blocksolver 0.9.3

Block Quasi-Minimal-Residual sparse linear solver

BlockSolver - Block Quasi-Minimal Residual (BLQMR) Sparse Linear Solver

• Copyright: (C) Qianqian Fang (2005, 2011, 2026) <q.fang at neu.edu>
• License: BSD-3-Clause and GPL-v3 dual-licensed
• Version: 0.9.3
• Website: https://neurojson.org/Page/blocksolver
• Github: https://github.com/fangq/blit
• PyPi Page: https://pypi.org/project/blocksolver/

BlockSolver is a Python package for solving large sparse linear systems using the Block Quasi-Minimal Residual (BLQMR) algorithm. It provides both a high-performance Fortran backend and a pure Python/NumPy implementation for maximum portability.

Features

• Block QMR Algorithm: Efficiently solves multiple right-hand sides simultaneously
• Complex Symmetric Support: Designed for complex symmetric matrices (A = Aᵀ, not A = A†)
• Dual Backend: Fortran extension for speed, Python fallback for portability
• Flexible Preconditioning: ILU, diagonal (Jacobi), and split preconditioners
• SciPy Integration: Works seamlessly with SciPy sparse matrices
• Optional Numba Acceleration: JIT-compiled kernels for the Python backend

Algorithm

Block Quasi-Minimal Residual (BLQMR)

The BLQMR algorithm is an iterative Krylov subspace method specifically designed for:

1. Complex symmetric systems: Unlike standard methods that assume Hermitian (A = A†) or general matrices, BLQMR exploits complex symmetry (A = Aᵀ) which arises in electromagnetics, acoustics, and diffuse optical tomography.

2. Multiple right-hand sides: Instead of solving each system independently, BLQMR processes all right-hand sides together in a block fashion, sharing Krylov subspace information and reducing total computation.

3. Quasi-minimal residual: The algorithm minimizes a quasi-residual norm at each iteration, providing smooth convergence without the erratic behavior of some Krylov methods.

Key Components

• Quasi-QR Decomposition: A modified Gram-Schmidt process using the quasi inner product ⟨x,y⟩ = Σ xₖyₖ (without conjugation) for complex symmetric systems.

• Three-term Lanczos Recurrence: Builds an orthonormal basis for the Krylov subspace with short recurrences, minimizing memory usage.

• Block Updates: Processes m right-hand sides simultaneously, with typical block sizes of 1-64.

When to Use BLQMR

Use Case	Recommendation
Complex symmetric matrix (A = Aᵀ)	✅ Ideal
Multiple right-hand sides	✅ Ideal
Real symmetric positive definite	Consider CG first
General non-symmetric	Consider GMRES or BiCGSTAB
Very large systems (>10⁶ unknowns)	✅ Good with preconditioning

Installation

From PyPI

pip install blocksolver

From Source

Prerequisites:

• Python ≥ 3.8
• NumPy ≥ 1.20
• SciPy ≥ 1.0
• (Optional) Fortran compiler + UMFPACK for the accelerated backend
• (Optional) Numba for accelerated Python backend

# Ubuntu/Debian
sudo apt install gfortran libsuitesparse-dev libblas-dev liblapack-dev

# macOS
brew install gcc suite-sparse openblas

# Install
cd python
pip install .

Quick Start

import numpy as np
from scipy.sparse import csc_matrix
from blocksolver import blqmr

# Create a sparse matrix
A = csc_matrix([
    [4, 1, 0, 0],
    [1, 4, 1, 0],
    [0, 1, 4, 1],
    [0, 0, 1, 4]
], dtype=float)

b = np.array([1., 2., 3., 4.])

# Solve Ax = b
result = blqmr(A, b, tol=1e-10)

print(f"Solution: {result.x}")
print(f"Converged: {result.converged}")
print(f"Iterations: {result.iter}")
print(f"Relative residual: {result.relres:.2e}")

Usage

Main Interface: blqmr()

The primary function blqmr() automatically selects the best available backend (Fortran if available, otherwise Python).

from blocksolver import blqmr, BLQMR_EXT

# Check which backend is active
print(f"Using Fortran backend: {BLQMR_EXT}")

# Basic usage
result = blqmr(A, b)

# With options
result = blqmr(A, b, 
    tol=1e-8,              # Convergence tolerance
    maxiter=1000,          # Maximum iterations
    precond_type='ilu',    # Preconditioner: 'ilu', 'diag', or None
)

Multiple Right-Hand Sides

BLQMR excels when solving the same system with multiple right-hand sides:

import numpy as np
from blocksolver import blqmr

# 100 different right-hand sides
B = np.random.randn(n, 100)

# Solve all systems at once (much faster than solving individually)
result = blqmr(A, B, tol=1e-8)

# result.x has shape (n, 100)

Complex Symmetric Systems

BLQMR is specifically designed for complex symmetric matrices (common in frequency-domain wave problems):

import numpy as np
from blocksolver import blqmr

# Complex symmetric matrix (A = A.T, NOT A.conj().T)
A = create_helmholtz_matrix(frequency=1000)  # Your application
b = np.complex128(source_term)

result = blqmr(A, b, tol=1e-8, precond_type='diag')

