Some aspects of Classical-quantum dynamics

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Some aspects of Classical-quantum dynamics Jan Tuziemski, Stockholm University and NORDITA Quantum Connections workshop 25.06.2021

Transcript of Some aspects of Classical-quantum dynamics

Page 1: Some aspects of Classical-quantum dynamics

Some aspects ofClassical-quantum dynamics

Jan Tuziemski, Stockholm University and NORDITA

Quantum Connections workshop 25.06.2021

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1. Realization of a classical system within quantum mechanics

2. A model of (consistent) classical quantum dynamics

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Part 1

Koopman von Neumann mechanics

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Koopman von Neumann mechanics

● Classical mechanics can be formulated in terms of Hilbert space

● In terms of states: one needs joint X and P eigenstates (they need to commute)

● In terms of dynamics: to have an analogue of Heisenberg equation of motion there should be operators not commuting with X and P

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Koopman von Neumann mechanics

● Minimal realization involves 4 operators with non-trivial commutators:

● Liouville operator governing evolution of classical wavefunction

● Standard Liouville equation is recovered in XP representation, assuming that probability density is given by modulus squared of the wavefunction

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Koopman von Neumann mechanics

● Minimal realization involves 4 operators with non-trivial commutators:

● Such a system can be realized within quantum mechanics

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Koopman von Neumann mechanics

● Minimal realization involves 4 operators with non-trivial commutators:

● Such a system can be realized within quantum mechanics

● These are EPR operators

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Koopman von Neumann mechanics

● Liouville operator (note the minus):

● Eg. for a harmonic oscillator – the second system has a negative mass

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Koopman von Neumann mechanics

● One can realize classical systems within QM (free particle, particle in a linear potential, harmonic oscillator)

● To do so one needs:

1) entanglement (EPR operators)

2) (effective) negative mass

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Koopman von Neumann mechanics

● One can realize classical systems within QM (free particle, particle in a linear potential, harmonic oscillator)

● This is useful for increasing measurements precision (e.g. a wavepacket does not spread)

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Open problems● Is there a similar trick for qubits (qudits)?

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Part 2

A model of classical-quantum dynamics

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Motivation● Why it is interesting to consider composite classical-quantum systems ?

– thermodynamics/chemistry: small molecules (quantum) interact with large reservoirs (classical)

– Measurement theory: quantum systems interact with macroscopic devices (classical)

– Gravity: quantum fields interact with gravitational field (effectively? classical)

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Introduction● Can one consistently couple classical and quantum systems?

– Many formulations e.g. :● Koopman-von Neuman hybrid dynamics

● Aleksandrov bracket

● Many others

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Introduction● Can one consistently couple classical and quantum systems?

– Many formulations – many problems :● No-go theorems

● Not completely positive dynamics (leading to “negative” probabilities)

● Non-linear formulations (density matrix looses its statistical interpretation)

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Introduction● Classical-quantum dynamics introduced in

and further applied in different contexts.

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Introduction● Main features of classical quantum coupling:

– Decoherence of quantum systems

– “Collapse” of the wavefunction (quantum system jumps to a pure state that can be determined from classical dof)

– Diffusion in the classical phase space

See: [A post-quantum theory of classical gravity?] J. Oppenheim [Objective trajectories in hybrid classical-quantum dynamics] J. Oppenheim et al.

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Some details● Object of study: hybrid density

● - phase space variables

● - distribution over z; - a valid quantum state.

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Some details● Object of study: hybrid density

● e.g. for a qubit

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Some details● Evolution equation (GKLS/Lindblad)

● - Describes change in phase space and jump of the quantum system

Commutator

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Some details● How to include “free” classical evolution?

● where

Poisson Bracket

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Some details● How to include “free” classical evolution?

● First order: Poisson bracket

● Second order: diffusion

● ...

Expansion

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Some details● Gravity (main features of the framework):

– Decomposition based on ADM Hamiltonian (Lindblad operators → field operators)

– Constraints implemented on the level of equations of motion → constrains possible realizations (see also “The constraints of post-quantum classical gravity” J. Oppenheim et al. arXiv:2011.15112)

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Open problems

– Characterization of decoherence/diffusion interplay

– Weak-field limit of the framework

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Some details● Evolution equation (expansion):

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Some details● Next term (diffusion)