STUDY OF CORRELATIONS AND NON-MARKOVIANITY IN DEPHASING OPEN QUANTUM SYSTEMS Università degli Studi di Milano Giacomo GUARNIERI Supervisor: Bassano VACCHINI.

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Presentation transcript:

STUDY OF CORRELATIONS AND NON-MARKOVIANITY IN DEPHASING OPEN QUANTUM SYSTEMS Università degli Studi di Milano Giacomo GUARNIERI Supervisor: Bassano VACCHINI Co-Supervisor: Matteo PARIS PhD school of Physics, XXIX Cicle

Open Quantum Systems Theory Quantum non-Markovianity Two-time correlation functions and Quantum Regression Theorem A case of study: The Pure Dephasing Spin-Boson System CONTENTS

Open Quantum Systems Theory Quantum non-Markovianity Two-time correlation functions and Quantum Regression Theorem A case of study: The Pure Dephasing Spin-Boson System CONTENTS

System Open Quantum Systems Theory Open Quantum Systems Theory H T = H S

Open Quantum Systems Theory Open Quantum Systems Theory H T = H S + H E System Environment

Open Quantum Systems Theory Open Quantum Systems Theory Interaction H T = H S + H E + H I U(t,0) = exp [ i H T t ] Environment System

Open Quantum Systems Theory Open Quantum Systems Theory PROPERTIES OF COMPLETE POSITIVITY (CP) TRACE PRESERVING (T)

Open Quantum Systems Theory Quantum non-Markovianity Two-time correlation functions and Quantum Regression Theorem A case of study: The Pure Dephasing Spin-Boson System CONTENTS

Quantum non-Markovianity System 1 Time (arbitrary units) D(t;ρ 1,2 ) Environment The trace distance measures the distinguishability between states System 2 Physical interpretation: evolution of information flow between S and E

System 1 Environment System 2 Quantum non-Markovianity Time (arbitrary units) D(t;ρ 1,2 ) The trace distance measures the distinguishability between states Physical interpretation: evolution of information flow between S and E

System 1 Environment System 2 Quantum non-Markovianity The trace distance measures the distinguishability between states Time (arbitrary units) D(t;ρ 1,2 ) Physical interpretation: evolution of information flow between S and E

Quantum non-Markovianity Backflow of information Memory effects non-Markovian dynamics H.P. Breuer, E. M. Laine, J. Piilo, PRL 103, (2009) B. H. Liu et al., Nat. Phys. 7, 931 (2011)

Open Quantum Systems Theory Quantum non-Markovianity Two-time correlation functions and Quantum Regression Theorem A case of study: The Pure Dephasing Spin-Boson System CONTENTS

Two-time correlation functions and Quantum Regression Theorem Mean Values : Two-time CF:

Two-time correlation functions and Quantum Regression Theorem Mean Values : Two-time CF: with ‘EASY’ ! VERY DIFFICULT!

? Two-time correlation functions and Quantum Regression Theorem Two-time CF: Quantum World Mean Values : Quantum non-Markovian dynamics relation between & Classical World of Stochastic Processes Markovian process iff

Two-time correlation functions and Quantum Regression Theorem Quantum Regression Theorem! Mean Values : Two-time CF: M. Lax, Phys. Rev 172, 350 (1968)

Two-time correlation functions and Quantum Regression Theorem Closed and linear system of evolution equations for mean values Basis for the space of operators

Two-time correlation functions and Quantum Regression Theorem Main assumption for the validity of QRT: Closed and linear system of evolution equations for mean values In most physical situation this assumption is never strictly satisfied!! Search for regions of parameters where Basis for the space of operators

Question to answer Quantum non- Markovianity Quantum Regression Theorem ?

Open Quantum Systems Theory Quantum non-Markovianity Two-time correlation functions and Quantum Regression Theorem A case of study: The Pure Dephasing Spin-Boson System CONTENTS

Pure Dephasing Spin-Boson System Two-level system coupled to an infinite number of bosonic modes The populations of the system are constants of motion! G.G., A. Smirne, B. Vacchini, PRA 90, (2014)

Pure Dephasing Spin-Boson System and therefore the reduced system state has the analytic form where The action of the total evolution operator can be explicitly evaluated is the DECOHERENCE FUNCTION.

Pure dephasing spin-boson model Ohmicity Coupling strength Cutoff frequency Thermal Bath If we assume... Spectral Density the decoherence function, in the limit β → +∞, becomes G.G., A. Smirne, B. Vacchini, PRA 90, (2014)

Pure dephasing spin-boson model Non-Markovianity condition for the pure dephasing spin-boson Indipendently of λ !!

Pure dephasing spin-boson model Non-Markovianity condition for the pure dephasing spin-boson Increasing s! Indipendently of λ !! The degree of non-Markovianity though depends on λ

Pure dephasing spin-boson model Two-time Correlation Functions & Quantum Regression Theorem To estimate the violations to the QRT by computing the RELATIVE ERROR S=1.5

Pure dephasing spin-boson model Two-time Correlation Functions & Quantum Regression Theorem S=1.5 < s crit ! To estimate the violations to the QRT by computing the RELATIVE ERROR

Pure dephasing spin-boson model CONCLUSIONS ≠ Quantum non- Markovia nity Quantum Regression Theorem Related to the EFFECTS OF CORRELATIONS between S and E at the level of the reduced dynamics Related to the ACTUAL CORRELATIONS between S and E at the level of the overall dynamics G.G., A. Smirne, B. Vacchini, PRA 90, (2014)

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