Quantum-Commutator of Many-Body Operators based on generalized Wick theorem
Project description
QCombo: Automated Commutator Calculation for Quantum Many-Body Operators
QCombo is a Python library for automated computation of commutators for normal-ordered many-body operators based on the generalized Wick theorem. Designed specifically for nuclear physics and condensed matter applications, it provides efficient and accurate tools for handling complex quantum many-body calculations.
Table of Contents
- Overview
- Features
- Installation
- Directory Structure
- Quick Start
- Command Line Interface
- Python API Usage
- Index Conventions
- Examples
- Applications
- Testing
- Citation
- License
- Support
Overview
Background and Motivation
In quantum mechanics, operator commutators form the foundation of theoretical calculations. In nuclear physics, ab initio methods (such as NCSM, CC, IMSRG, etc.) are essential tools for studying nuclear many-body systems. These methods start from nuclear forces constructed from chiral effective field theory and provide approximate but rigorous solutions to quantum many-body problems.
As the number of many-body terms increases, the number of terms in commutators grows exponentially, making manual calculations extremely tedious and error-prone. QCombo addresses this challenge by providing an automated solution for computing commutators of normal-ordered many-body operators.
Features
- Based on Generalized Wick Theorem: Implements automated computation of commutators for normal-ordered many-body operators
- Many-Body Coupling Support: Handles commutators of arbitrary-order many-body operators
- Automated Output Generation:
- Generates LaTeX files for commutator expressions
- Produces input files for the AMC software package to obtain expressions in J-scheme
- Flexible Configuration: Allows specification of output to specific many-body ranks
- Symbolic Computation: Built on SymPy for precise algebraic manipulations
- Command Line Interface: Easy-to-use terminal commands for quick calculations
- Interactive Mode: Step-by-step guided interface for exploratory calculations
Installation
Install from PyPI (Recommended)
pip install qcombo
Install from Source
git clone https://github.com/chenlh73/qcombo.git
cd qcombo
pip install -e .
Note that for the first execution, running "pip install -e ."n the terminal may be required to activate the qcombo library in the current directory before the examples can be run.
System Requirements
- Python >= 3.12
- SymPy >= 1.13.3
You can install Sympy from PyPI
pip install sympy
as you run the jupter notebook, you may need to install ipython libraty
pip install ipython
Directory Structure
The directory structure of the qcombo package is organized to clearly separate core code, packaging configurations, and example resources. Below is a breakdown of key components:
qcombo/ # Root directory of the Python package.
├── qcombo/ # Core computation modules.
│ ├── __init__.py # Marks the qcombo directory as a Python package.
│ ├── __main__.py # Entry point for command-line interface (enables qcombo to run via terminal).
│ ├── canonical.py # Implements core algorithms for canonical commutator computations.
│ ├── output.py # Handles generation of LaTeX/AMC-formatted output files.
│ ├── simplify.py # Provides symbolic simplification utilities using SymPy.
│ ├── tools.py # Contains helper functions for operator manipulation.
│ └── wickcalculate.py # Applies the generalized Wick theorem for commutator calculation.
├── examples/ # Example notebooks and scripts demonstrating various use cases.
│ ├── easyCombo_Guide.ipynb # Comprehensive guide for using the easyCombo function.
│ ├── MR_IMSRG2.ipynb # Multi-reference IMSRG(2) flow equation example.
│ ├── SR_IMSRG3.ipynb # Single-reference IMSRG(3) flow equation example.
│ ├── Brillouin.ipynb # Demonstration of Brillouin's theorem.
│ ├── Product_1B1B.ipynb # Product of two one-body operators.
│ ├── easyCombo.py # Python script example for easyCombo usage.
│ ├── easyCombo_110.py # Python script example for [1B,1B] commutator coupled to 0-body.
│ ├── qcombo_to_amc.ipynb # Workflow for converting QCombo results to AMC input.
│ └── results/ # Output files generated from example scripts.
├── test/ # Test notebooks for validating correctness.
│ ├── FunctionTest.ipynb # Comprehensive function tests.
│ ├── Jacobi_Identity.ipynb # Verification of Jacobi identity for commutators.
│ ├── CommutatorAntisymmetry.ipynb # Tests for antisymmetry properties.
│ ├── Indices_test.ipynb # Tests for index manipulation functions.
│ └── parallelTest.ipynb # Tests for parallel computing functionality.
├── results/ # Example output files from typical calculations.
│ ├── commutator_*.tex # LaTeX output files for various commutator calculations.
│ └── commutator_*.amc # AMC input files for various commutator calculations.
├── LICENSE # Open-source license file (MIT License).
