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Data and Code for: Quenched Properties of the Spectral Form Factor

Dimitrios Charamis

Published Jan 12, 2026• 0 citations
Publisher

Abstract

These files serve to comply to the data availability statement for the publicpation of (https://arxiv.org/abs/2509.14406) to PRE. The 'Local Minima' python notebook is the code used to (after choosing/generating the desired spectrum) compute the SFF and the corresponding Y variable defined in Eq. (16) of the text, from which its empirical distribution shown or various cases (Figures 1,2,6,7,10,11 and A3 in the text) is readily obtained. Finally, the notebook also includes the computation of the local minima discussed in the beginning of Section V. The data can be then plotted as is done in Figures 8 and 12 in the text. The .npy files '3003_FORSFF.npy', '792_FORSFF.npy', etc. are examples of generated spectra for the Hermitian Model defined in Eq. (23) of the text. Each file is a NumPy array containing energy spectra for many independent disorder realizations of the model at fixed system size. The array has shape (n_samples, D), where n_samples is the number of realizations and D is the Hilbert-space dimension. Each row corresponds to one realization, and each column corresponds to an energy level; within each row, the eigenvalues are real and sorted in ascending order. From these spectra, the distribution of the local energy gap ratios defined in Eq. (19) can be empirically obtained as is shown in Fig. 4 of the text. Using these spectra, the Spectral Form Factor (Eq (1) and its quenched and annealed counterparts (Eq.s (7) and (8) respectively) are obtained. The corresponding data examples are given in 'D3003_sff_L_14_logtimes' and D792_sff_L_12_logtimes''. Each CSV file contains ensemble-averaged spectral form factor data computed from the corresponding eigenvalue file. Rows correspond to different time values, and columns store the time (time), the averaged spectral form factor (K), its disconnected part (K_disc), the connected contribution (K_conn), and the ensemble average of the logarithm of the spectral form factor (mean_lnSFF). The results for the quenched SFF are shown in Fig. 5 of the text The various DSFFs (Eq, (5)) for the Dissipative XY model defined in Eq. (25) are obtained using samples found in the file 'XY_spin_L_14_dim_3003_g_0.4.npy'. The file contains complex energy spectra of a bosonic lattice Hamiltonian for many independent disorder realizations at fixed model parameters. The stored array has shape (n_samples, dim), where n_samples is the number of disorder realizations and dim is the Hilbert-space dimension of the fixed-particle-number sector. Each row corresponds to one realization of the random onsite potential, and each column corresponds to one eigenvalue of the Hamiltonian; the eigenvalues are complex and are not sorted. With these, the empirical distributions of the Complex Spacing ratios (Figures 13 and 14) can be obtained. The DSFF data is saved in the file 'sff_data_XY_3003_g_0.4.npz'. It stores a one-dimensional array of time values (times), a one-dimensional array of projection angles (phis), and the Hilbert-space dimension (D). For each angle, the file includes the sample-averaged spectral form factor (mean_SFF_label), the sample-averaged complex partition sum (mean_Z_label), and the sample average of the logarithm of the spectral form factor (mean_log_SFF_label), all stored as two-dimensional arrays with rows corresponding to different angles and columns corresponding to different times. Similar Constructions are available for the standard RMT spectra and the Random Energy Model

