Trigintaduonion: Difference between revisions
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with real coefficients {{mvar|x<sub>i</sub>}}. |
with real coefficients {{mvar|x<sub>i</sub>}}. |
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The trigintaduonions can be obtained by applying the [[Cayley–Dickson construction]] to the [[sedenion]]s, which can be mathematically expressed as <math>\mathbb{T}=\mathcal{CD}(\mathbb{S},1)</math>.<ref name="Ensembles">{{cite web|url=https://mathsci.kaist.ac.kr/~tambour/fichiers/publications/Ensembles_de_nombres.pdf|date=6 September 2011|title=Ensembles de nombre|publisher=Forum Futura-Science|access-date=11 October 2024|language=fr}}</ref> Applying the Cayley–Dickson construction to the |
The trigintaduonions can be obtained by applying the [[Cayley–Dickson construction]] to the [[sedenion]]s, which can be mathematically expressed as <math>\mathbb{T}=\mathcal{CD}(\mathbb{S},1)</math>.<ref name="Ensembles">{{cite web|url=https://mathsci.kaist.ac.kr/~tambour/fichiers/publications/Ensembles_de_nombres.pdf|date=6 September 2011|title=Ensembles de nombre|publisher=Forum Futura-Science|access-date=11 October 2024|language=fr}}</ref> Applying the Cayley–Dickson construction to the trigintaduonions yields a 64-dimensional algebra called the ''64-ions'', ''64-nions'', ''sexagintaquatronions'', or ''sexagintaquattuornions'', sometimes also known as the ''chingons''.<ref>{{cite web | title=Visualization of the Cayley-Dickson Hypercomplex Numbers Up to the Chingons (64D) | first=Michael | last=Carter | website=MaplePrimes | date=2011-08-19 | url=https://www.mapleprimes.com/posts/124913-Visualization-Of-The-CayleyDickson | access-date=2024-10-08}}</ref><ref>{{cite web | title=Application Center | website=Maplesoft | date=2010-01-18 | url=https://www.maplesoft.com/applications/Preview.aspx?id=35196 | access-date=2024-10-08}}</ref><ref name=DSP>{{cite journal | last1=Valkova-Jarvis | first1=Zlatka | last2=Poulkov | first2=Vladimir | last3=Stoynov | first3=Viktor | last4=Mihaylova | first4=Dimitriya | last5=Iliev | first5=Georgi | title=A Method for the Design of Bicomplex Orthogonal DSP Algorithms for Applications in Intelligent Radio Access Networks | journal=Symmetry | publisher=MDPI AG | volume=14 | issue=3 | date=2022-03-18 | issn=2073-8994 | doi=10.3390/sym14030613 | doi-access=free | page=613| bibcode=2022Symm...14..613V }}</ref> |
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As a result, the trigintaduonions can also be defined as the following.<ref name="Ensembles" /> |
As a result, the trigintaduonions can also be defined as the following.<ref name="Ensembles" /> |
Revision as of 22:42, 1 November 2024
Trigintaduonions | |
---|---|
Symbol | |
Type | Hypercomplex algebra |
Units | e0, ..., e31 |
Multiplicative identity | e0 |
Main properties | |
Common systems | |
Less common systems |
In abstract algebra, the trigintaduonions, also known as the 32-ions, 32-nions, 25-nions, or sometimes pathions (),[1][2] form a 32-dimensional noncommutative and nonassociative algebra over the real numbers,[3][4] usually represented by the capital letter T, boldface T or blackboard bold .[2]
Names
The word trigintaduonion is derived from Latin triginta 'thirty' + duo 'two' + the suffix -nion, which is used for hypercomplex number systems.
Although trigintaduonion is typically the more widely used term, Robert P. C. de Marrais instead uses the term pathion in reference to the 32 paths of wisdom from the Kabbalistic (Jewish mystical) text Sefer Yetzirah, since pathion is shorter and easier to remember and pronounce. It is represented by blackboard bold .[1] Other alternative names include 32-ion, 32-nion, 25-ion, and 25-nion.
Definition
Every trigintaduonion is a linear combination of the unit trigintaduonions , , , , ..., , which form a basis of the vector space of trigintaduonions. Every trigintaduonion can be represented in the form
with real coefficients xi.
