Next seminars

20 IVMarek Kopciuch (Adam Mickiewicz University, Poznań and Jagiellonian University, Kraków)
The Spectral Role of Quantum Jumps for Atomic Open Systems
Location: A-1-03 and MS Teams [ZOA-test], 12:15
Department Seminar
Online: [link]
20 IVmgr Pedro Nicácio Falcão (IFT UJ)
Magic resources in disordered quantum spin chains.
Location: F-1-04 and ZOOM
14:15
Online: [link], pass: on request!

Chaos and Quantum Info Seminar
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[Abstract, more info]

Conferences

23-25.10.2025 - Workshop Quantum Chaos II

More details here.

06-10.09.2025 - A Panorama of Tensor Networks: from Condensed Matter to Quantum Field Theory, Holography and Beyond

More details on conference website.

01-15.09.2025 - Quantum Optics XI

More details na stronie konferencji.

16-17.07.2025 - Time Crystals Conference 2025

More details on conference website.

20-22.02.2024 - Workshop on Quantum Simulators of the Future: From Dynamical Gauge Fields to Lattice Gauge Theories | (smr 3922)

An ICTP Meeting This Workshop will gather world-leading groups that design, realize, and characterize a new generation of simulators with ultracold atoms and beyond. It will address novel quantum simulators of statistical gauge fields, dynamical lattices, and lattice gauge theory models (LGT), as well as connections to quantum computing and tensor network methods. https://indico.ictp.it/event/10460

06-08.09.2023 - Time Crystals Conference


27.06-2.07.2022 - 6th Workshop on Algebraic Designs, Hadamard Matrices & Quanta

More details on conference website.

05-11.09.2021 - Quantum Optics X

More details on conference website.

Open Data

Current: /2109.08408/spins

Arxiv link

Here, we give the spin site values arranged for each site over columns. These were used to to calculate the histograms shown in Fig. 2. and Fig. 3. The corresponding number of disorder realizations and number of eigenvalues extracted from the middle of the energy eigenvalue spectrum($\epsilon=\frac{E-E_{min}}{Emax-E_{min}}\sim 0.5 $) corresponds with Table I of the cited paper. Except in case of L=18 and L=20, where the eigenvalues extracted for each disorder is $\leq$ to the eigenvalues shown in the table whereas the number of disorder realizations are $\geq$ to the numbers shown in Table I.

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