ed-lgt
Code for Exact Diagonalization of Quantum Many-Body Hamiltonians and Lattice (Abelian and Non-Abelian) Gauge Theories in D=1,2,3 spatial dimensions
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Repository
Code for Exact Diagonalization of Quantum Many-Body Hamiltonians and Lattice (Abelian and Non-Abelian) Gauge Theories in D=1,2,3 spatial dimensions
Basic Info
- Host: GitHub
- Owner: gcataldi96
- License: apache-2.0
- Language: Python
- Default Branch: main
- Size: 1.47 MB
Statistics
- Stars: 2
- Watchers: 1
- Forks: 0
- Open Issues: 0
- Releases: 1
Metadata Files
README.md
Exact_Diagonalization
Code for Exact Diagonalization of Quantum Many-Body Hamiltonians and Lattice Gauge Theories.
Read the whole Documentation on https://ed-su2.readthedocs.io/en/latest/
Setup
1) Download from git the repository
git clone --recursive git@github.com:gcataldi96/ed-lgt.git
2) Create the Environment with all the needed python packages
conda env create -f ed-lgt/environment.yml
conda activate ed
3) Install the library
cd ed-lgt/
pip install -e .
Enjoy 👏
Configure Simsio Simulations
Just in case you want to use Simsio to run simulations, do the following steps:
1) (ignore it unless you create the repo for the first time) Add the simsio library as a submodule (it should be already there)
git submodule add https://github.com/rgbmrc/simsio.git
git add .
git commit -m "Add simsio submodule to the TTN code"
2) Update and get all the submodules
git submodule update
git submodule recursive
This is an example of a config file that should be created inside the folder configs (if this latter does not exist, create the directory):
===:
template: |
n$enum:
<<<: common
g: $g
common:
dim: 2
lvals: [2,2]
pure: false
has_obc: false
DeltaN: 2
m: 1.0
n0:
<<<: common
g: j0
n1:
<<<: common
g: j1
where j0 and j1 are two values of g that one would like to simulate.
If you want to create a larger set of simulations automatically, run a script like the following:
from simsio import gen_configs
import numpy as np
params = {"g": np.logspace(-1, 1, 10)}
gen_configs("template", params, "config_NAME_FILE")
Then, in "configNAMEFILE.yaml" it will add simulations like
ni:
<<<: common
g: j
where
$i$ is the $i^{th}$ simulation corresponding to the model with the g-parameter (which is not common to all the other simulations) equal to $j$.
Run Simulations
To run simulations, just type on the command shell the following command. On linux:
nohup bash -c "printf 'n%s\n' {0..N} | shuf | xargs -PA -i python script.py config_NAME_FILE {} B" &>/dev/null &
On MAC:
nohup bash -c "printf 'n%s\n' {0..N} | xargs -PA -I% python script.py config_NAME_FILE % B" &>/dev/null &
where
1) N is the total number of simulations in the configfilename,
2) A is the number of processes in parallel
3) B is the number of single-node threads per simulation
Owner
- Name: Giovanni Cataldi
- Login: gcataldi96
- Kind: user
- Company: University of Padua
- Website: https://giocataldi.com/
- Repositories: 4
- Profile: https://github.com/gcataldi96
I am a PhD student in Physics at the University of Padua. I am interested in Quantum Many-Body Systems and Tensor Network simulations
Citation (CITATION.cff)
cff-version: 1.2.0
title: ed-lgt
message: >-
If you use this software, please cite it using the
metadata from this file.
type: software
authors:
- given-names: Giovanni
family-names: Cataldi
email: giovacataldi96@gmail.com
affiliation: University of Padua
orcid: 'https://orcid.org/0000-0002-9073-8978'
repository-code: 'https://github.com/gcataldi96/ed-lgt'
abstract: >-
The Exact Diagonalization Library for Lattice Gauge
Theories provides a powerful set of tools for performing
exact diagonalization calculations on d-dimensional
lattices, specifically targeting both Abelian and
non-Abelian Lattice Gauge Theories. This library empowers
researchers and practitioners in the field of quantum
many-body systems to analyze and explore the behavior of
complex lattice gauge theories through the precise
computation of Hamiltonian eigenvalues and eigenvectors.
keywords:
- Lattice Gauge Theories
- Exact Diagonalization
- Quantum Many Body Systems
license: Apache-2.0
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