The trigintaduonions can be obtained by applying the Cayley–Dickson construction to the sedenions, which can be mathematically expressed as .[5] Applying the Cayley–Dickson construction to the trigintaduonions yields a 64-dimensional algebra called the 64-ions, 64-nions, sexagintaquatronions, or sexagintaquattuornions, sometimes also known as the chingons.[6][7][8]
As a result, the trigintaduonions can also be defined as the following.[5]
An algebra of dimension 4 over the octonions :
- where and
An algebra of dimension 8 over quaternions :
- where and
An algebra of dimension 16 over the complex numbers :
- where and
An algebra of dimension 32 over the real numbers :
- where and
are all subsets of . This relation can be expressed as:
Multiplication
Properties
Like octonions and sedenions, multiplication of trigintaduonions is neither commutative nor associative. However, being products of a Cayley–Dickson construction, trigintaduonions have the property of power associativity, which can be stated as that, for any element x of , the power is well defined. They are also flexible, and multiplication is distributive over addition. [9] As with the sedenions, the trigintaduonions contain zero divisors and are thus not a division algebra.
Geometric representations
Whereas octonion unit multiplication patterns can be geometrically represented by PG(2,2) (also known as the Fano plane) and sedenion unit multiplication by PG(3,2), trigintaduonion unit multiplication can be geometrically represented by PG(4,2). This can be also extended to PG(5,2) for the 64-nions, as explained in the abstract of Saniga, Holweck & Pracna (2015):
Given a -dimensional Cayley–Dickson algebra, where , we first observe that the multiplication table of its imaginary units , is encoded in the properties of the projective space if these imaginary units are regarded as points and distinguished triads of them and , as lines. This projective space is seen to feature two distinct kinds of lines according as or .[10]
Furthermore, Saniga, Holweck & Pracna (2015) state that:
The corresponding point-line incidence structure is found to be a specific binomial configuration ; in particular, (octonions) is isomorphic to the Pasch (62,43)-configuration, (sedenions) is the famous Desargues (103)-configuration, (32-nions) coincides with the Cayley–Salmon (154,203)-configuration found in the well-known Pascal mystic hexagram and (64-nions) is identical with a particular (215,353)-configuration that can be viewed as four triangles in perspective from a line where the points of perspectivity of six pairs of them form a Pasch configuration.[10]
The configuration of -nions can thus be generalized as:[10]
Multiplication tables
The multiplication of the unit trigintaduonions is illustrated in the two tables below. Combined, they form a single 32×32 table with 1024 cells.[11][5]
Below is the trigintaduonion multiplication table for . The top half of this table, for , corresponds to the multiplication table for the sedenions. The top left quadrant of the table, for and , corresponds to the multiplication table for the octonions.
Below is the trigintaduonion multiplication table for .
Triples
There are 155 distinguished triples (or triads) of imaginary trigintaduonion units in the trigintaduonion multiplication table, which are listed below. In comparison, the octonions have 7 such triples, the sedenions have 35, while the sexagintaquatronions have 651.[10]
