Najbliższe seminaria

28 IVRomuald Janik (Jagiellonian University)
Universality and emergent fluid from string breaking in the Schwinger model via tensor networks
Gdzie: B-1-46 AND MS Teams [ZOA-test], 12:15
Seminarium Zakładowe
Online: [link]
28 IVNatalia Łygan (UJ)
Quantum Kolmogorov-Sinai entropy and Pesin relation
Gdzie: F-1-04 and ZOOM [14:15]
Online: [link], pass: on request!
Chaos i Informacja Kwantowa
Pokaż pozostałe

[Abstrakt, pełna informacja]

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

Konferencje

06-08.09.2023 - Konferencja "Time Crystals"


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

Więcej szczegółów on conference website.

05-11.09.2021 - Quantum Optics X

Więcej szczegółów na stronie konferencji.

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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