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Contextuality, memory cost, and nonclassicality for sequential quantum measurements Costantino Budroni Institute for Quantum Optics and Quantum Information (IQOQI), Austrian Academy of Sciences, Vienna, Austria Winer Memorial Lectures 2018


  1. Contextuality, memory cost, and nonclassicality for sequential quantum measurements Costantino Budroni Institute for Quantum Optics and Quantum Information (IQOQI), Austrian Academy of Sciences, Vienna, Austria Winer Memorial Lectures 2018

  2. Outline ◮ Motivation: ◮ Kochen-Specker from logical contradiction to experimental tests ◮ Operational definitions of contextuality? ◮ Contextuality and sequential measurements ◮ Memory cost, temporal correlations, applications ◮ Temporal correlations in C/Q/GPT (unconstrained case) ◮ Memory restriction and finite-state machines ◮ Temporal bounds for C/Q/GPT correlations in the simplest scenario ◮ Conclusions and outlook

  3. Kochen-Specker contextuality 13 12 10 7 5 3 14 9 8 1 6 4 11 2 Hilbert space of dimension d ≥ 3, for each set of d orthogonal directions ( a context ), we associated 1-dim projections P 1 , . . . , P d , s.t. O P i P j = 0 if i � = j (Orthogonality); C � i P i = 1 1(Completeness). Kochen-Specker considered 117 directions in d = 3, each direction will appear in several sets.

  4. Kochen-Specker contextuality 13 12 10 7 5 3 14 9 8 1 6 4 11 2 We interpret each projection as a proposition, we want to assign a “truth value” s.t. in each context P 1 , . . . , P d : O’ P i and P j cannot be both “true” for i � = j ; C’ P 1 , . . . , P d they cannot be all “false”. We want the assignment to be context-independent.

  5. Kochen-Specker contextuality 13 12 10 7 5 3 9 14 8 1 6 4 11 2 Kochen-Specker Th. (1967): Such an assignment is impossible 1 . 1 S. Kochen and E. P. Specker, J. Math. Mech. 17, 59 (1967)

  6. Kochen-Specker contextuality Initial approach ◮ Truth-value assignements to propositions associated with projectors, with O and C rules: Logical impossibility proof. ◮ No operational approach: what to measure? How to identify the “same measurement” in “different contexts”? ◮ Not clear whether this was experimetnally testable at all. ◮ Can we pass from logical argument to statistical one and test contextuality in the lab?

  7. Experimental tests of contextuality Possible operational definition: ◮ Each context corresponds to a measurement (PVM) M = { P i } i ◮ We want to identify effects in different contexts, e.g., i ∈ M ′ with P i = P ′ P i ∈ M , P ′ i . ◮ In QM: P i = P ′ i ⇔ tr[ ρ P i ] = tr[ ρ P ′ i ] for all states ρ . ◮ We extract an operational rule for identifying “the same effect in different contexts”: same statistics ⇒ same effect.

  8. Experimental tests of contextuality Possible operational definition: Measurement noncontextuality 2 : ξ ( k | λ, M ) = ξ ( k | λ, M ′ ) ∀ λ if p ( k |P , M ) = p ( k |P , M ′ ) ∀P Where classical theories compute probabilities as � p ( k |P , M ) := µ ( λ |P ) ξ ( k | λ, M ) λ 2 R. W. Spekkens, Phys. Rev. A 71 (2005)

  9. Experimental tests of contextuality Measurement noncontextuality ξ ( k | λ, M ) = ξ ( k | λ, M ′ ) ∀ λ if p ( k |P , M ) = p ( k |P , M ′ ) ∀P Can we use this definition to experimental test Kochen-Specker? In this language value assignements for M = { P 1 , P 2 , P 3 } satisfy ξ ( i | λ, M ) ξ ( j | λ, M ) = 0 for i � = j ; � ξ ( i | λ, M ) = 1 i

  10. Experimental tests of contextuality Measurement noncontextuality ξ ( k | λ, M ) = ξ ( k | λ, M ′ ) ∀ λ if p ( k |P , M ) = p ( k |P , M ′ ) ∀P Problem Assuming MNC, if measurements are not ideal (i.e., they contain noise) the functions ξ will not be in { 0 , 1 } . We are no longer comparing { 0 , 1 } -valued assignements following O , C rules 3 . We cannot experimentally test KS theorem with this assumption! 3 R. W. Spekkens, Found. Phys. 44, 1125 (2014).

  11. Experimental tests of contextuality Other approaches ◮ Is it possible to extend Kochen-Specker notion of contextuality to contain Bell experiments? ◮ What is the notion of context there? ◮ Under which assumption we can identify “the same measurement in different contexts”?

  12. Experimental tests of contextuality x y B A S a b Bell scenario ◮ Contexts: joint measurements of ( A x , B y ). ◮ Identification of same measurement in different context: same local “black-box”. ◮ “Noncontextuality assumption”: the choice of measurement on B does not influence the outcome of A .

  13. Experimental tests of contextuality x y A B S a b Bell scenario In terms of probabilities (Local hidden variable theory) � p ( ab | xy ) = p ( λ ) p ( a | x , λ ) p ( b | y , λ ) λ Compare with previous definition: � p ( k |P , M ) = µ ( λ |P ) ξ ( k | λ, M ) λ Joint measurements instead of preparation-measurement.

