi '' O i j)) (h_prod : ∀ {i j k l : ι} {f : CPTPMap (ResourcePretheory.H i) (ResourcePretheory.H k)} {g : CPTPMap (ResourcePretheory.H j) (ResourcePretheory.H l)}, f O i kg O j lResourcePretheory.prodCPTPMap f g O (ResourcePretheory.prod i j) (ResourcePretheory.prod k l)) (h_fullRank : {i : ι} → sorry) (h_appendFree : {i j k : ι} → sorry) :

          A ResourceTheory can be constructed from a set of operations (satisfying appropriate axioms of closure), and then the free states are taken to be the set of states that can be prepared from any initial state.

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            The 'fully free' quantum resource theory: the category is all finite Hilbert spaces, all maps are free and all states are free. Marked noncomputable because we assume that all types have DecidableEq.

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