Preconditioning

BlockSolver supports multiple preconditioner types for both backends:

from blocksolver import blqmr, make_preconditioner

# Using precond_type parameter (works with both backends)
result = blqmr(A, b, precond_type='ilu')    # Incomplete LU
result = blqmr(A, b, precond_type='diag')   # Diagonal (Jacobi)
result = blqmr(A, b, precond_type=None)     # No preconditioning

# Custom preconditioner (Python backend only)
M1 = make_preconditioner(A, 'ilu', drop_tol=1e-4, fill_factor=10)
result = blqmr(A, b, M1=M1, precond_type=None)

# Split preconditioning for symmetric systems (Python backend)
# Preserves symmetry: M1^{-1} A M2^{-1}
M = make_preconditioner(A, 'diag', split=True)  # Returns sqrt(D)
result = blqmr(A, b, M1=M, M2=M, precond_type=None)

SciPy-Compatible Interface

For drop-in replacement in existing code:

from blocksolver import blqmr_scipy

# Returns (x, flag) like scipy.sparse.linalg solvers
x, flag = blqmr_scipy(A, b, tol=1e-10)

Low-Level CSC Interface

For maximum control, use the CSC component interface:

from blocksolver import blqmr_solve

# CSC format components (0-based indexing)
Ap = np.array([0, 2, 5, 9, 10, 12], dtype=np.int32)  # Column pointers
Ai = np.array([0, 1, 0, 2, 4, 1, 2, 3, 4, 2, 1, 4], dtype=np.int32)  # Row indices
Ax = np.array([2., 3., 3., -1., 4., 4., -3., 1., 2., 2., 6., 1.])  # Values
b = np.array([8., 45., -3., 3., 19.])

result = blqmr_solve(Ap, Ai, Ax, b, 
    tol=1e-8,
    droptol=0.001,         # ILU drop tolerance (Fortran backend only)
    precond_type='ilu',    # Preconditioner type
    zero_based=True,       # 0-based indexing (default)
)

API Reference

blqmr(A, B, **kwargs) -> BLQMRResult

Main solver interface.

Parameters:

Parameter	Type	Default	Description
A	sparse matrix or ndarray	required	System matrix (n × n)
B	ndarray	required	Right-hand side (n,) or (n × m)
tol	float	1e-6	Convergence tolerance
maxiter	int	n	Maximum iterations
M1, M2	preconditioner	None	Custom preconditioners (Python backend)
x0	ndarray	None	Initial guess
precond_type	str or None	'ilu'	Preconditioner: 'ilu', 'diag', or None
droptol	float	0.001	ILU drop tolerance (Fortran backend)
residual	bool	False	Use true residual for convergence (Python)
workspace	BLQMRWorkspace	None	Pre-allocated workspace (Python)

Returns: BLQMRResult object with:

Attribute	Type	Description
x	ndarray	Solution vector(s)
flag	int	0=converged, 1=maxiter, 2=precond fail, 3=stagnation
iter	int	Iterations performed
relres	float	Final relative residual
converged	bool	True if flag == 0
resv	ndarray	Residual history (Python backend only)

blqmr_solve(Ap, Ai, Ax, b, **kwargs) -> BLQMRResult

Low-level CSC interface for single RHS.

blqmr_solve_multi(Ap, Ai, Ax, B, **kwargs) -> BLQMRResult

Low-level CSC interface for multiple right-hand sides.

blqmr_scipy(A, b, **kwargs) -> Tuple[ndarray, int]

SciPy-compatible interface returning (x, flag).

make_preconditioner(A, precond_type, **kwargs) -> Preconditioner

Create a preconditioner for the Python backend.

Parameters:

Parameter	Type	Default	Description
A	sparse matrix	required	System matrix
precond_type	str	required	'diag', 'jacobi', 'ilu', 'ilu0', 'ilut', 'lu', 'ssor'
split	bool	False	Return sqrt(D) for split preconditioning
drop_tol	float	1e-4	Drop tolerance for ILUT
fill_factor	float	10	Fill factor for ILUT
omega	float	1.0	Relaxation parameter for SSOR

Utility Functions

from blocksolver import (
    BLQMR_EXT,        # True if Fortran backend available
    HAS_NUMBA,        # True if Numba acceleration available
    get_backend_info, # Returns dict with backend details
    test,             # Run built-in tests
)

Benchmarks

BLQMR vs Direct Solver (mldivide)

Complex symmetric FEM matrices, 4 right-hand sides, tolerance 10⁻⁸, split Jacobi preconditioner:

Grid	Nodes	NNZ	mldivide	BLQMR	Speedup
20³	8,000	110K	135ms	115ms	1.2×
30³	27,000	384K	1.36s	373ms	3.6×
40³	64,000	922K	6.40s	947ms	6.8×
50³	125,000	1.8M	25.9s	1.76s	14.7×

Block Size Efficiency

With 64 RHS on a 8,000-node complex symmetric system:

Block Size	Iterations	Speedup vs Single
1 (point)	10,154	1.0×
4	2,220	1.8×
8	956	2.0×
16	361	2.1×
32	178	2.2×

Optimal block size: 8-16 for most problems. Larger blocks have diminishing returns due to increased per-iteration cost.