- 45 triples of type {α, α, β}: {3, 13, 14}, {3, 21, 22}, {3, 25, 26}, {5, 11, 14}, {5, 19, 22}, {5, 25, 28}, {6, 11, 13}, {6, 19, 21}, {6, 26, 28}, {7, 9, 14}, {7, 10, 13}, {7, 11, 12}, {7, 17, 22}, {7, 18, 21}, {7, 19, 20}, {7, 25, 30}, {7, 26, 29}, {7, 27, 28}, {9, 19, 26}, {9, 21, 28}, {10, 19, 25}, {10, 22, 28}, {11, 17, 26}, {11, 18, 25}, {11, 19, 24}, {11, 21, 30}, {11, 22, 29}, {11, 23, 28}, {12, 21, 25}, {12, 22, 26}, {13, 17, 28}, {13, 19, 30}, {13, 20, 25}, {13, 21, 24}, {13, 22, 27}, {13, 23, 26}, {14, 18, 28}, {14, 19, 29}, {14, 20, 26}, {14, 21, 27}, {14, 22, 24}, {14, 23, 25}, {15, 19, 28}, {15, 21, 26}, {15, 22, 25}
- 20 triples of type {β, β, β}: {3, 5, 6}, {3, 9, 10}, {3, 17, 18}, {3, 29, 30}, {5, 9, 12}, {5, 17, 20}, {5, 27, 30}, {6, 10, 12}, {6, 18, 20}, {6, 27, 29}, {9, 17, 24}, {9, 23, 30}, {10, 18, 24}, {10, 23, 29}, {12, 20, 24}, {12, 23, 27}, {15, 17, 30}, {15, 18, 29}, {15, 20, 27}, {15, 23, 24}
- 15 triples of type {β, β, β}: {3, 12, 15}, {3, 20, 23}, {3, 24, 27}, {5, 10, 15}, {5, 18, 23}, {5, 24, 29}, {6, 9, 15}, {6, 17, 23}, {6, 24, 30}, {9, 18, 27}, {9, 20, 29}, {10, 17, 27}, {10, 20, 30}, {12, 17, 29}, {12, 18, 30}
- 60 triples of type {α, β, γ}: {1, 6, 7}, {1, 10, 11}, {1, 12, 13}, {1, 14, 15}, {1, 18, 19}, {1, 20, 21}, {1, 22, 23}, {1, 24, 25}, {1, 26, 27}, {1, 28, 29}, {2, 5, 7}, {2, 9, 11}, {2, 12, 14}, {2, 13, 15}, {2, 17, 19}, {2, 20, 22}, {2, 21, 23}, {2, 24, 26}, {2, 25, 27}, {2, 28, 30}, {3, 4, 7}, {3, 8, 11}, {3, 16, 19}, {3, 28, 31}, {4, 9, 13}, {4, 10, 14}, {4, 11, 15}, {4, 17, 21}, {4, 18, 22}, {4, 19, 23}, {4, 24, 28}, {4, 25, 29}, {4, 26, 30}, {5, 8, 13}, {5, 16, 21}, {5, 26, 31}, {6, 8, 14}, {6, 16, 22}, {6, 25, 31}, {7, 8, 15}, {7, 16, 23}, {7, 24, 31}, {8, 17, 25}, {8, 18, 26}, {8, 19, 27}, {8, 20, 28}, {8, 21, 29}, {8, 22, 30}, {9, 16, 25}, {9, 22, 31}, {10, 16, 26}, {10, 21, 31}, {11, 16, 27}, {11, 20, 31}, {12, 16, 28}, {12, 19, 31}, {13, 16, 29}, {13, 18, 31}, {14, 16, 30}, {14, 17, 31}
- 15 triples of type {β, γ, γ}: {1, 2, 3}, {1, 4, 5}, {1, 8, 9}, {1, 16, 17}, {1, 30, 31}, {2, 4, 6}, {2, 8, 10}, {2, 16, 18}, {2, 29, 31}, {4, 8, 12}, {4, 16, 20}, {4, 27, 31}, {8, 16, 24}, {8, 23, 31}, {5, 16, 31}
Computational algorithms
The first computational algorithm for the multiplication of trigintaduonions was developed by Cariow & Cariowa (2014).
Applications
The trigintaduonions have applications in particle physics,[12] quantum physics, and other branches of modern physics.[11] More recently, the trigintaduonions and other hypercomplex numbers have also been used in neural network research[13] and cryptography.
Further algebras
Robert de Marrais' terms for the algebras immediately following the sedenions are the pathions (i.e. trigintaduonions), chingons, routons, and voudons.[8][14] They are summarized as follows.[1][5]
Name | Dimension | Symbol | Etymology | Other names |
---|---|---|---|---|
pathions | 32 = 25 | , [10] | 32 paths of wisdom of Kabbalah, from the Sefer Yetzirah | trigintaduonions (), 32-nions |
chingons | 64 = 26 | , | 64 hexagrams of the I Ching | sexagintaquatronions, 64-nions |
routons | 128 = 27 | , | Massachusetts Route 128, of the "Massachusetts Miracle" | centumduodetrigintanions, 128-nions |
voudons | 256 = 28 | , | 256 deities of the Ifá pantheon of Voodoo or Voudon | ducentiquinquagintasexions,[15] 256-nions |
References
- ^ a b c de Marrais, Robert P. C. (2002). "Flying Higher Than a Box-Kite: Kite-Chain Middens, Sand Mandalas, and Zero-Divisor Patterns in the 2n-ions Beyond the Sedenions". arXiv:math/0207003.
