Ontological models as functors Andru Gheorghiu Chris Heunen - - PowerPoint PPT Presentation

ontological models as functors
SMART_READER_LITE
LIVE PREVIEW

Ontological models as functors Andru Gheorghiu Chris Heunen - - PowerPoint PPT Presentation

Ontological models as functors Andru Gheorghiu Chris Heunen arXiv:1905.09055 1 / 20 (Finite-dimensional) Quantum theory unit vector in | H, | 2 = 1 state complex Hilbert space uu = u u = 1 transformation


slide-1
SLIDE 1

Ontological models as functors

Andru Gheorghiu Chris Heunen arXiv:1905.09055

1 / 20

slide-2
SLIDE 2

(Finite-dimensional) Quantum theory

state unit vector in complex Hilbert space |ψ ∈ H, |ψ2 = 1 transformation unitary operator uu† = u†u = 1 composition tensor product HAB = HA ⊗ HB

  • bservation
  • rthonormal basis

{|i}, i | j = δij

2 / 20

slide-3
SLIDE 3

Ontological interpretation

Are quantum states real?

3 / 20

slide-4
SLIDE 4

Ontological interpretation

Are quantum states real? Hilbert space − →

  • ntic (measurable) space

H − → (Λ, ΣΛ)

3 / 20

slide-5
SLIDE 5

Ontological interpretation

Are quantum states real? Hilbert space − →

  • ntic (measurable) space

H − → (Λ, ΣΛ) |ψ − → Λ µψ

3 / 20

slide-6
SLIDE 6

Ontological interpretation

state |ψ − → probability measure µψ : ΣΛ → [0, 1]

4 / 20

slide-7
SLIDE 7

Ontological interpretation

state |ψ − → probability measure µψ : ΣΛ → [0, 1] measurement {|i}1≤i≤dim(H) − → response function ξi : Λ → [0, 1]

4 / 20

slide-8
SLIDE 8

Ontological interpretation

state |ψ − → probability measure µψ : ΣΛ → [0, 1] measurement {|i}1≤i≤dim(H) − → response function ξi : Λ → [0, 1]

  • Λ ξi(λ)dµψ(λ)) = |i | ψ|2

4 / 20

slide-9
SLIDE 9

Ontological interpretation

state |ψ − → probability measure µψ : ΣΛ → [0, 1] measurement {|i}1≤i≤dim(H) − → response function ξi : Λ → [0, 1]

  • Λ ξi(λ)dµψ(λ)) = |i | ψ|2

∀λ ∈ Λ: dim(H)

i=1

ξi = 1

4 / 20

slide-10
SLIDE 10

Ontological interpretation

0 < |ψ|φ| < 1 − → Λ µψ µφ

5 / 20

slide-11
SLIDE 11

Ontological interpretation

0 < |ψ|φ| < 1 − → Λ µψ µφ Epistemic model

5 / 20

slide-12
SLIDE 12

Ontological interpretation

0 < |ψ|φ| < 1 − → Λ µψ µφ Epistemic model “Quantum state is state of knowledge about underlying ontic reality”

5 / 20

slide-13
SLIDE 13

Ontological interpretation

0 < |ψ|φ| < 1 − → Λ µψ µφ Epistemic model (otherwise ontic model) “Quantum state is state of knowledge about underlying ontic reality” [Leifer arXiv:1409.1570]

5 / 20

slide-14
SLIDE 14

No-go results for epistemic models

◮ [Pusey-Barrett-Rudolph arXiv:1111.3328] Preparation independence: {|ψ ⊗ |φ}ψ∈HA,φ∈HB → (ΛA × ΛB, ΣΛA ⊗ ΣΛB) µψ⊗φ = µψ ⊗ µφ

6 / 20

slide-15
SLIDE 15

No-go results for epistemic models

◮ [Pusey-Barrett-Rudolph arXiv:1111.3328] Preparation independence: {|ψ ⊗ |φ}ψ∈HA,φ∈HB → (ΛA × ΛB, ΣΛA ⊗ ΣΛB) µψ⊗φ = µψ ⊗ µφ ◮ [Leifer-Maroney arXiv:1208.5132] Maximally epistemic: ∀|ψ, |φ: |ψ|φ|2 =

