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hypercomplex-engine

License: MIT Python 3.8+ Tests

Fast, validated multiplication and table generation for Cayley–Dickson algebras.

This library provides the computational substrate for high-dimensional hypercomplex algebra, featuring:

  • Full multiplication table generation for standard, split, and dual algebras.
  • O(n) holographic table-free recursive descent multiplication.
  • O(1) fast bitwise closed-form multiplication.
  • Integer, graded, and LaTeX notation formatting.
  • CSV export for tables (matrix and long formats).
  • A simple facade API for everyday use, and direct low-level classes for advanced physics/math engines.

📄 Publications & Preprints

This library serves as the formal verification substrate and computational engine for the following mathematical preprints:

1. The Sign Structure of Cayley–Dickson and Split Algebras By Blocks Proves the OPMT (Ordered-Pair Multiplication Table) sign laws, block decomposition, and the O(1) closed-form sign evaluator implemented in the fast engine of this library.


Supported algebras

Kind Description
standard Ordinary Cayley–Dickson algebras: real, complex, quaternions, octonions, sedenions, ...
split Split Cayley–Dickson algebras: standard parent plus one split doubling at the top
dual Dual extension of a standard algebra, with ε² = 0
dual_split Dual extension of a split algebra, with ε² = 0

Installation

Clone the repository:

git clone https://github.com/maher1719/hypercomplex-engine.git
cd hypercomplex-engine

Install in editable mode:

pip install -e .

Run the tests:

pytest -v

Basic Use

The simplest way to use the library is through the top-level facade API.

from hypercomplex import (
    build_table,
    multiply,
    format_element,
    print_table,
    export_csv,
)

Build a table

table = build_table("standard", 3)

This builds the octonion multiplication table.

Dimensions:

n = 0 -> real numbers,       dimension 1
n = 1 -> complex numbers,    dimension 2
n = 2 -> quaternions,        dimension 4
n = 3 -> octonions,          dimension 8
n = 4 -> sedenions,          dimension 16

Print a table

print_table(table, title="Octonions", mode="integer")

Example output style:

      e0  e1  e2  e3  e4  e5  e6  e7
e0 | +e0 +e1 +e2 +e3 +e4 +e5 +e6 +e7
e1 | +e1 -e0 +e3 -e2 +e5 -e4 -e7 +e6
...

You can also use graded notation:

print_table(table, title="Octonions", mode="graded")

Example:

       1  o1  o2  o3  o4  o5  o6  o7
1   | +1 +o1 +o2 +o3 +o4 +o5 +o6 +o7
o1  | +o1 -1 ...
...

Export a table to CSV

Matrix-style CSV:

export_csv(
    "octonions_graded.csv",
    table,
    mode="graded",
    csv_mode="matrix",
)

Long-format CSV for data analysis:

export_csv(
    "octonions_long.csv",
    table,
    mode="integer",
    csv_mode="long",
)

The long format produces rows like:

i,j,sign,index
0,0,1,0
0,1,1,1
1,0,1,1
1,1,-1,0
...

Multiply two basis elements

result = multiply("standard", (1, 1), (1, 2))

print(result)
# (1, 3)

This means:

e1 * e2 = +e3

Format the result:

print(format_element(result, mode="integer"))
# +e3

print(format_element(result, mode="graded"))
# +o12

print(format_element(result, mode="latex"))
# +e_{12}

Note:

integer mode uses the basis index:
    e3

graded mode uses the generator decomposition:
    index 3 = binary 011 = generators 1 and 2 = o12

Split multiplication

result = multiply("split", (1, 1), (1, 1), dim=1)

print(result)
# (1, 0)

In split-complex numbers:

e1² = +e0

Dual multiplication

# eps*e0 represented as local tuple: (sign, local_index, eps_flag)
eps_e0 = (1, 0, 1)

result = multiply("dual", (1, 0), eps_e0, dim=1)

print(result)
# (1, 0, 1)

print(format_element(result, mode="integer"))
# +eps

Nilpotency:

result = multiply("dual", eps_e0, eps_e0, dim=1)

print(result)
# (0, 0, 0)

This means:

ε² = 0

Intermediate Use

The facade API is enough for most users.