  14. Experimental tests of contextuality x y z M x M y M z ϱ in a c b Generalization? Analogous expression in terms of probabilities � p ( abc | xyz ) = p ( λ ) p ( a | x , λ ) p ( b | y , λ ) p ( c | z , λ ) λ Can we interpret measurements as black-boxes? What are the physical assumptions?

  15. Experimental tests of contextuality x y z M x M y M z ϱ in a c b Sequential measurements Classical models for seq. meas: Leggett-Garg macrorealism 4 � p ( abc | xyz ) = p ( λ ) p ( a | x , λ ) p ( b | y , λ ) p ( c | z , λ ) λ Assumptions: ◮ Macrorealism (i.e., classical probability) ◮ Non-invasive measurements (i.e., context-independence of the outcome). 4 A. J. Leggett and A. Garg, Phys. Rev. Lett. 54, 857 (1985).

  16. Experimental tests of contextuality x y z M x M y M z ϱ in a c b Assumptions: ◮ (MR) Macrorealism (i.e., classical probability) ◮ (NIM) Non-invasive measurements (i.e., context-independence of the outcome). Problem NIM very strong assumption. Not clear why it should be satisfied and how it is related to KS theorem.

  17. Experimental tests of contextuality x y z M x M y M z ϱ in a c b Ideal case Can we use properties of ideal projective measurements to justify NIM assumption? E.g., A and B compatible implies A does not “disturb” the outcome of B in any sequence and with arbitrary repetitions, e.g., BAABBAAAB . p (1 xx 11 xxx 1 | B 1 = 1 , A 2 , A 3 , B 4 , B 5 , A 6 , A 7 , A 8 , B 9 ) = 1 (1) Repeatability of the outcomes, in all orders, for arbitrary sequences.

  18. Experimental tests of contextuality Two versions of KCBS inequality 5 : { P i } 4 i =0 , [ P i , P i +1 ] = 0 4 � � P i � ≤ 2 , (KS inequality) , i =0 4 � � A i A i +1 � ≥ − 3 , with A i = 1 1 − 2 P i , (NC inequality) i =0 Transformation of KS inequalities into NC inequalities always possible 6 5 AA. Klyachko et al. Phys. Rev. Lett., 101(2):020403, (2008). J. Ahrens et al. Scientific reports, 3, 2170 (2013). 6 X.-D. Yu and D. M. Tong Phys. Rev. A 89 (2014).

  19. Experimental tests of contextuality What if measurements are not ideal? They must introduce some disturbance, we can try to quantify (incomplete list) ◮ Otfried G¨ an Cabello, Jan-˚ uhne, Matthias Kleinmann, Ad´ Ake Larsson, Gerhard Kirchmair, Florian Z¨ ahringer, Rene Gerritsma, and Christian F. Roos. Compatibility and noncontextuality for sequential measurements , Phys. Rev. A, 81(2):022121, 2010. ◮ Jochen Szangolies, Matthias Kleinmann, and Otfried G¨ uhne. Tests against noncontextual models with measurement disturbances , Phys. Rev. A, 87(5):050101, 2013. Jochen Szangolies, Testing Quantum Contextuality: The Problem of Compatibility , Springer, 2015. ◮ Janne V. Kujala, Ehtibar N. Dzhafarov, and Jan-˚ Ake Larsson, Necessary and Sufficient Conditions for an Extended Noncontextuality in a Broad Class of Quantum Mechanical Systems , Phys. Rev. Lett. 115, 150401 (2015)

  20. Experimental tests of contextuality Different physical assumptions on the properties of “noise”, E.g., Innsbruck experiment 7 : noise always adds up. Correction terms to the classical bound of the form p err [ BAB ], i.e., probability that B flips its value due to a measurement of A . 7 Kirchmair et al. Nature 460 (2009). G¨ uhne et al. Phys. Rev. A, 81(2):022121, (2010).

  21. Applications of contextuality A possible indication of the most intresting notions could come from the applications of contextual correlations: ◮ Quantum computation ◮ Other applications? (Dimension witnesses? Random access codes? Cryptography?)

  22. Contextuality and Quantum computation Incomplete list: 1. M. Howard, J. Wallman, V. Veitch, J. Emerson, Nature 510 (2014). 2. R. Raussendorf, PRA 88 (2013) 3. N. Delfosse, P.A. Guerin, J. Bian, R. Raussendorf, PRX 5 (2015) 4. J. Bermejo-Vega, N. Delfosse, D.E. Browne, C. Okay, R. Raussendorf PRL 119 (12) (2017) 5. R. Raussendorf, D.E. Browne, N. Delfosse, C. Okay, J. Bermejo-Vega PRA 95 (2017) ◮ 1. about QC via Magic State Injection (MSI) → CSW approach and KS ineq. 8 ◮ All others about Measurement Based Quantum Computation (MBQC) → sequential measurements and NC inequalities. 8 Cabello, Severini, Winter Phys. Rev. Lett. 112, 040401 (2014).

  23. Contextuality and Quantum computation Measurement based quantum computation Computation on N qubits → measurement of N compatible obs. Efficient simulation of measurements ⇒ efficient simulation of computation.

  24. Contextuality and Quantum computation Measurement based quantum computation Measurement scheme: adaptive measurements on N qubits in a 2D cluster state 9 . 9 H. J. Briegel et al. Nature Physics 5 (2009)

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