  • supp(µφ) dµψ(λ)

6 / 20

slide-16
SLIDE 16

No-go results for epistemic models

◮ [Pusey-Barrett-Rudolph arXiv:1111.3328] Preparation independence: {|ψ ⊗ |φ}ψ∈HA,φ∈HB → (ΛA × ΛB, ΣΛA ⊗ ΣΛB) µψ⊗φ = µψ ⊗ µφ ◮ [Leifer-Maroney arXiv:1208.5132] Maximally epistemic: ∀|ψ, |φ: |ψ|φ|2 =

  • supp(µφ) dµψ(λ)

◮ [Aaronson-Bouland-Chua-Lowther arXiv:1303.2834] Symmetric and maximally nontrivial: Λ = H u|ψ = ψ = ⇒ µuψ(uλ) = µψ(λ) ∀|ψ, |φ: |ψ|φ|2 > 0 ⇐ ⇒

  • supp(µψ) dµφ(λ) > 0

6 / 20

slide-17
SLIDE 17

No-go results for epistemic models

◮ [Pusey-Barrett-Rudolph arXiv:1111.3328] Preparation independence: {|ψ ⊗ |φ}ψ∈HA,φ∈HB → (ΛA × ΛB, ΣΛA ⊗ ΣΛB) µψ⊗φ = µψ ⊗ µφ ◮ [Leifer-Maroney arXiv:1208.5132] Maximally epistemic: ∀|ψ, |φ: |ψ|φ|2 =

  • supp(µφ) dµψ(λ)

◮ [Aaronson-Bouland-Chua-Lowther arXiv:1303.2834] Symmetric and maximally nontrivial: Λ = H u|ψ = ψ = ⇒ µuψ(uλ) = µψ(λ) ∀|ψ, |φ: |ψ|φ|2 > 0 ⇐ ⇒

  • supp(µψ) dµφ(λ) > 0

◮ [Gheorghiu-Heunen arXiv:1905.09055]:

  • ne approach to rule them all

6 / 20

slide-18
SLIDE 18

Category theory

Explicitly invented to translate structure between different areas: ◮ Algebraic topology: topology → groups ◮ Algebraic geometry: varieties → schemes ◮ Logic: theories → models ◮ Computer compilers: high-level language → assembly ◮ Complexity theory: algorithm → function ◮ Semantics: computer programs → mathematical model ◮ Physics: physical systems → mathematical abstractions Here: quantum physics → statistical physics

7 / 20

slide-19
SLIDE 19

Categorical approach

HA HB HC M N N ◦ M FHilb

8 / 20

slide-20
SLIDE 20

Categorical approach

HA HB HC M N N ◦ M FHilb bounded linear maps Hilbert space

8 / 20

slide-21
SLIDE 21

Categorical approach

(XA, ΣA) (XB, ΣB) (XC, ΣC) g f g ◦ f BoRel

8 / 20

slide-22
SLIDE 22

Categorical approach

(XA, ΣA) (XB, ΣB) (XC, ΣC) g f g ◦ f BoRel Markov kernels Borel spaces

8 / 20

slide-23
SLIDE 23

Categorical approach

(XA, ΣA) (XB, ΣB) (XC, ΣC) g f g ◦ f BoRel Borel space: topological measurable space Markov kernels: f : XA × ΣB → [0, 1] f(−, W): XA → [0, 1] bounded measurable f(x, −): ΣB → [0, 1] probability measure

8 / 20

slide-24
SLIDE 24

Categorical approach

HA HB HC M N N ◦ M FHilb (XA, ΣA) (XB, ΣB) (XC, ΣC) g f g ◦ f BoRel functor F

8 / 20

slide-25
SLIDE 25

States

C H |ψ

9 / 20

slide-26
SLIDE 26

States

C H |ψ F

{•}, {∅, {•}}

  • (Λ, ΣΛ)

