Faculty of Physics University of Vienna Institute for

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Faculty of Physics, University of Vienna & Institute for Quantum Optics and Quantum Information,

Faculty of Physics, University of Vienna & Institute for Quantum Optics and Quantum Information, Vienna Indefinite causal order in quantum mechanics Časlav Brukner Mateus Araujo, Cyril Branciard, Fabio Costa, Adrian Feix, Christina Giarmatzi, Ognyan Oreshkov, Magdalena Zych The 11 th “Vienna Central European Seminar on Particle Physics and Quantum Field Theory”

Possible causal influences

Possible causal influences

Question: Can one have situations in which the causal order is not fixed, but

Question: Can one have situations in which the causal order is not fixed, but rather is subject to quantum indefiniteness?

Question: Can one have situations in which the causal order is not fixed, but

Question: Can one have situations in which the causal order is not fixed, but rather is subject to quantum indefiniteness? Dynamical causal structure of general relativity + Superposition principle of quantum mechanics

Question: Can one have situations in which the causal order is not fixed, but

Question: Can one have situations in which the causal order is not fixed, but rather is subject to quantum indefiniteness? Dynamical causal structure of general relativity + Superposition principle of quantum mechanics

Question: Can one have situations in which the causal order is not fixed, but

Question: Can one have situations in which the causal order is not fixed, but rather is subject to quantum indefiniteness? Dynamical causal structure of general relativity + Superposition principle of quantum mechanics

Outline § “Causal inequalities“ Device-independent approach to causality § Framework for quantum mechanics with

Outline § “Causal inequalities“ Device-independent approach to causality § Framework for quantum mechanics with no assumed global causal structure: Device-dependent approach to causality Causally non-separable processes § Quantum computation with indefinite order of gates Computational task that cannot be accomplished on a computer with fixed order of gates § Physical realization of causally non-separable processes Linear optical schemes & via superposition of large masses

“Correlation does not imply causation”

“Correlation does not imply causation”

The notion of “causation” Effect Cause One-directional signalling Necessity of interventions, or free variables,

The notion of “causation” Effect Cause One-directional signalling Necessity of interventions, or free variables, statistically independent of “the rest of the experiment”

The notion of “causation” One-directional signalling Necessity of interventions, or free variables, statistically independent

The notion of “causation” One-directional signalling Necessity of interventions, or free variables, statistically independent of “the rest of the experiment”

Definite causal order No-signalling Space-like separated One-directional signalling Alice before Bob Time-like separated

Definite causal order No-signalling Space-like separated One-directional signalling Alice before Bob Time-like separated

Causal inequalities (Device-independent approach to causality) Assumptions: § System enters each laboratory only once.

Causal inequalities (Device-independent approach to causality) Assumptions: § System enters each laboratory only once. § The laboratories are shielded and interact with “the outside world” only through the system entering and exiting it. Causal correlations: either A signals to B or B signals to A, or no-signalling or a convex combination of these situations.

Causal inequalities (Device-independent approach to causality) No-signalling One-directional signalling: Alice to Bob Causal correlations:

Causal inequalities (Device-independent approach to causality) No-signalling One-directional signalling: Alice to Bob Causal correlations: either A signals to B or B signals to A, or no-signalling or a convex combination of these situations.

The simplest causal inequality 1 bit input, 1 bit output Causal correlations satisfy causal

The simplest causal inequality 1 bit input, 1 bit output Causal correlations satisfy causal inequalities, which are facets of the causal polytope Guess Your Neighbour’s Input (GYNI) game: C. Branciard, M. Araújo, A. Feix, F. Costa, Č. B. , to appear in New J. Phys. (2015)

“Non-causal correlations” (violating causal inequalities) Interpretation: Both A signals to B and B signals

“Non-causal correlations” (violating causal inequalities) Interpretation: Both A signals to B and B signals to A, although the system enters only once the laboratory and the laboratories are shielded. Two-directional signalling

Local quantum laboratory (Device-dependent approach to causality) Output space Future Hilbert space-like surface Input

Local quantum laboratory (Device-dependent approach to causality) Output space Future Hilbert space-like surface Input Past space-like Hilbert space surface

Local quantum laboratory (Device-dependent approach to causality) Output space Future Hilbert space-like surface Input

Local quantum laboratory (Device-dependent approach to causality) Output space Future Hilbert space-like surface Input Past space-like Hilbert space surface Transformations = completely positive (CP) trace-nonincreasing maps

Many local quantum laboratories b c Quantum mechanics locally valid. (no globar causal order

Many local quantum laboratories b c Quantum mechanics locally valid. (no globar causal order fixed) Probabilities: Process matrix: O. Oreshkov, F. Costa, Č. B. , Nature Communication 3: 1092 (2012)

Conditions on W b c Quantum mechanics locally valid. (no global causal order fixed)

Conditions on W b c Quantum mechanics locally valid. (no global causal order fixed) Positivity: Normalization: O. Oreshkov, F. Costa, Č. B. , Nature Communication 3: 1092 (2012)

Forbidden processes No “grandfather paradox” Single Loops Double Loops O. Oreshkov, F. Costa, Č.

