roseking's picture
Add lean source and binary files (part 91)
caec230 verified
Raw History Blame Contribute Delete
7.88 kB
import Mathlib
namespace OAI
noncomputable section
open scoped BigOperators ComplexOrder Matrix.Norms.L2Operator MatrixOrder
open Matrix
noncomputable section
open scoped BigOperators ComplexOrder
namespace PolynomialPEPS.PhysicalMove
abbrev Vertex (L : ℕ) := Fin L × Fin L
def ForwardAdjacent {L : ℕ} (v w : Vertex L) : Prop :=
(v.1.val + 1 = w.1.val ∧ v.2 = w.2) ∨
(v.1 = w.1 ∧ v.2.val + 1 = w.2.val)
abbrev Edge (L : ℕ) := {e : Vertex L × Vertex L // ForwardAdjacent e.1 e.2}
instance edgeFintype (L : ℕ) : Fintype (Edge L) := Fintype.ofFinite _
def Incident {L : ℕ} (v : Vertex L) (e : Edge L) : Prop :=
v = e.val.1 ∨ v = e.val.2
abbrev IncidentEdge {L : ℕ} (v : Vertex L) := {e : Edge L // Incident v e}
instance incidentFintype {L : ℕ} (v : Vertex L) : Fintype (IncidentEdge v) :=
Fintype.ofFinite _
abbrev Configuration (L q : ℕ) := Vertex L → Fin q
abbrev State (L q : ℕ) := EuclideanSpace ℂ (Configuration L q)
abbrev Operator (L q : ℕ) := Matrix (Configuration L q) (Configuration L q) ℂ
abbrev RegionConfiguration {L : ℕ} (q : ℕ) (S : Finset (Vertex L)) :=
{v : Vertex L // v ∈ S} → Fin q
def liftLocal {L q : ℕ} (S : Finset (Vertex L))
(a : Matrix (RegionConfiguration q S) (RegionConfiguration q S) ℂ) :
Operator L q := fun x y =>
if ∀ v, v ∉ S → x v = y v then
a (fun v => x v.val) (fun v => y v.val)
else 0
def SupportedOn {L q : ℕ} (a : Operator L q) (S : Finset (Vertex L)) : Prop :=
∃ aS : Matrix (RegionConfiguration q S) (RegionConfiguration q S) ℂ,
a = liftLocal S aS
def EdgeSites {L : ℕ} (e : Edge L) : Finset (Vertex L) := {e.val.1, e.val.2}
def Hamiltonian {L q : ℕ} (hv : Vertex L → Operator L q)
(he : Edge L → Operator L q) : Operator L q :=
(∑ v, hv v) + ∑ e, he e
def asMap {L q : ℕ} (a : Operator L q) : State L q →L[ℂ] State L q :=
Matrix.toEuclideanCLM (n := Configuration L q) (𝕜 := ℂ) a
def opNorm {L q : ℕ} (a : Operator L q) : ℝ := ‖asMap a‖
def IsGridHamiltonian {L q : ℕ} (J : ℝ)
(hv : Vertex L → Operator L q) (he : Edge L → Operator L q) : Prop :=
(∀ v, SupportedOn (hv v) {v} ∧ opNorm (hv v) ≤ J) ∧
(∀ e, SupportedOn (he e) (EdgeSites e) ∧ opNorm (he e) ≤ J) ∧
(Hamiltonian hv he).IsHermitian
def phase (θ : ℝ) : ℂ := Complex.exp ((θ : ℂ) * Complex.I)
def UniqueGround {L q : ℕ} (H : Operator L q) (Ω : State L q) (E₀ : ℝ) : Prop :=
‖Ω‖ = 1 ∧
asMap H Ω = (E₀ : ℂ) • Ω ∧
(∀ ψ : State L q,
E₀ * ‖ψ‖ ^ 2 ≤ (inner ℂ ψ (asMap H ψ)).re) ∧
(∀ ψ : State L q, ‖ψ‖ = 1 →
asMap H ψ = (E₀ : ℂ) • ψ →
∃ θ : ℝ, ψ = phase θ • Ω)
def FullSystemGap {L q : ℕ} (H : Operator L q) (Ω : State L q)
(E₀ Δ : ℝ) : Prop :=