For more control, you can choose the computation engine and work directly with tables or multipliers.


Engines

The multiply function supports two engines:

multiply(kind, a, b, dim=None, engine="fast")
Engine Complexity Description
"fast" O(1) Bitwise closed-form sign evaluator
"holographic" O(n) Recursive block descent

Example:

from hypercomplex import multiply

a = (1, 3)
b = (1, 5)

fast_result = multiply("standard", a, b, engine="fast")
holo_result = multiply("standard", a, b, engine="holographic")

assert fast_result == holo_result

Algebra kinds

multiply("standard", a, b)
multiply("split", a, b, dim=3)
multiply("dual", a, b, dim=3)
multiply("dual_split", a, b, dim=3)

For standard, dim is not needed.

For split, dim is optional and can often be inferred from the indices.

For dual and dual_split, dim is required.


Table builders directly

from hypercomplex import (
    StandardTableBuilder,
    SplitTableBuilder,
    DualTableBuilder,
)

standard_builder = StandardTableBuilder()
split_builder = SplitTableBuilder()
dual_builder = DualTableBuilder()

signs, indices = standard_builder.build(3)
signs, indices = split_builder.build(3)
signs, indices, eps = dual_builder.build(2, split=False)

Return conventions:

standard:
    signs, indices

split:
    signs, indices

dual:
    signs, indices, eps

For dual tables:

  • signs[i, j] is the sign.
  • indices[i, j] is the local base index.
  • eps[i, j] is the epsilon flag.

Multipliers directly

from hypercomplex import (
    StandardHolographic,
    SplitHolographic,
    DualHolographic,
)

holo = StandardHolographic()
result = holo.multiply((1, 1), (1, 2))

print(result)
# (1, 3)

Split:

split_holo = SplitHolographic()
result = split_holo.multiply((1, 2), (1, 2), dim=2)

print(result)
# (1, 0)

Dual:

dual_holo = DualHolographic(split=False)

result = dual_holo.multiply((1, 0), (1, 2), dim=1)

print(result)
# (1, 0, 1)

Fast O(1) multipliers directly

from hypercomplex import (
    FastStandard,
    FastSplit,
    FastDual,
)

fast = FastStandard()

result = fast.multiply((1, 1), (1, 2))

print(result)
# (1, 3)

Split:

fast_split = FastSplit()

result = fast_split.multiply((1, 2), (1, 2), dim=2)

print(result)
# (1, 0)

Dual:

fast_dual = FastDual(split=False)

result = fast_dual.multiply((1, 0), (1, 0, 1), dim=1)

print(result)
# (1, 0, 1)

Formatting modes

Mode Example
"integer" +e5
"graded" +o13
"latex" +o_{13}
"latex_integer" +e_{5}
"latex_graded" +o_{13}

Example:

from hypercomplex import format_element

element = (-1, 5)

print(format_element(element, mode="integer"))
# -e5

print(format_element(element, mode="graded"))
# -o13

print(format_element(element, mode="latex_integer"))
# -e_{5}

print(format_element(element, mode="latex_graded"))
# -o_{13}

Advanced Use

This section is for contributors, benchmarking, physics engines, and symbolic pipelines.


Direct low-level imports

If you prefer explicit imports:

from hypercomplex.core.table_builder import (
    StandardTableBuilder,
    SplitTableBuilder,
    DualTableBuilder,
)

from hypercomplex.core.holographic import (
    StandardHolographic,
    SplitHolographic,
    DualHolographic,
)

from hypercomplex.core.fast import (
    FastStandard,
    FastSplit,
    FastDual,
)

from hypercomplex.printer import (
    CDFormat,
    CDTablePrinter,
)

Cross-validating O(1) against the full table

from hypercomplex import StandardTableBuilder, FastStandard

builder = StandardTableBuilder()
fast = FastStandard()

n = 4
signs, indices = builder.build(n)

dim = 1 << n

for i in range(dim):
    for j in range(dim):
        fast_sign, fast_idx = fast.multiply_indices(i, j)

        assert int(signs[i, j]) == fast_sign
        assert int(indices[i, j]) == fast_idx

This proves that the O(1) evaluator agrees with the O(4^n) table builder.