DOI
10.5281/zenodo.18220613

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These files serve to comply to the data availability statement for the publicpation of (https://arxiv.org/abs/2509.14406) to PRE. The 'Local Minima' python notebook is the code used to (after choosing/generating the desired spectrum) compute the SFF and the corresponding Y variable defined in Eq. (16) of the text, from which its empirical distribution shown or various cases (Figures 1,2,6,7,10,11 and A3 in the text) is readily obtained. Finally, the notebook also includes the computation of the local minima discussed in the beginning of Section V. The data can be then plotted as is done in Figures 8 and 12 in the text. The .npy files '3003_FORSFF.npy', '792_FORSFF.npy', etc. are examples of generated spectra for the Hermitian Model defined in Eq. (23) of the text. Each file is a NumPy array containing energy spectra for many independent disorder realizations of the model at fixed system size. The array has shape (n_samples, D), where n_samples is the number of realizations and D is the Hilbert-space dimension. Each row corresponds to one realization, and each column corresponds to an energy level; within each row, the eigenvalues are real and sorted in ascending order. From these spectra, the distribution of the local energy gap ratios defined in Eq. (19) can be empirically obtained as is shown in Fig. 4 of the text. Using these spectra, the Spectral Form Factor (Eq (1) and its quenched and annealed counterparts (Eq.s (7) and (8) respectively) are obtained. The corresponding data examples are given in 'D3003_sff_L_14_logtimes' and D792_sff_L_12_logtimes''. Each CSV file contains ensemble-averaged spectral form factor data computed from the corresponding eigenvalue file. Rows correspond to different time values, and columns store the time (time), the averaged spectral form factor (K), its disconnected part (K_disc), the connected contribution (K_conn), and the ensemble average of the logarithm of the spectral form factor (mean_lnSFF). The results for the quenched SFF are shown in Fig. 5 of the text The various DSFFs (Eq, (5)) for the Dissipative XY model defined in Eq. (25) are obtained using samples found in the file 'XY_spin_L_14_dim_3003_g_0.4.npy'. The file contains complex energy spectra of a bosonic lattice Hamiltonian for many independent disorder realizations at fixed model parameters. The stored array has shape (n_samples, dim), where n_samples is the number of disorder realizations and dim is the Hilbert-space dimension of the fixed-particle-number sector. Each row corresponds to one realization of the random onsite potential, and each column corresponds to one eigenvalue of the Hamiltonian; the eigenvalues are complex and are not sorted. With these, the empirical distributions of the Complex Spacing ratios (Figures 13 and 14) can be obtained. The DSFF data is saved in the file 'sff_data_XY_3003_g_0.4.npz'. It stores a one-dimensional array of time values (times), a one-dimensional array of projection angles (phis), and the Hilbert-space dimension (D). For each angle, the file includes the sample-averaged spectral form factor (mean_SFF_label), the sample-averaged complex partition sum (mean_Z_label), and the sample average of the logarithm of the spectral form factor (mean_log_SFF_label), all stored as two-dimensional arrays with rows corresponding to different angles and columns corresponding to different times. Similar Constructions are available for the standard RMT spectra and the Random Energy Model
This archive contains the numerical data and scripts used to generate the figures for the paper “Energy-selective quantum search with Ising Hamiltonian phase oracles”. The main numerical dataset is used for the scaling analysis of the correlation-induced resonance displacement φ₀ in the zero-field random Ising ensemble. The simulations use dimensionless units with σ_J = 1 and the Hamiltonian H(s) = 2 sum_{i<j} J_ij s_i s_j, where the couplings are independent Gaussian random variables, J_ij ~ N(0, 1), and h_i = 0. For each random Ising instance, the archive stores the truncated characteristic-function coefficients g_m = 2^{-n} Tr exp(-i m T H), m = 0, ..., 15. These coefficients are used to extract the local displacement φ₀ from the zero of the imaginary part of the response function C(φ) = 2 sum_{m=0}^{15} g_m (-1)^m exp(i m φ) - 1. The quantity plotted in the paper is the disorder-averaged second moment <φ₀²> and the scaled combination n⁶<φ₀²>. The Monte Carlo average is over independent disorder realizations only. For each realization, the trace over spin configurations is evaluated deterministically. The data cover even system sizes n = 18, 20, 22, ..., 36. For the largest systems, the computation splits the spins into two equal halves, performs GPU block contractions, and uses the zero-field spin-flip symmetry H(s)=H(-s) to reduce the sum by a factor of two. Archive contents - scripts/01_generate_phi0_coefficients.py Generates the characteristic-function coefficient files g_m for the random Ising ensemble. - scripts/02_analyze_phi0_scaling.py Computes φ₀, bootstrap confidence intervals, the finite-n covariance-sum comparison, and the scaling plots. - scripts/03_make_gaussian_amplification.py Generates the Gaussian amplification figure used as Fig. 1 in the paper. - data/phi0_coefficients/ Directory for the NumPy .npz files containing the characteristic-function coefficients. The production