PAP - about KCIK results
Award for
Prof. M. Horodecki
Award for
Prof. M. Żukowski
5 Jan 2017
JTF Seminar:
Kavan Modi
Monash University, Victoria, Australia
19 Dec 2016
JTF Work in Progress Seminar:
Bogna Bylicka
ICFO, Barcelona
15 Dec 2016
JTF Seminar:
Krzysztof A. Meissner
University of Warsaw
17 Nov 2016
JTF Work in Progress Seminar:
Aniello Lampo
ICFO, Barcelona
09 Nov 2016
Seminar: Johannes Kofler
''No Fine theorem for macrorealism''
21-23 Sept 2016
Quantum phenomena:
Between the whole and the parts
19-21 May 2016
Symposium KCIK 2016
Upcoming Event
JTF Seminar
Speaker: Kavan Modi
Date: 5 Jan 2017 10:15 a.m.

Title: Full and efficient characterisation of non-Markovian quantum processes                                                                                                                                        Abstract: In science, we often want to characterise the processes undergone by a system of interest; this allows us to both identify the underlying physics driving the process and to predict what will happen to the system the next time the process occurs. If the state of the system at any time depends only on the state of the system at the previous time-step and some predetermined rule then these dynamics are characterised with relative ease. For instance, the dynamics of quantum mechanical systems in isolation is described in this way. But, when a quantum system repeatedly interact with an environment, the environment often ’remembers’ information about the system's past. This leads to non-Markovian processes, which depend nontrivially on the state of the system at all times during its evolution and they are not, in general, be easily characterised using conventional techniques. Since the early days of quantum mechanics it has been a challenge to describe non-Markovian processes. Here we will show that using operational tools from quantum information theory we can fully characterise any non-Markovian process. In general the full characterisation is not efficient, as it requires exponentially large number of experiments. To overcome this obstacle we map the full process to a many-body state. We show that this can be achieved by using linear, in the number of time steps, amount of bipartite entanglement. Next, the state can be measured to any desired precision, thus the process can be characterised to any desired precision. Finally, we define a natural measure for the degree of non-Markovianity.

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