Cross-validating split O(1) against the split table

from hypercomplex import SplitTableBuilder, FastSplit

builder = SplitTableBuilder()
fast = FastSplit()

n = 4
signs, indices = builder.build(n)

dim = 1 << n

for i in range(dim):
    for j in range(dim):
        fast_sign, fast_idx = fast.multiply_indices(i, j, dim=n)

        assert int(signs[i, j]) == fast_sign
        assert int(indices[i, j]) == fast_idx

Dual local and global indices

For dual multiplication, the total dimension is:

2^(dim + 1)

The epsilon bit is bit dim.

Example for dim=1:

lower half: 0, 1        base elements
upper half: 2, 3        epsilon elements

The dual multipliers accept both:

# global index tuple
(1, 2)

# local tuple with epsilon flag
(1, 0, 1)

Both represent ε·e₀ when dim=1.

The output convention is:

(sign, local_index, eps_flag)

This makes formatting easy:

from hypercomplex import format_element

result = (1, 0, 1)

print(format_element(result, mode="integer"))
# +eps

print(format_element(result, mode="latex"))
# +\epsilon

Using the fast engine in a physics loop

For simulations, avoid building large tables. Use the fast engine directly.

from hypercomplex import FastStandard

fast = FastStandard()

def basis_product(i: int, j: int):
    sign, index = fast.multiply((1, i), (1, j))
    return sign, index

sign, index = basis_product(1, 2)

print(sign, index)
# 1 3

For octonionic or higher-dimensional simulations, this avoids O(4^n) memory.


Table size warning

Full table generation grows as:

entries = 4^n

where n is the dimension exponent.

n Dimension Entries
0 1 1
1 2 4
2 4 16
3 8 64
4 16 256
5 32 1,024
6 64 4,096
8 256 65,536
10 1,024 1,048,576
12 4,096 16,777,216

For large dimensions, prefer:

engine="fast"

or:

engine="holographic"

API Reference

Top-level functions

build_table(kind, n)

Builds a multiplication table.

table = build_table("standard", 3)

Returns:

standard:
    (signs, indices)

split:
    (signs, indices)

dual:
    (signs, indices, eps)

dual_split:
    (signs, indices, eps)

multiply(kind, a, b, dim=None, engine="fast")

Multiplies two basis elements.

result = multiply("standard", (1, 1), (1, 2))

Returns:

standard:
    (sign, index)

split:
    (sign, index)

dual:
    (sign, local_index, eps_flag)

dual_split:
    (sign, local_index, eps_flag)

format_element(element, mode="integer")

Formats a basis element tuple.

format_element((1, 3), mode="integer")
# "+e3"

format_element((1, 3), mode="graded")
# "+o12"

print_table(table, title=None, limit=None, mode="integer")

Prints a table.

table = build_table("standard", 2)
print_table(table, mode="graded")

export_csv(path, table, mode="integer", csv_mode="matrix")

Exports a table to CSV.

table = build_table("standard", 3)

export_csv(
    "octonions.csv",
    table,
    mode="graded",
    csv_mode="matrix",
)

CSV modes:

csv_mode Output
"matrix" Spreadsheet-style grid
"long" One row per product

Algebra kinds

Kind Meaning
"standard" Ordinary Cayley–Dickson
"split" Split Cayley–Dickson
"dual" Dual extension of standard algebra
"dual_split" Dual extension of split algebra

Aliases:

standard: "std", "ordinary", "o"
split:    "s"
dual:     "d", "dual_standard"
dual_split: "split_dual", "ds"

Engines

Engine Aliases Complexity
"fast" "o1", "bitwise", "constant" O(1) Word-RAM
"holographic" "on", "descent" O(n)

Mathematical Background

Basis product rule

For standard and split Cayley–Dickson algebras:

e_i * e_j = sign(i, j) * e_{i XOR j}

The index is always:

i XOR j

The sign is determined by the OPMT block laws.