µψ

9 / 20

slide-27
SLIDE 27

States

C H |ψ F

{•}, {∅, {•}}

  • (Λ, ΣΛ)

µψ F(|ψ)(•, −): ΣΛ → [0, 1] probability measure

9 / 20

slide-28
SLIDE 28

Effects

C H ψ|

10 / 20

slide-29
SLIDE 29

Effects

C H ψ| F

{•}, {∅, {•}}

  • (Λ, ΣΛ)

ξi

10 / 20

slide-30
SLIDE 30

Effects

C H ψ| F

{•}, {∅, {•}}

  • (Λ, ΣΛ)

ξi F(ψ|)(−, {•}): Λ → [0, 1] response function

10 / 20

slide-31
SLIDE 31

Operational category

◮ is monoidal (⊗,I) ◮ has distinguishing object 2 ◮ has set Ω of elements called probabilities ◮ has evaluation −: C(I, 2) → Ω

11 / 20

slide-32
SLIDE 32

Operational category

◮ is monoidal (⊗,I) ◮ has distinguishing object 2 ◮ has set Ω of elements called probabilities ◮ has evaluation −: C(I, 2) → Ω FHilb is operational: ◮ 2 = C2, Ω = [0, 1] ◮ η: C → C2 η = |a|2 if η(1) = (a, b), |a|2 + |b|2 = 1

11 / 20

slide-33
SLIDE 33

Operational category

◮ is monoidal (⊗,I) ◮ has distinguishing object 2 ◮ has set Ω of elements called probabilities ◮ has evaluation −: C(I, 2) → Ω FHilb is operational: ◮ 2 = C2, Ω = [0, 1] ◮ η: C → C2 η = |a|2 if η(1) = (a, b), |a|2 + |b|2 = 1 BoRel is operational: ◮ 2 =

{0, 1}, ∅, {0}, {1}, {0, 1} , Ω = [0, 1]

◮ f : I → 2, f = f(•, {0}) if f(•, {0}) = 1 − f(•, {1})

11 / 20

slide-34
SLIDE 34

Operational model

is functor F : C → D between operational categories satisfying: F(I) = I F(2) = 2 F(η) = η

12 / 20

slide-35
SLIDE 35

Operational model

is functor F : C → D between operational categories satisfying: F(I) = I F(2) = 2 F(η) = η For C = FHilb and D = BoRel:

  • Λ

ξi(λ)dµψ(λ) = |i|ψ|2 F(|ψ) = µψ F(i|) = ξi

12 / 20

slide-36
SLIDE 36

Distinguishability

If C operational category with Ω = [0, 1], Ψ ⊆ C(I, A) collection of states χ: A → 2 measurement, χ distinguishes ψ from Ψ when χ ◦ ψ = 1

  • φ∈Ψ,φ=ψ

χ ◦ φ = 0

13 / 20

slide-37
SLIDE 37

Epistemic operational models

Operational model is epistemic when there are distinct states ψ = φ: I → A such that F(ψ) and F(φ) are not distinguishable

14 / 20

slide-38
SLIDE 38

Epistemic operational models

Operational model is epistemic when there are distinct states ψ = φ: I → A such that F(ψ) and F(φ) are not distinguishable i.e. “distributions overlap”: Λ F(ψ) F(φ)

14 / 20

slide-39
SLIDE 39

Operational vs ontological

◮ operational model is more restrictive ◮ composition needs to be preserved ◮ trivial ontic models can be constructed ◮ not clear whether ontic operational models exist at all

15 / 20

slide-40
SLIDE 40

No-go results: Pusey-Barrett-Rudolph

No epistemic ontological model when: preparation independence {|ψ ⊗ |φ}ψ∈HA,φ∈HB → (ΛA × ΛB, ΣΛA ⊗ ΣΛB) µψ⊗φ = µψ ⊗ µφ

16 / 20

slide-41
SLIDE 41

No-go results: Pusey-Barrett-Rudolph

No epistemic ontological model when: preparation independence {|ψ ⊗ |φ}ψ∈HA,φ∈HB → (ΛA × ΛB, ΣΛA ⊗ ΣΛB) µψ⊗φ = µψ ⊗ µφ Monoidal operational model implies this So cannot have monoidal epistemic operational model!

