Abstract

More than a century after the inception of quantum theory, the question of which traits and phenomena are fundamentally quantum remains under debate. Here we give an answer to this question for temporal processes which are probed sequentially by means of projective measurements of the same observable. Defining classical processes as those that can---in principle---be simulated by means of classical resources only, we fully characterize the set of such processes. Based on this characterization, we show that for non-Markovian processes (i.e., processes with memory), the absence of coherence does not guarantee the classicality of observed phenomena and furthermore derive an experimentally and computationally accessible measure for non-classicality in the presence of memory. We then provide a direct connection between classicality and the vanishing of quantum discord between the evolving system and its environment. Finally, we demonstrate that---in contrast to the memoryless setting---in the non-Markovian case, there exist processes that are genuinely quantum, i.e., they display non-classical statistics independent of the measurement scheme that is employed to probe them.

Highlights

  • Quantum coherence is considered to be one of the fundamental traits that distinguishes quantum from classical mechanics [1,2,3]

  • While this always holds true for processes in classical physics, as well as memoryless quantum processes, we show, by means of an explicit example, that this is not necessarily the case for quantum processes with memory; in the presence of quantum memory, there exists a fundamentally new class of processes, which we will call “genuinely quantum” processes, that lead to nonclassical statistics independent of how they are probed

  • Throughout this article, we define the classicality of a process based on observed multitime statistics Pnðxn; tn; Á Á Á ; x1; t1Þ for measurements at different times ft1; ...; tng

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Summary

INTRODUCTION

Quantum coherence is considered to be one of the fundamental traits that distinguishes quantum from classical mechanics [1,2,3]. In a similar manner to the analysis of coherences, our results will predominantly be phrased with respect to measurements in an arbitrary, but predetermined basis, i.e., with respect to a fixed observable, raising the issue of whether classicality is merely a question of perspective; in principle, for every process, there could exist a sequential measurement scheme that yields classical statistics While this always holds true for processes in classical physics, as well as memoryless quantum processes, we show, by means of an explicit example, that this is not necessarily the case for quantum processes with memory; in the presence of quantum memory, there exists a fundamentally new class of processes, which we will call “genuinely quantum” processes, that lead to nonclassical statistics independent of how they are probed.

SUMMARY OF MAIN RESULTS
GENERAL FRAMEWORK
Kolmogorov conditions and classicality
Measurement setup
COHERENCE AND CLASSICALITY
One-to-one connection in the Markovian case
Coherence in the non-Markovian case
NON-MARKOVIAN CLASSICAL PROCESSES
Classicality and processes with memory
Choi-Jamiołkowski representation of general quantum processes
Structural properties of classical combs
Quantifying nonclassicality
DYNAMICAL PROPERTIES OF K-CLASSICAL PROCESSES
Discord and classicality
Non-discord-generating-and-detecting dynamics and classical processes
GENUINELY QUANTUM PROCESSES
A POVM that satisfies the above equation can be readily constructed
Conclusions
Outlook
Cðt1ÆÞ f

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