Iteration Efficiency

With 4 RHS, BLQMR uses only ~24% of total iterations compared to 4 separate single-RHS solves — achieving super-linear block acceleration.

Performance Tips

1. Use the Fortran backend when available (faster for large systems)

2. Enable preconditioning for ill-conditioned systems:

   result = blqmr(A, b, precond_type='ilu')
   

3. Batch multiple right-hand sides instead of solving one at a time:

   # Fast: single call with all RHS
   result = blqmr(A, B_matrix)
   
   # Slow: multiple calls
   for b in B_columns:
       result = blqmr(A, b)
   

4. Install Numba for faster Python backend:

   pip install numba
   

5. Reuse workspace for repeated solves with the same dimensions:

   from blocksolver import BLQMRWorkspace
   ws = BLQMRWorkspace(n, m, dtype=np.complex128)
   for b in many_rhs:
       result = blqmr(A, b, workspace=ws)
   

6. Use split Jacobi for complex symmetric systems:

   # Preserves symmetry of preconditioned system
   M = make_preconditioner(A, 'diag', split=True)
   result = blqmr(A, b, M1=M, M2=M, precond_type=None)
   

Examples

Diffuse Optical Tomography

import numpy as np
from scipy.sparse import diags, kron, eye
from blocksolver import blqmr

def create_diffusion_matrix(nx, ny, D=1.0, mu_a=0.01, omega=1e9):
    """Create 2D diffusion matrix for DOT."""
    n = nx * ny
    h = 1.0 / nx
    
    # Laplacian
    Lx = diags([-1, 2, -1], [-1, 0, 1], shape=(nx, nx)) / h**2
    Ly = diags([-1, 2, -1], [-1, 0, 1], shape=(ny, ny)) / h**2
    L = kron(eye(ny), Lx) + kron(Ly, eye(nx))
    
    # Diffusion equation: (-D∇² + μ_a + iω/c) φ = q
    c = 3e10  # speed of light in tissue (cm/s)
    A = -D * L + mu_a * eye(n) + 1j * omega / c * eye(n)
    
    return A.tocsc()

# Setup problem
A = create_diffusion_matrix(100, 100, omega=2*np.pi*100e6)
sources = np.random.randn(10000, 16) + 0j  # 16 source positions

# Solve for all sources at once
result = blqmr(A, sources, tol=1e-8, precond_type='diag')
print(f"Solved {sources.shape[1]} systems in {result.iter} iterations")

Frequency-Domain Acoustics

import numpy as np
from blocksolver import blqmr

# Helmholtz equation: (∇² + k²)p = f
# Results in complex symmetric matrix

def solve_helmholtz(K, M, f, frequencies):
    """Solve Helmholtz at multiple frequencies."""
    solutions = []
    for omega in frequencies:
        # A = K - ω²M (complex symmetric if K, M are symmetric)
        A = K - omega**2 * M
        result = blqmr(A, f, tol=1e-10, precond_type='diag')
        solutions.append(result.x)
    return np.array(solutions)

Troubleshooting

"No Fortran backend available"

Install the package with Fortran support:

# Install dependencies first
sudo apt install gfortran libsuitesparse-dev  # Linux
brew install gcc suite-sparse                  # macOS

# Reinstall blocksolver
pip install --no-cache-dir blocksolver

Check backend status

from blocksolver import get_backend_info
print(get_backend_info())
# {'backend': 'binary', 'has_fortran': True, 'has_numba': True}

Slow convergence

1. Enable preconditioning: precond_type='ilu' or precond_type='diag'
2. Reduce ILU drop tolerance: droptol=1e-4 (Fortran backend)
3. Check matrix conditioning with np.linalg.cond(A.toarray())

ILU factorization fails

For indefinite or complex symmetric matrices, ILU may fail:

# Fall back to diagonal preconditioner
result = blqmr(A, b, precond_type='diag')

Memory issues with large systems

1. Use the Fortran backend (more memory efficient)
2. Reduce block size for multiple RHS
3. Use iterative refinement instead of tighter tolerance

License

BSD-3-Clause or GPL-3.0+ (dual-licensed)

Citation

If you use BlockSolver in your research, please cite:

@software{blocksolver,
  author = {Qianqian Fang},
  title = {BlockSolver: Block Quasi-Minimal Residual Sparse Linear Solver},
  url = {https://github.com/fangq/blit},
  year = {2024}
}

See Also

• BLIT - The underlying Fortran library
• SciPy sparse.linalg - Other iterative solvers
• PyAMG - Algebraic multigrid solvers