files have names of the form Nq_<n>_K_<K>.npz. The .npz files are saved without pickle objects. They can be read with standard NumPy using np.load. Typical usage To regenerate the Gaussian amplification figure: python scripts/03_make_gaussian_amplification.py --output-dir output/fig1_gaussian To analyze the φ₀ scaling data: python scripts/02_analyze_phi0_scaling.py \ --data-dir data/phi0_coefficients \ --output-dir output/phi0_scaling To run a short test calculation of the characteristic-function coefficients: python scripts/01_generate_phi0_coefficients.py \ --smoke-test \ --output-dir output/smoke_test_coefficients To regenerate the full production dataset on a CUDA-capable GPU: python scripts/01_generate_phi0_coefficients.py \ --production \ --output-dir data/phi0_coefficients The production calculations were performed using CuPy on an NVIDIA GPU. The analysis and plotting scripts use NumPy, pandas, and Matplotlib.
Shortcuts to adiabaticity with a quantum control field — Code & data========================================================== This repository contains a Jupyter notebook and supporting data files (csv) to reproduce the numerical results and figures in our manuscript (arXiv 2508.06304), which investigates adiabatic shortcuts mediated by a quantum control field.The code implements a Landau–Zener two-level system coupled to a spectator qubit, time evolution of the full system (LZ qubit + spectator) via QuTiP, parameter sweeps (parallelized with joblib), and plotting utilities for the manuscript figures. Related publication----------------------------This code is complementary to the preprint: https://arxiv.org/abs/2508.06304. Requirements---------------------The simulations were developed for and tested on Python 3.9+. Recommended packages and minimum versions: - Python >= 3.9- numpy >= 1.22- scipy >= 1.8- matplotlib >= 3.5- qutip >= 4.6 (install a recent stable qutip; some installations require `pip install qutip` or `conda` channels)- joblib >= 1.2- tqdm >= 4.60- pandas (optional, for CSV handling)- jupyterlab / notebook (for interactive use) Running the notebook (interactive) Open the notebook with JupyterLab or Jupyter Notebook. Execute cells sequentially in the order indicated by the notebook outline.The sections “Definitions” and “Figure imports and setup” must be executed before generating any data or figures, as they define all operators, and helper functions. The notebook is organized into separate sections for each figure of the manuscript, allowing you to re-run only the figure(s) of interest. Note: Figure 4 (Density plot) is configured to load precomputed data files to reduce computational cost. To reproduce Figure 4 without recomputing the full dataset, ensure the required .csv files are downloaded and located in the same directory as the notebook. To explore different parameter regimes: Modify the relevant parameter definitions (e.g., anneal_window, g, epsilon, omega_c, x0, x0_vals, q_vals). To include dissipation of the spectator (ancilla) qubit, set the parameter kappa> 0. For questions about reproducing the figures or about parameter choices used in the paper, contact the corresponding authors listed in the preprint. If you reuse this data/code, please cite the associated preprint and this code archive.
This repository contains the numerical data and computational codes supporting the results presented in the manuscript: "Engineered non-Gaussian Coherence as a Thermodynamic Resource for Quantum Batteries". The archive (data_QB.zip) includes all datasets, Jupyter notebooks, and figure files required to reproduce the results reported in both the main text and the Supplemental Material. Each figure is organised in a separate directory containing the corresponding data (.txt), code (.ipynb), and generated plots (.png/.pdf). The provided materials are sufficient to reproduce all figures and results without restriction. Detailed instructions and directory structure are described in the accompanying README.txt file. This dataset is made openly available to ensure transparency and reproducibility of the reported results.
This repository provides the figure data and numerical simulation codes supplement to the manuscript “Dynamical freezing and enhanced magnetometry in an interacting spin ensemble” (arXiv:2507.22982). Contents:--Main_text_figures--Extended_Data_figures Each folder contains the numerical or experimental data used to generate the corresponding figures in the manuscript. All figures can be reproduced by straightforward plotting of the included .csv files. A short description of each dataset is provided within the file headers. --Exact_diagonalization_code--Discrete_truncated_Wigner_approximation_code These directories contain the codes used in the numerical simulations presented in the paper. Each code package includes a detailed README file explaining the workflow, parameters, and usage.
We provide the numerical codes to produce the data contained in "Competition between pair and single-particle superfluidity in bosonic quasi-flat bands: A Gaussian state approach", https://arxiv.org/abs/2605.26231, as well as notebooks to plot them. v1 contains a minimal version of Python and Julia codes. v2 provides the final version of the plots, explicitly stores data used in the plots and avoids Julia notebooks (in order to avoid compatibility issues). The LaTeX script allows to generate the manuscipt. Some of the Python codes rely on the external library QuSpin.py.