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Faculty of Physics University of Warsaw > Events > Seminars > Joint Seminar on Quantum Information and Technologies

Joint Seminar on Quantum Information and Technologies

2012/2013 | 2013/2014 | 2014/2015 | 2015/2016 | 2016/2017 | 2017/2018 | 2018/2019 | 2019/2020 | 2020/2021 | 2021/2022 | 2022/2023 | 2023/2024 | 2024/2025 | YouTube channel

until 2023/2024 Quantum Information Seminar | YouTube channel

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2017-03-16 (Thursday)
room 1.02, Pasteura 5 at 10:30  Calendar icon
Rafał Demkowicz-Dobrzański (IFT UW)

Quantum Metrology: towards the "Grand Unified Theory"…

2017-03-09 (Thursday)
room 1.02, Pasteura 5 at 10:30  Calendar icon
Lucas Celeri (Federal University of Goiás, Brazylia)

Geometric approach to time-energy uncertainty relations

The attempt to gain a theoretical understanding of the concept of time in quantum mechanics has triggered significant progress towards the search for faster and more efficient quantum technologies. One of such advances consists in the interpretation of the time-energy uncertainty relations as lower bounds for the minimal evolution time between two distinguishable states of a quantum system, also known as quantum speed limits. Here we discuss how the nonuniqueness of a bona fide measure of distinguishability defined on the quantum-state space affects the quantum speed limits and can be exploited in order to derive improved bounds. Specifically, we establish an infinite family of quantum speed limits valid for unitary and nonunitary evolutions, based on an elegant information geometric formalism. Some possible applications in quantum thermodynamics are also discussed.
2017-03-02 (Thursday)
room 1.02, Pasteura 5 at 10:30  Calendar icon
Adam Sawicki (CFT PAN)

Universality of single qudit gates

2017-02-02 (Thursday)
room 1.02, Pasteura 5 at 10:30  Calendar icon
Alexsander Smith (University of Waterloo)

Quantizing time: General Hamiltonians in the conditional probability interpretation of time

The canonical quantization of gravity leads to the Hamiltonian constraint, that is, physical states of the theory are annihilated by the Hamiltonian. Combined with the Schrodinger equation, the Hamiltonian constraint dictates that the physical states do not evolve in time. This poses a problem for time in the theory: Given that the physical states do not evolve, how do we explain the time evolution we see around us?I will begin by reviewing how the Hamiltonian constraint arises in both classical and quantum mechanics and then introduce the conditional probability interpretation of time, which is a possible answer to the question above. I will then discuss two generalizations of this interpretation which are necessary if it is to be applied to time in quantum gravity.
2017-01-26 (Thursday)
room 1.02, Pasteura 5 at 10:30  Calendar icon

Seminarium odwolane!

2017-01-19 (Thursday)
room 1.02, Pasteura 5 at 10:30  Calendar icon
dr hab. inż. Tomasz Kozacki (Instytut Mikromechaniki i Fotoniki, Politechnika Warszawska)

Color coherent and incorerent holographic displays

2017-01-12 (Thursday)
room 1.02, Pasteura 5 at 10:30  Calendar icon
Karol Gietka (IFT UW)

Enhancing interferometric sensitivity by non-classical light from quantum-non demolition measurements in cavity QED

2016-12-15 (Thursday)
room 1.02, Pasteura 5 at 10:30  Calendar icon
Adam Bednorz (IFT UW)

Relativity in quantum realism

2016-12-08 (Thursday)
room 1.02, Pasteura 5 at 10:30  Calendar icon
Rafał Demkowicz-Dobrzański (IFT UW)

When simultaneous quantum estimation of many parameters is no more difficult than estimating each of them separately?

Simultaneous estimation of multiple parameters in quantum metrological models is complicated by factors relating to the (i) existence of a single probe state allowing for optimal sensitivity for all parameters of interest, (ii) existence of a single measurement optimally extracting information from the probe state on all the parameters, and (iii) statistical independence of the estimated parameters. We consider the situation when these concerns present no obstacle and for every estimated parameter the variance obtained in the multiparameter scheme is equal to that of an optimal scheme for that parameter alone, assuming all other parameters are perfectly known. We call such models compatible. In establishing a rigorous framework for investigating compatibility, we clarify some ambiguities and inconsistencies present in the literature and discuss several examples to highlight interesting features of unitary and non-unitary parameter estimation, as well as deriving new bounds for physical problems of interest, such as the simultaneous estimation of phase and local dephasing.
2016-12-01 (Thursday)
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