├── README.md # Main documentation file (this document).
├── setup.cfg # Configuration file for setuptools (specifies build/distribution rules).
└── setup.py # Script for building and distributing the Python package.
Quick Start
Command Line Interface (Recommended)
After installation, you can use QCombo directly from the command line:
# Compute the [2B, 2B] commutator with all possible contractions
qcombo 2 2
# Compute only 0-body and 1-body contractions
qcombo 2 2 -c 0,1
# Compute with range of contractions (0-2 body)
qcombo 1 3 -c 0-2
# Specify custom output filenames
qcombo 2 2 -c 0,1,2 --latex-output my_result.tex --amc-output my_result.txt
# Use specific indices (Python list syntax)
qcombo "[['a','b'], ['c','d']]" "[['e','f','g'], ['h','i','j']]" -c 0,1,2
# Use single-reference Wick's theorem mode
qcombo 2 2 -w SR
# Enable parallel computing
qcombo 2 2 --parallel
# Start interactive mode
qcombo
# or explicitly:
qcombo -i
# Show help message
qcombo --help
# Show version information
qcombo --version
Python API
You can also use QCombo within Python scripts:
import qcombo
# Compute the [2B, 2B] commutator coupled to all possible many-body ranks
qcombo.easyCombo(2, 2)
# Output only terms coupled to 0-body and 1-body ranks
qcombo.easyCombo(2, 2, [0, 1])
Command Line Interface
Basic Usage
QCombo provides a powerful command-line interface that allows you to perform calculations directly from your terminal:
qcombo LEFT RIGHT [OPTIONS]
Where:
LEFT: Number of particles in left operator (integer) or index list (Python list string)RIGHT: Number of particles in right operator (integer) or index list (Python list string)
Command Line Options
| Option | Short | Description | Example |
|---|---|---|---|
--contraction |
-c |
Contraction body numbers: single integer(0), range(0-2), list(0,1,2), or 'all' (calculate all) | qcombo 2 2 -c 0,1,2 |
--latex-output |
-lo |
LaTeX output filename | qcombo 2 2 -lo result.tex |
--amc-output |
-ao |
AMC program input file output name | qcombo 2 2 -ao result.txt |
--wick-mode |
-w |
Wick's theorem mode: 'SR' (single-reference) or 'MR' (multi-reference). Default: MR | qcombo 2 2 -w SR |
--no-process |
-ns |
Disable the process bar of calculation | qcombo 2 2 --no-process |
--parallel |
-p |
Enable parallel computing using ProcessPoolExecutor | qcombo 2 2 --parallel |
--version |
-v |
Show version information | qcombo --version |
--quiet |
-q |
Quiet mode, reduce output (also disables process bar) | qcombo 2 2 -q |
--interactive |
-i |
Start interactive mode | qcombo -i |
Interactive Mode
For exploratory calculations, QCombo offers an interactive mode that guides you through the process step-by-step:
qcombo
Or explicitly:
qcombo -i
In interactive mode, you will be prompted for:
- Left operator (integer or index list)
- Right operator (integer or index list)
- Contraction body numbers
- Wick's theorem mode ('SR' or 'MR')
- Show process bar (y/n)
- Enable parallel computing (y/n)
- Output filenames (optional)
Examples
Basic calculations:
# 2-body with 2-body operator commutator
qcombo 2 2
# 1-body with 3-body operator commutator
qcombo 1 3
# 2-body with 2-body, only 0-body and 1-body terms
qcombo 2 2 -c 0,1
# Enable parallel computing for large calculations
qcombo 2 3 --parallel
With custom indices:
# Using specific index lists
qcombo "[['a','b'], ['c','d']]" "[['e','f'], ['g','h']]"
# Using range contractions
qcombo "[['i','j'], ['k','l']]" "[['m','n','o'], ['p','q','r']]" -c 0-2
With output files:
# Save results to specific files
qcombo 2 2 --latex-output commutator.tex --amc-output commutator.txt
# Using short options
qcombo 2 2 -c 0,1,2 -lo result.tex -ao result.txt
Python API Usage
Function Parameters
qcombo.easyCombo(left, right, contraction=None, latexOutput=None, amcOutput=None, **kwargs)
left: Many-body rank of the first operator (integer) or index listright: Many-body rank of the second operator (integer) or index listcontraction: Optional parameter specifying output ranks- Example:
[0, 1]outputs only zero-body and one-body terms None(default) outputs all possible many-body terms
- Example:
latexOutput: Custom LaTeX output filenameamcOutput: Custom AMC input filename**kwargs: Optional keyword argumentswick_mode:'SR'(single-reference) or'MR'(multi-reference). Default:'MR'show_process: Whether to display progress bar. Default:Trueparallel: Enable parallel computing using ProcessPoolExecutor. Default:False
Basic Examples
import qcombo
# Compute [2B, 2B] commutator
result = qcombo.easyCombo(2, 2)
# Compute with specific contractions
result = qcombo.easyCombo(2, 2, contraction=[0, 1])
# Compute with custom output files
result = qcombo.easyCombo(2, 2,
contraction=[0, 1, 2],
latexOutput="my_commutator.tex",
amcOutput="my_commutator.txt")
# Compute with single-reference mode and disable parallel computing
result = qcombo.easyCombo(2, 2, contraction=[0, 1],
wick_mode='SR', show_process=False, parallel=False)
# Compute with specific indices
left_indices = [['a', 'b'], ['c', 'd']]
right_indices = [['e', 'f', 'g'], ['h', 'i', 'j']]
result = qcombo.easyCombo(left_indices, right_indices, contraction=[0, 1])
Output Description
After execution, QCombo generates:
- Console Output: Displays the computed commutator expressions in formatted text
- LaTeX Files: Generated expressions in LaTeX format (ready for inclusion in papers)
- AMC Input Files: Input files for the AMC software package to obtain expressions in J-scheme
The output filenames follow the pattern:
- LaTeX:
commutator_[left]B[right]B_to_[contractions]B.tex - AMC:
commutator_[left]B[right]B_to_[contractions]B.amc
For example: commutator_2B2B_to_0_1_2B.tex, commutator_2B2B_to_0_1_2B.amc
Output Format
The returned result is a dictionary where keys are strings in the format '{filter_body}B_lambda{lambda_body}B' and values are SymPy expressions:
{
'0B_lambda1B': sympy_expression_1,
'0B_lambda2B': sympy_expression_2,
# ...
}
Example Output
For example, compute the commutator of two normal-ordered one-body operators contracting to zero-body:
qcombo.easyCombo(1, 1, 0)
In the output file commutator_1B1B_to_0B.tex, the equation is expected to be:
$$R^{}{} = \sum{ab} (n^{}{a}-n^{}{b}) G^{a}{b} H^{b}{a}$$
In the output file commutator_1B1B_to_0B.amc, the equation is expected to be:
declare G{mode= (1,1),latex ="G" }
declare H{mode= (1,1),latex ="H" }
declare R0{mode= (0,0),latex ="R" }
declare n { mode=2, diagonal=true, latex="n"}
# commutator [1B,1B]-0B
# lambda_1B
R0 = 1*sum_ab((n_a-n_b)*G_ab*H_ba);
Index Conventions
QCombo uses a specific index notation based on the generalized Wick theorem for normal-ordered many-body operators. Understanding these conventions is essential for correctly interpreting input and output expressions.
Upper and Lower Indices
In second quantization, a many-body operator is expressed in terms of creation and annihilation operators. QCombo represents the matrix elements of such operators using upper indices (creation/particle indices) and lower indices (annihilation/hole indices):
Operator: O = Σ O^{a₁a₂...}_{b₁b₂...} a†_{a₁} a†_{a₂} ... a_{b₂} a_{b₁}
In QCombo's SymPy representation:
O[(a1, a2, ...), (b1, b2, ...)] # upper tuple, lower tuple
Example: A two-body operator G with upper indices a, b and lower indices c, d:
G[(a, b), (c, d)] # represents G^{ab}_{cd}
Normal Ordering and the A Operator
QCombo expresses all results in terms of normal-ordered products with respect to a reference state (Fermi vacuum). The normal-ordering symbol is represented by the tensor A:
A[(a, b), (c, d)] # normal-ordered product: {a†_a a†_b a_d a_c}
The indices of A are the external (free) indices of the commutator result and are NOT summed over. They define the many-body rank of the output term:
A[(), ()]→ 0-body (scalar) termA[(a,), (b,)]→ 1-body termA[(a, b), (c, d)]→ 2-body term
Special Tensors
The generalized Wick theorem introduces the following contraction tensors:
| Symbol | Name | Meaning |
|---|---|---|
λ (lambda) |
Irreducible density matrix | λ^{a₁...}_{b₁...},one-body is particle density matrix λ^i_j = ⟨a†_i a_j⟩ |
ξ (xi) |
Hole density | ξ^i_j = λ^i_j - δ^i_j, only has one-body |
δ (delta) |
Kronecker delta | δ^a_b = 1 if a = b, else 0 |
n |
Occupation number | n_a = ⟨a†_a a_a⟩, diagonal part of the one-body density |
In MR (multi-reference) mode, λ can be multi-body (e.g., λ^{ab}_{cd} for 2-body density).
