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Related papers: An octonionic formulation of the M-theory algebra

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Following [1] we further apply the octonionic structure to supersymmetric D=11 $M$-theory. We consider the octonionic $2^{n+1} \times 2^{n+1}$ Dirac matrices describing the sequence of Clifford algebras with signatures ($9+n,n$) ($n=0,1,2,…

High Energy Physics - Theory · Physics 2015-12-24 Jerzy Lukierski , Francesco Toppan

The generalized supersymmetries admitting abelian bosonic tensorial central charges are classified in accordance with their division algebra structure (over ${\bf R}$, ${\bf C}$, ${\bf H}$ or ${\bf O}$). It is shown in particular that in…

High Energy Physics - Theory · Physics 2007-05-23 Francesco Toppan

The connection of (split-)division algebras with Clifford algebras and supersymmetry is investigated. At first we introduce the class of superalgebras constructed from any given (split-)division algebra. We further specify which real…

High Energy Physics - Theory · Physics 2007-05-23 Zhanna Kuznetsova , Francesco Toppan

We describe the set of generalized Poincare and conformal superalgebras in D=4,5 and 7 dimensions as two sequences of superalgebraic structures, taking values in the division algebras R, C and H. The generalized conformal superalgebras are…

High Energy Physics - Theory · Physics 2015-06-26 Jerzy Lukierski , Francesco Toppan

It is shown that the $M$-algebra related with the $M$ theory comes in two variants. Besides the standard $M$ algebra based on the real structure, an alternative octonionic formulation can be consistently introduced. This second variant has…

High Energy Physics - Theory · Physics 2011-01-17 Francesco Toppan

We study the Euclidean supersymmetric D=11 M-algebras. We consider two such D=11 superalgebras: the first one is N=(1,1) self-conjugate complex-Hermitean, with 32 complex supercharges and 1024 real bosonic charges, the second is N=(1,0)…

High Energy Physics - Theory · Physics 2009-11-10 Jerzy Lukierski , Francesco Toppan

Using elementary linear algebra, this paper clarifies and proves some concepts about a recently introduced octonion-like associative division algebra over R. This octonion-like algebra is actually the same as the split-biquaternion algebra,…

General Mathematics · Mathematics 2022-12-06 Juhi Khalid , Martin Bouchard

Quaternionic and octonionic realizations of Clifford algebras and spinors are classified and explicitly constructed in terms of recursive formulas. The most general free dynamics in arbitrary signature space-times for both quaternionic and…

High Energy Physics - Theory · Physics 2009-11-10 H. L. Carrion , M. Rojas , F. Toppan

We discuss how to represent the non-associative octonionic structure in terms of the associative matrix algebra using the left and right octonionic operators. As an example we construct explicitly some Lie and Super Lie algebra. Then we…

High Energy Physics - Theory · Physics 2009-10-30 Khaled Abdel-Khalek

We give a unified division algebraic description of (D=3, N=1,2,4,8), (D=4, N=1,2,4), (D=6, N=1,2) and (D=10, N=1) super Yang-Mills theories. A given (D=n+2, N) theory is completely specified by selecting a pair (A_n, A_{nN}) of division…

High Energy Physics - Theory · Physics 2014-09-09 A. Anastasiou , L. Borsten , M. J. Duff , L. J. Hughes , S. Nagy

We construct a new extension of the Poincar\'e superalgebra in eleven dimensions which contains super one-, two- and five-form charges. The latter two are associated with the supermembrane and the superfivebrane of M-theory. Using the…

High Energy Physics - Theory · Physics 2009-10-30 Ergin Sezgin

The classification of the octonionic realizations of the one-dimensional extended supersymmetries is here furnished. These are non-associative realizations which, albeit inequivalent, are put in correspondence with a subclass of the already…

High Energy Physics - Theory · Physics 2009-11-07 H. L. Carrion , M. Rojas , F. Toppan

Introducing products between multivectors of Cl(0,7) and octonions, resulting in an octonion, and leading to the non-associative standard octonionic product in a particular case, we generalize the octonionic X-product, associated with the…

Mathematical Physics · Physics 2012-08-27 Roldao da Rocha , Jayme Vaz,

We study the four-dimensional {\it N}=8 maximal supergravity in the context of Lie superalgebra SU(8/1). All possible successive superalgebraic truncations from four-dimensional {\it N}=8 theory to {\it N}=7, 6, $\cdots$, 1 supergravity…

High Energy Physics - Theory · Physics 2014-11-18 Chang-Ho Kim , Young-Jai Park , Kee Yong Kim , Yongduk Kim

The Maxwell algebra, an enlargement of Poincare algebra by Abelian tensorial generators, can be obtained in arbitrary dimension D by the suitable contraction of O(D-1,1) \oplus O(D-1,2) (Lorentz algebra \oplus AdS algebra). We recall that…

Mathematical Physics · Physics 2012-01-25 Kiyoshi Kamimura , Jerzy Lukierski

We formulate D=11 supergravity over the octonions by rewriting 32-component Majorana spinors as 4-component octonionic spinors. Dimensional reduction to D=4 and D=3 suggests an interpretation of the so-called 'dilaton vectors', which…

High Energy Physics - Theory · Physics 2015-06-12 A. Anastasiou , M. J. Hughes

We apply the techniques of $S^7$-algebras to the construction of N=5-8 superconformal algebras and of S{\bf O}(1,9), a modification of SO(1,9) which commutes with $S^7$-transformations. We discuss the relevance of S{\bf O}(1,9) for…

High Energy Physics - Theory · Physics 2007-05-23 C. R. Preitschopf

Starting from the four normed division algebras - the real numbers, complex numbers, quaternions and octonions - a systematic procedure gives a 3-cocycle on the Poincare Lie superalgebra in dimensions 3, 4, 6 and 10. A related procedure…

High Energy Physics - Theory · Physics 2015-02-23 John C. Baez , John Huerta

We describe a new first-order formulation of D=11 supergravity which shows that that theory can be understood to arise from a certain topological field theory by the imposition of a set of local constraints on the fields, plus a lagrange…

High Energy Physics - Theory · Physics 2016-09-06 Yi Ling , Lee Smolin

Octonionic algebra being nonassociative is difficult to manipulate. We introduce left-right octonionic barred operators which enable us to reproduce the associative GL(8,R) group. Extracting the basis of GL(4,C), we establish an interesting…

High Energy Physics - Theory · Physics 2009-10-30 Stefano De Leo , Khaled Abdel-Khalek
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