2000
DOI: 10.1103/physrevd.62.125019
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BPS states and automorphisms

Abstract: The purpose of the present paper is twofold. In the first part, we provide an algebraic characterization of several families of ϭ1/2 n nр5 Bogomol'nyi-Prasad-Sommerfield ͑BPS͒ states in M theory, at threshold and non-threshold, by an analysis of the BPS bound derived from the Nϭ1 Dϭ11 super Poincaré algebra. We determine their BPS masses and their supersymmetry projection conditions, explicitly. In the second part, we develop an algebraic formulation to study the way BPS states transform under GL(32,R) transfo… Show more

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Cited by 4 publications
(7 citation statements)
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“…In particular, the third one can be written as a product of the first two ones, that is, Γ 1278 = Γ 1234 Γ 1256 . Under these circumstances, as pointed out in [72] and generalised in [71], preservation of an exotic amount of supersymmetry is allowed. An explicit matrix realisation for these operators…”
Section: Conditions For ν Inmentioning
confidence: 98%
“…In particular, the third one can be written as a product of the first two ones, that is, Γ 1278 = Γ 1234 Γ 1256 . Under these circumstances, as pointed out in [72] and generalised in [71], preservation of an exotic amount of supersymmetry is allowed. An explicit matrix realisation for these operators…”
Section: Conditions For ν Inmentioning
confidence: 98%
“…Despite the fact that exotic BPS states with n k 32 . 1 2 can also be treated algebraically as a kind of superposition of branes and antibranes [12,13], solitonic solutions are known only for BPS states that preserve a fraction n # 1 2 of supersymmetries. In this paper we propose another algebraic scheme aimed to describe the representations of M algebra, with a different choice of primary and composite objects.…”
mentioning
confidence: 99%
“…A point of view based on the study of solitonic solutions of D=11 supergravity [10,11] considers as the most elementary ones the 1 2 -BPS states describing the M2 and M5 branes, the M9 brane and the M-KK6 brane (D=11 Kaluza-Klein monopole), as well as the M-wave (M0-brane). By considering superpositions of these D=11 elementary objects (intersecting branes and branes ending on branes) one can construct k 32 -BPS D=11 supergravity solitons with k ≤ 16 (ν ≤ 1 2 ) [5,12]. Despite that exotic BPS states with ν = k 32 > 1 2 can also be treated algebraically as a kind of superposition of branes and antibranes [13,12], solitonic solutions are known only for BPS states that preserve a fraction ν ≤ 1 2 of supersymmetries.…”
mentioning
confidence: 99%
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“…The argument can be extended to any number of them. This will change the explicit saturating function in (216) (see [395]), but not the conceptual difference between the two cases outlined above. It is important to stress that just as in supergravity solving the gravitino/dilatino equations, i.e.…”
Section: Hamiltonian Formalismmentioning
confidence: 99%