In SR (single-reference) mode, only the one-body λ^a_b is non-zero,
In Natural Orbital Basis the one-body lambda simplifies to:
λ^a_b = n_a · δ^a_b
Dummy Indices vs. Free Indices
- Free indices: Indices that appear exactly once in a term. These are the indices of the
Aoperator and define the output many-body rank. - Dummy indices: Indices that appear exactly twice (once upper, once lower) and are summed over. They can be freely renamed without changing the value of the expression.
Example:
Σ_p G^{ap}_{cd} · H^{eb}_{pf} # p is a dummy index (summed)
# a, b, c, d, e, f are free indices
Antisymmetry
Matrix elements in QCombo are fully antisymmetric under exchange of upper indices or lower indices:
G^{ab}_{cd} = -G^{ba}_{cd} = -G^{ab}_{dc} = G^{ba}_{dc}
This property is automatically exploited during simplification to combine equivalent terms.
Input Format
When specifying operators by integer rank, QCombo automatically assigns indices from a predefined alphabetical list ['a', 'b', 'c', ...]:
# left = 2 means a 2-body operator with indices [['a','b'], ['c','d']]
# right = 2 means a 2-body operator with indices [['e','f'], ['g','h']]
qcombo.easyCombo(2, 2)
You can also specify custom indices explicitly:
left = [['i', 'j'], ['k', 'l']] # upper indices [i,j], lower [k,l]
right = [['p', 'q'], ['r', 's']]
qcombo.easyCombo(left, right)
Examples
QCombo includes a rich collection of example notebooks in the examples/ directory:
Getting Started
| Notebook | Description |
|---|---|
| easyCombo_Guide.ipynb | Comprehensive guide covering all features of the easyCombo function |
| Product_1B1B.ipynb | Simple example: product of two one-body operators |
Physics Applications
| Notebook | Description |
|---|---|
| MR_IMSRG2.ipynb | Multi-reference IMSRG(2) flow equations |
| SR_IMSRG3.ipynb | Single-reference IMSRG(3) flow equations |
| Brillouin.ipynb | Verification of Brillouin generator |
Advanced Usage
| Notebook | Description |
|---|---|
| qcombo_to_amc.ipynb | Complete workflow from QCombo calculation to AMC input file generation |
| easyCombo_110.ipynb | [1B, 1B] commutator coupled to 0-body term |
Python Script Examples
For users who prefer Python scripts over Jupyter notebooks:
- easyCombo.py - Basic usage example
- easyCombo_110.py - [1B, 1B] commutator example
Applications
Nuclear Physics Applications
In nuclear ab initio methods, QCombo can be used for:
- IMSRG Flow Equations: Computing commutators between generators and Hamiltonians
- Similarity Renormalization Group (SRG): Evaluating flow equations
- Configuration Interaction: Deriving effective interactions
Education and Research
QCombo is also valuable for quantum mechanics education and research:
- Verifying theoretical derivations
- Exploring contributions from higher-order many-body terms
- Automating tedious symbolic calculations
- Teaching quantum many-body theory concepts
Testing
QCombo includes test notebooks in the test/ directory to validate correctness:
| Notebook | Description |
|---|---|
| FunctionTest.ipynb | Comprehensive tests for all core functions |
| Jacobi_Identity.ipynb | Verification that commutators satisfy the Jacobi identity |
| CommutatorAntisymmetry.ipynb | Tests for antisymmetry properties of commutators |
| Indices_test.ipynb | Tests for index manipulation and simplification functions |
| parallelTest.ipynb | Validation of parallel computing results |
Running Tests
Open the test notebooks in Jupyter:
jupyter notebook test/
Run all cells in each notebook to verify correctness. The notebooks include:
- Expected output comparisons
- Algebraic identity verifications
- Parallel vs. serial result consistency checks
Citation
If you use QCombo in your research, please cite:
@misc{chen2026qcombo,
title={Qcombo: A Python Package for Automated Commutator Calculations of Quantum Many-Body Operators},
author={L. H. Chen and Y. Li and H. Hergert and J. M. Yao},
year={2026},
eprint={2603.24399},
archivePrefix={arXiv},
primaryClass={nucl-th},
url={https://arxiv.org/abs/2603.24399},
}
License
This project is licensed under the MIT License - see the LICENSE file for details.
Support
- Issues: Report bugs or request features on GitHub Issues: https://github.com/chenlh73/qcombo/issues
- Documentation: Visit the GitHub repository for more information: https://github.com/chenlh73/qcombo
- Questions: Contact the development team via email
*QCombo - Quantum Commutator of Many-Body operator *
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