16 / 20

slide-42
SLIDE 42

No-go results: Leifer-Maroney

No maximally epistemic ontological model ∀|ψ, |φ: |ψ|φ|2 =

  • supp(µφ)

dµψ(λ)

17 / 20

slide-43
SLIDE 43

No-go results: Leifer-Maroney

No maximally epistemic ontological model ∀|ψ, |φ: |ψ|φ|2 =

  • supp(µφ)

dµψ(λ) This is implied when operational model preserves duality: F(ψ†) = F(ψ)† ψ† ◦ φ = F(ψ)† ◦ F(φ)

17 / 20

slide-44
SLIDE 44

No-go results: Leifer-Maroney

No maximally epistemic ontological model ∀|ψ, |φ: |ψ|φ|2 =

  • supp(µφ)

dµψ(λ) This is implied when operational model preserves duality: F(ψ†) = F(ψ)† ψ† ◦ φ = F(ψ)† ◦ F(φ) So cannot have duality preserving operational model!

17 / 20

slide-45
SLIDE 45

No-go results: Aaronson-Bouland-Chua-Lowther

No symmetric epistemic ontological model Λ = H U|ψ = ψ = ⇒ µUψ(Uλ) = µψ(λ) ∀|ψ, |φ: |ψ|φ|2 > 0 ⇐ ⇒

  • supp(µψ)

dµφ(λ) > 0

18 / 20

slide-46
SLIDE 46

No-go results: Aaronson-Bouland-Chua-Lowther

No symmetric epistemic ontological model Λ = H U|ψ = ψ = ⇒ µUψ(Uλ) = µψ(λ) ∀|ψ, |φ: |ψ|φ|2 > 0 ⇐ ⇒

  • supp(µψ)

dµφ(λ) > 0 Implied by equivariance of operational model: M : HA → HB F(M ◦ ψ)(•, U) = F(ψ)(•, M · U) M · U measurable

18 / 20

slide-47
SLIDE 47

No-go results: Aaronson-Bouland-Chua-Lowther

No symmetric epistemic ontological model Λ = H U|ψ = ψ = ⇒ µUψ(Uλ) = µψ(λ) ∀|ψ, |φ: |ψ|φ|2 > 0 ⇐ ⇒

  • supp(µψ)

dµφ(λ) > 0 Implied by equivariance of operational model: M : HA → HB F(M ◦ ψ)(•, U) = F(ψ)(•, M · U) M · U measurable So cannot have equivariant operational model!

18 / 20

slide-48
SLIDE 48

What about a “go” result?

(XA, ΣA) (XB, ΣB) (XC, ΣC) g f g ◦ f QBoRel Borel space: topological measurable space signed Markov kernels: f : XA × ΣB → [−1, 1] f(−, W): XA → [−1, 1] bounded measurable f(x, −): ΣB → [−1, 1] quasi-probability measure

19 / 20

slide-49
SLIDE 49

What about a “go” result?

(XA, ΣA) (XB, ΣB) (XC, ΣC) g f g ◦ f QBoRel Borel space: topological measurable space signed Markov kernels: f : XA × ΣB → [−1, 1] f(−, W): XA → [−1, 1] bounded measurable f(x, −): ΣB → [−1, 1] quasi-probability measure ◮ Possible! In fact monoidal (in odd dimension)! ◮ Wigner functions ◮ quasi-probabilistic epistemic model [Ferrie arXiv:1010.2701]

19 / 20

slide-50
SLIDE 50

Summary

◮ Unify ontological interpretations ◮ Many questions ◮ Can have operational model at all? ◮ What about target category of quantum measures? µ(U ∪ V ) = µ(U) + µ(V ) µ(U ∪ V ∪ W) = µ(U ∪ V ) + µ(V ∪ W) + µ(W ∪ U) − µ(U) − µ(V ) −

20 / 20