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
2024-07-22 (Monday)
Sibasish Ghosh (The Institute of Mathematical Sciences, Chennai, India)
Unambiguous discrimination of two-photon entangled states in linear optical set-ups
A linear optics-based scheme to implement various quantum information processing tasks is of paramount importance due to ease of implementation and low noise. Many information-theoretic tasks depend on the successful discrimination of Bell states. A no-go theorem has been proved in literature which tells that it is not possible to perfectly discriminate among the four Bell states by restricting measurement apparatus to linear optical elements. The success probability is only 50%. Through using extra resources such as hyper entanglement, ancillary entanglement, and even a minimum amount of non-linearity complete Bell-state discrimination can be achieved. The success probability for Bell-like state discrimination is only 25%. We find that this can be boosted up to 50% using hyperentanglement in polarization, momentum, or OAM degrees of freedom of the photons which is in contrast to the Bell-state discrimination scenario where 100% can be achieved. Furthermore, we find that by using correlation in time of the photons all four Bell states can be distinguished with 100% success probability while for the Bell-like state discrimination, it strictly lies between 25% and 50% depending on the state parameter with only three Bell-like states being distinguishable. We also observe a similar contrast when we use ancillary entangled photons. While the success probability for all four Bell-state discrimination increases as $1 − 1/2^N$ where $N$ is the number of ancillary photons for Bell-like states it depends again on the state parametersand can be less than 25% in some cases. Also adding further ancillary photons decreases the success probability. We then show that using non-linear gadgets namely SFG 100% success probability can be achieved even forBell-like state discrimination.[Based on the joint work arXiv:2402.00832 (quant-ph) with Jatin Ghai]
2024-06-14 (Friday)
Aleksander Lasek (University of Maryland)
Thermalization with noncommuting conserved quantities [Extra seminar: room and time changed!]
2024-06-13 (Thursday)
Jayanth Jayakumar (MIMUW UW)
Quantum-enhanced joint estimation of phase and phase diffusion
Accurate phase estimation in the presence of unknown phase diffusive noise is a crucial yet challenging task in noisy quantum metrology. This problem is particularly interesting due to the detrimental impact of the associated noise. Here, we investigate the joint estimation of phase and phase diffusion using generalized Holland-Burnett states, known for their experimental accessibility. These states provide performance close to the optimal state in single-parameter phase estimation, even in the presence of photon losses. We adopt a twofold approach by analyzing the joint information extraction through the double homodyne measurement and the joint information availability across all probe states. Through our analysis, we find that the highest sensitivities are obtained by using states created by directing all input photons into one port of a balanced beam splitter. Furthermore, we infer that good levels of sensitivity persist even in the presence of moderate photon losses, illustrating the remarkable resilience of our probe states under lossy conditions.
2024-06-06 (Thursday)
Julia Amoros Binefa (QOT CENT UW)
Quantum atomic sensors operated in real time
2024-05-23 (Thursday)
Lewis Clark (Palacky University, Olomouc)
Efficient inference of quantum system parameters by Approximate Bayesian Computation
2024-05-16 (Thursday)
Olgierd Żurek (Wydział Fizyki UW)
Introduction to Joint Measurements
2024-05-09 (Thursday)
David Ziemkiewicz (Politechnika Bydgoska)
Emerging quantum technologies with Rydberg excitons
The recent discovery of Rydberg excitons in Cu2O opened up a completely new field of solid state physics, with many exciting applications. Rydberg atoms are a well-known tool in quantum information science, but their potential applications require high vacuum and sophisticated laser cooling schemes. Rydberg excitons are a solid state counterpart to Rydberg atoms, providing a basis for a plethora of Cu2O-based devices. For example, a superlattice containing a Rydberg exciton [1] is an analog of a Rydberg atom trapped in an optical lattice, which can be a promising tool in quantum computing [2-4]. Moreover, due to the small energy spacing between high exciton states, one can devise a scheme for frequency conversion from optical to microwave range [5], possibly providing an interface to systems such as superconducting qubits operating at these frequencies [6].
References
[1] D. Ziemkiewicz, G. Czajkowski, S. Zielińska-Raczyńska, Optical properties of Rydberg excitons in Cu2O-based superlattices, Phys. Rev. B 109, 085309 (2024)
[2] L. Isenhower, et al, Demonstration of a neutral atom controlled-NOT quantum gate, Phys. Rev. Lett. 104, 010503 (2010).
[3] A. Omran, et al, Generation and manipulation of Schrödinger cat states in Rydberg atom arrays, Science 365, 570 (2019).
[4] W. Li, A boost to Rydberg quantum computing, Nat. Phys. 16, 820 (2020).
[5] D. Ziemkiewicz, S. Zielińska-Raczyńska, Optical-to-microwave frequency conversion with Rydberg excitons, Phys. Rev. B 107, 195303 (2023)
[6] N. J. Lambert et al, Coherent conversion between microwave and optical photons - An overview of physical implementations, Adv. Quantum Technol. 3, 1900077 (2020).
References
[1] D. Ziemkiewicz, G. Czajkowski, S. Zielińska-Raczyńska, Optical properties of Rydberg excitons in Cu2O-based superlattices, Phys. Rev. B 109, 085309 (2024)
[2] L. Isenhower, et al, Demonstration of a neutral atom controlled-NOT quantum gate, Phys. Rev. Lett. 104, 010503 (2010).
[3] A. Omran, et al, Generation and manipulation of Schrödinger cat states in Rydberg atom arrays, Science 365, 570 (2019).
[4] W. Li, A boost to Rydberg quantum computing, Nat. Phys. 16, 820 (2020).
[5] D. Ziemkiewicz, S. Zielińska-Raczyńska, Optical-to-microwave frequency conversion with Rydberg excitons, Phys. Rev. B 107, 195303 (2023)
[6] N. J. Lambert et al, Coherent conversion between microwave and optical photons - An overview of physical implementations, Adv. Quantum Technol. 3, 1900077 (2020).
2024-04-25 (Thursday)
Wojciech Bruzda (CFT PAN)
A rank of a tensor
A rank of a tensor is analyzed in context of quantum entanglement. We define and discuss various notions of tensor ranks: generic, maximal and border ones, and review selected results for the low dimensions. A relation between different ranks and norms of a tensor and the entanglement of the corresponding quantum state is presented.
2024-04-18 (Thursday)
Arpan Das (IFT UW)
Universal time scalings of sensitivity in Markovian quantum metrology
Assuming a Markovian time evolution of a quantum sensing system, we provide a general characterization of the optimal sensitivity scalings with time, under the most general quantum control protocols. We allow the estimated parameter to influence both the Hamiltonian as well as the dissipative part of the quantum master equation. We focus on the asymptotic-time as well as the short-time sensitivity scalings, and investigate the relevant time scales on which the transition between the two regimes appears. This allows us to characterize, via simple algebraic conditions (in terms of the Hamiltonian, the jump operators as well as their parameter derivatives), the four classes of metrological models that represent: quadratic-linear, quadratic-quadratic, linear-linear and linear-quadratic time scalings. We also provide universal numerical methods to obtain quantitative bounds on sensitivity that are the tightest that exist in the literature.
2024-04-11 (Thursday)
Lorenzo Maccone (University of Pavia)
Quantum time and quantum spacetime
We present a new way to approach relativistic quantum mechanics, whichis based on constructing a Hilbert space for events. In this wayspatial and temporal degrees of freedom are treated completelysymmetrically, so that a completely relativistically covariantformulation of quantum mechanics it is possible. It is a minimalextension of textbook quantum mechanics. The consequences ofconsidering time as a quantum observable are detailed.