- ^ a b Cawagas, Raoul E.; Carrascal, Alexander S.; Bautista, Lincoln A.; Maria, John P. Sta.; Urrutia, Jackie D.; Nobles, Bernadeth (2009). "The Subalgebra Structure of the Cayley-Dickson Algebra of Dimension 32 (trigintaduonion)". arXiv:0907.2047 [math.RA].
- ^ Saini, Kavita; Raj, Kuldip (2021). "On generalization for Tribonacci Trigintaduonions". Indian Journal of Pure and Applied Mathematics. 52 (2). Springer Science and Business Media LLC: 420–428. doi:10.1007/s13226-021-00067-y. ISSN 0019-5588.
- ^ "Trigintaduonion". University of Waterloo. Retrieved 2024-10-08.
- ^ a b c d "Ensembles de nombre" (PDF) (in French). Forum Futura-Science. 6 September 2011. Retrieved 11 October 2024.
- ^ Carter, Michael (2011-08-19). "Visualization of the Cayley-Dickson Hypercomplex Numbers Up to the Chingons (64D)". MaplePrimes. Retrieved 2024-10-08.
- ^ "Application Center". Maplesoft. 2010-01-18. Retrieved 2024-10-08.
- ^ a b Valkova-Jarvis, Zlatka; Poulkov, Vladimir; Stoynov, Viktor; Mihaylova, Dimitriya; Iliev, Georgi (2022-03-18). "A Method for the Design of Bicomplex Orthogonal DSP Algorithms for Applications in Intelligent Radio Access Networks". Symmetry. 14 (3). MDPI AG: 613. Bibcode:2022Symm...14..613V. doi:10.3390/sym14030613. ISSN 2073-8994.
- ^ "Trigintaduonions". ArXiV. Retrieved 2024-10-28.
- ^ a b c d e Saniga, Holweck & Pracna (2015).
- ^ a b Weng, Zi-Hua (2024-07-23). "Gauge fields and four interactions in the trigintaduonion spaces". Mathematical Methods in the Applied Sciences. Wiley. doi:10.1002/mma.10345. ISSN 0170-4214.
- ^ Weng, Zihua (2007-04-02). "Compounding Fields and Their Quantum Equations in the Trigintaduonion Space". arXiv:0704.0136 [physics.gen-ph].
- ^ Baluni, Sapna; Yadav, Vijay K.; Das, Subir (2024). "Lagrange stability criteria for hypercomplex neural networks with time varying delays". Communications in Nonlinear Science and Numerical Simulation. 131. Elsevier BV: 107765. Bibcode:2024CNSNS.13107765B. doi:10.1016/j.cnsns.2023.107765. ISSN 1007-5704.
- ^ de Marrais, Robert P. C. (2006). "Presto! Digitization, Part I: From NKS Number Theory to "XORbitant" Semantics, by way of Cayley-Dickson Process and Zero-Divisor-based "Representations"". arXiv:math/0603281.
- ^ Cariow, Aleksandr (2015). "An unified approach for developing rationalized algorithms for hypercomplex number multiplication". Przegląd Elektrotechniczny. 1 (2). Wydawnictwo SIGMA-NOT: 38–41. doi:10.15199/48.2015.02.09. ISSN 0033-2097.
- Cariow, A.; Cariowa, G. (2014). "An algorithm for multiplication of trigintaduonions". Journal of Theoretical and Applied Computer Science. 8 (1): 50–75. ISSN 2299-2634. Retrieved 2024-10-10.
- Saniga, Metod; Holweck, Frédéric; Pracna, Petr (2015). "From Cayley-Dickson Algebras to Combinatorial Grassmannians". Mathematics. 3 (4). MDPI AG: 1192–1221. arXiv:1405.6888. doi:10.3390/math3041192. ISSN 2227-7390. This article incorporates text from this source, which is available under the CC BY 4.0 license.