Standard doubling formula

(a, b)(c, d) = (ac - d* b, da + b c*)

with conjugation:

e0* = e0
ek* = -ek for k > 0

Split doubling formula

(a, b)(c, d) = (ac + d* b, da + b c*)

The only difference from the standard construction is the sign of the d* b term.

This causes Block d signs to invert relative to the standard algebra.


Block decomposition

Each multiplication table splits into four blocks:

[ a  b ]
[ c  d ]

where:

Block a: e_i * e_j
Block b: e_i * (e_j ℓ)
Block c: (e_i ℓ) * e_j
Block d: (e_i ℓ) * (e_j ℓ)

For standard algebras:

Block d interior sign = -σ_a

For split algebras:

Block d interior sign = +σ_a

Dual numbers

Dual algebras adjoin ε such that:

ε² = 0

Multiplication rules:

e_i * e_j       = parent product
e_i * (ε e_j)   = ε (e_i e_j)
(ε e_i) * e_j   = ε (e_i e_j)
(ε e_i) * (ε e_j) = 0

Complexity

Operation Complexity Memory
Full table generation O(4^n) O(4^n)
Holographic multiplication O(n) O(1)
Fast bitwise multiplication O(1) Word-RAM O(1)

For arbitrary-precision integers, the fast evaluator uses O(n) bit operations, where:

n = ceil(log2(max(i, j) + 1))

Testing

Run all tests:

pytest -v

Run specific test files:

pytest tests/test_mega_mother.py -v
pytest tests/test_fast_mode.py -v

The test suite validates:

  • Basis notation conversion.
  • Input validation.
  • Standard table generation.
  • Split table generation.
  • Dual table generation.
  • Holographic O(n) multiplication.
  • Fast O(1) multiplication.
  • Cross-validation between tables and multipliers.
  • Facade API behavior.
  • CSV export.

Repository Structure

hypercomplex-engine/
├── examples/
│   ├── direct_implementation/
│   │   └── full_table_builder_simple.py
│   └── uses/
│       ├── outputs/
│       └── use.ipynb
├── hypercomplex/
│   ├── core/
│   │   ├── basis_element.py
│   │   ├── basis_notation.py
│   │   ├── validation.py
│   │   ├── table_builder/
│   │   │   ├── common.py
│   │   │   ├── standard.py
│   │   │   ├── split.py
│   │   │   └── dual.py
│   │   ├── holographic/
│   │   │   ├── standard.py
│   │   │   ├── split.py
│   │   │   └── dual.py
│   │   └── fast/
│   │       ├── bit_utils.py
│   │       ├── fast_standard.py
│   │       ├── fast_split.py
│   │       └── fast_dual.py
│   ├── printer/
│   │   ├── cd_format.py
│   │   └── cd_table_printer.py
│   ├── facade.py
│   └── __init__.py
├── tests/
│   ├── test_algebra.py
│   ├── test_fast_mode.py
│   ├── test_holographic_vs_table.py
│   └── test_mega_mother.py
├── LICENSE
├── README.md
└── pyproject.toml

Citation

If you use this engine in your research, physics simulations, or geometric deep learning models, please cite the underlying theoretical preprints:

@article{ben abdessalem2026,
author = "maher ben abdessalem",
title = "{A Proven Sign Law for Cayley-Dickson Algebras: Ordinary, Split, dual Constructions and their computational proofs and implementations}",
year = "2026",
month = "9",
url = "https://figshare.com/articles/preprint/A_Proven_Sign_Law_for_Cayley-Dickson_Algebras_Ordinary_and_Split_Constructions/33705022",
doi = "10.6084/m9.figshare.33705022.v5"
}

License

MIT License.

See LICENSE for details.

Copyright (c) 2026 Maher Ben Abdessalem

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