∀ ψ : State L q,
Δ * (‖ψ‖ ^ 2 - ‖inner ℂ Ω ψ‖ ^ 2) ≤
(inner ℂ ψ (asMap H ψ)).re - E₀ * ‖ψ‖ ^ 2
abbrev LocalTensor {L : ℕ} (q : ℕ) (D : Edge L → ℕ) (v : Vertex L) :=
Fin q → ((e : IncidentEdge v) → Fin (D e.val)) → ℂ
def contractPEPS {L q : ℕ} (D : Edge L → ℕ)
(A : (v : Vertex L) → LocalTensor q D v) : State L q :=
WithLp.toLp 2 (fun x => ∑ a : (e : Edge L) → Fin (D e),
∏ v : Vertex L, A v (x v) (fun e => a e.val))
def HasPEPSApproximation {L q : ℕ} (Ω : State L q) (C c : ℝ) : Prop :=
∃ (D : Edge L → ℕ) (A : (v : Vertex L) → LocalTensor q D v),
(∀ e, 0 < D e) ∧
(∀ e, (D e : ℝ) ≤ C * Real.rpow (L : ℝ) c) ∧
contractPEPS D A ≠ 0 ∧
∃ θ : ℝ,
‖((‖contractPEPS D A‖⁻¹ : ℝ) : ℂ) • contractPEPS D A - phase θ • Ω‖ ≤
(L : ℝ)⁻¹
def MainStatement : Prop :=
∀ (q : ℕ), 2 ≤ q → ∀ (J Δ : ℝ), 0 < J → 0 < Δ →
∃ C c : ℝ, 0 < C ∧ 0 < c ∧
∀ (L : ℕ), 2 ≤ L →
∀ (hv : Vertex L → Operator L q) (he : Edge L → Operator L q)
(Ω : State L q) (E₀ : ℝ),
IsGridHamiltonian J hv he →
UniqueGround (Hamiltonian hv he) Ω E₀ →
FullSystemGap (Hamiltonian hv he) Ω E₀ Δ →
HasPEPSApproximation Ω C c
end PolynomialPEPS.PhysicalMove
namespace PolynomialPEPS.PhysicalMove
def joinConfigurations {L q : ℕ} (A : Finset (Vertex L))
(x : RegionConfiguration q A) (z : RegionConfiguration q Aᶜ) :
Configuration L q := by
classical
exact fun v => if h : v ∈ A then x ⟨v, h⟩ else z ⟨v, Finset.mem_compl.mpr h⟩
def coefficientMatrix {L q : ℕ} (Ω : State L q) (A : Finset (Vertex L)) :
Matrix (RegionConfiguration q A) (RegionConfiguration q Aᶜ) ℂ :=
fun x z => Ω (joinConfigurations A x z)
def reducedDensity {L q : ℕ} (Ω : State L q) (A : Finset (Vertex L)) :
Matrix (RegionConfiguration q A) (RegionConfiguration q A) ℂ :=
coefficientMatrix Ω A * (coefficientMatrix Ω A).conjTranspose
theorem reducedDensity_isHermitian {L q : ℕ} (Ω : State L q)
(A : Finset (Vertex L)) : (reducedDensity Ω A).IsHermitian := by
exact Matrix.isHermitian_mul_conjTranspose_self _
def vonNeumannEntropy {L q : ℕ} (Ω : State L q) (A : Finset (Vertex L)) : ℝ :=
∑ i, Real.negMulLog ((reducedDensity_isHermitian Ω A).eigenvalues i)
def boundaryCard {L : ℕ} (A : Finset (Vertex L)) : ℕ := by
classical
exact Fintype.card {e : Edge L //
(e.val.1 ∈ A ∧ e.val.2 ∉ A) ∨ (e.val.1 ∉ A ∧ e.val.2 ∈ A)}
def UniformAreaLaw : Prop :=
∀ (q : ℕ), 2 ≤ q → ∀ (J Δ : ℝ), 0 < J → 0 < Δ →
∃ C_A : ℝ, 0 < C_A ∧
∀ (L : ℕ), 2 ≤ L →
∀ (hv : Vertex L → Operator L q) (he : Edge L → Operator L q)
(Ω : State L q) (E₀ : ℝ),
IsGridHamiltonian J hv he →
UniqueGround (Hamiltonian hv he) Ω E₀ →
FullSystemGap (Hamiltonian hv he) Ω E₀ Δ →
∀ A : Finset (Vertex L),
vonNeumannEntropy Ω A ≤ C_A * (boundaryCard A : ℝ)
end PolynomialPEPS.PhysicalMove
end
end
end OAI