2014
DOI: 10.1007/s11232-014-0161-2
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Jacobi-type identities in algebras and superalgebras

Abstract: We introduce two remarkable identities written in terms of single commutators and anticommutators for any three elements of arbitrary associative algebra. One is a consequence of other (fundamental identity). From the fundamental identity, we derive a set of four identities (one of which is the Jacobi identity) represented in terms of double commutators and anticommutators. We establish that two of the four identities are independent and show that if the fundamental identity holds for an algebra, then the mult… Show more

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Cited by 3 publications
(8 citation statements)
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“…Perhaps one reason of a purely algebraic nature is the fact that of the four basic identities (B.1) -(B.4), only two ones are independent, namely (B.2) and (B.3). This circumstance and its consequence were analyzed in detail in the paper by Lavrov et al [46]. In particular, the Jacobi identity (B.1) is a consequence of the generalized identity (B.2).…”
Section: Resultsmentioning
confidence: 99%
“…Perhaps one reason of a purely algebraic nature is the fact that of the four basic identities (B.1) -(B.4), only two ones are independent, namely (B.2) and (B.3). This circumstance and its consequence were analyzed in detail in the paper by Lavrov et al [46]. In particular, the Jacobi identity (B.1) is a consequence of the generalized identity (B.2).…”
Section: Resultsmentioning
confidence: 99%
“…The following theorem shows that the torsion tensor (2.6) of product semi-symmetric connection satisfies Jacoby's identity. For Jacoby's identity you can see the article [3].…”
Section: Theorem 21 ([21])mentioning
confidence: 99%
“…The canonical commutation relation [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15] is the fundamental relation between canonical conjugate quantities. For example, a set of equal-time commutation relations are introduced as xi , pj…”
Section: Canonical Commutation Relationmentioning
confidence: 99%
“…The operator corresponding to any mechanical quantity F is expressed as F in quantum mechanics, so there is F → F , namely it's shown as [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15]…”
Section: Groenewold's Theoremmentioning
confidence: 99%
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