Forbidden processes No “grandfather paradox” Single Loops Double Loops O. Oreshkov, F. Costa, Č. B. , Nature Communication 3: 1092 (2012)

Admissible processes Channels from Alice to Bob Time-like separated States Space-like separated O. Oreshkov,

Admissible processes Channels from Alice to Bob Time-like separated States Space-like separated O. Oreshkov, F. Costa, Č. B. , Nature Communication 3: 1092 (2012)

Causally separable processes Ordered processes: A signals to B, or no signaling B signals

Causally separable processes Ordered processes: A signals to B, or no signaling B signals to A, or no signaling Most general processes compatible with definite causal structure (convex mixtures of ordered processes): There are causally non-separable processes

Quantum switch – quantum control of causal order Path degree of freedom (quantum control)

Quantum switch – quantum control of causal order Path degree of freedom (quantum control) Internal degree of freedom Alice Bob Channel from Alice to Bob Channel from Bob to Alice

Quantum switch – quantum control of causal order Bob Cleve Alice Quantum switch is

Quantum switch – quantum control of causal order Bob Cleve Alice Quantum switch is a causally nonseparable process

Quantum switch – quantum control of causal order Bob Cleve Alice Quantum switch is

Quantum switch – quantum control of causal order Bob Cleve Alice Quantum switch is a causally nonseparable process However, the switch cannot violate a „causal inequality“

„Superposition of unitarities“ Bob Alice Cleve

„Superposition of unitarities“ Bob Alice Cleve

Computational advantages 1 C. Branciard, M. Araújo, A. Feix, F. Costa, and C. B.

Computational advantages 1 C. Branciard, M. Araújo, A. Feix, F. Costa, and C. B. , ar. Xiv: 1508. 01704 (2015). Colnaghi, G. M. D’Ariano, S. Facchini, and P. Perinotti, Phys. Lett. A 376, 29402943 (2012) 3 G. Chiribella, Phys. Rev. A 86, 040301(R) (2012) 4 M. Araujo, F. Costa, and C. B. , Phys. Rev. Lett. 113, 250402 (2015) 5 A. Feix, M. Araujo, and C. B. Phys. Rev. A 92, 052326 (2015)

Experimental Demonstration L. M. Procopio et. al, Nature Communication 6, 7913

Experimental Demonstration L. M. Procopio et. al, Nature Communication 6, 7913

Order of events determined by their position in space-time B A

Order of events determined by their position in space-time B A

General relativity: space-time is dynamical

General relativity: space-time is dynamical

General relativity: space-time is dynamical Proper times of clocks a & b Dynamics of

General relativity: space-time is dynamical Proper times of clocks a & b Dynamics of the clock describe M. Zych, F. Costa, I. Pikovski, Č. B. , Nature Communication 2: 505 (2011) I. Pikovski, M. Zych, F. Costa, Č. B. , Nature Physics 11, 668 (2015)

General relativity: space-time is dynamical Proper times of clocks a & b Dynamics of

General relativity: space-time is dynamical Proper times of clocks a & b Dynamics of the clock describe M. Zych, F. Costa, I. Pikovski, Č. B. , Nature Communication 2: 505 (2011) I. Pikovski, M. Zych, F. Costa, Č. B. , Nature Physics 11, 668 (2015)

Gravitational quantum switch Quantum control of temporal order

Gravitational quantum switch Quantum control of temporal order

Summary and Outlook § Global causal order need not be a necessary element of

Summary and Outlook § Global causal order need not be a necessary element of quantum theory. § There exist physical processes that are causally nonseparable. § Causally nonseparable processes is a new resource for quantum information processing § The framework also includes processes with no (known) physical interpretation § Does a theory of quantum gravity provide a physical interpretation to such processes?

Thank you! quantumfoundations. org

Thank you! quantumfoundations. org

Force-free time dilation Potential R r A r. B B r

Force-free time dilation Potential R r A r. B B r

Relative degrees of freedom = Local clock Superposition of backgrouds Clock in a superposition

Relative degrees of freedom = Local clock Superposition of backgrouds Clock in a superposition Fixed backgroud

Clock in a superposition running clock in a superposition GR: time shown by the

Clock in a superposition running clock in a superposition GR: time shown by the clock depends on the path taken QM: either path or interference QM+GR: interference cannot be observed since the whichpath information is stored in the clock time

Visibility modulation Difference in proper time Orthogonalization time M. Zych, F. Costa, I. Pikovski,

Visibility modulation Difference in proper time Orthogonalization time M. Zych, F. Costa, I. Pikovski, Č. B. , Nature Communication 2: 505 (2011) I. Pikovski, M. Zych, F. Costa, Č. B. , Nature Physics 11, 668 (2015)