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Gravity and Strings

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integrability equation in N = 2, d = 4 theories, 382–383<br />

of N = 1, d = 4 AdS supergravity, 385<br />

of N = 1, d = 4 Poincaré supergravity, 183, 398<br />

of N = 1, d = 6 supergravity, 390<br />

of N = 2, d = 4 Poincaré supergravity, 387<br />

spinors<br />

general form in maximally supersymmetric vacua, 380<br />

T-duality tranformation rules, see Buscher T duality, in type-II<br />

theories, transformations of Killing spinors<br />

vector, 21, 98, 110, 111, 177–180, 183, 270, 288, 330, 370, 375,<br />

378, 391, 504, 608<br />

<strong>and</strong> symmetry of the point-particle action, 307<br />

as bosonic generator of a symmetry superalgebra, 374, 378<br />

as generators of the isometry algebra, 371, 504<br />

commuting <strong>and</strong> compactification on T n , 331<br />

conformal, 21<br />

conformal <strong>and</strong> Lie–Lorentz derivative, 376–377<br />

gauge, 176<br />

null, covariantly constant <strong>and</strong> Brinkmann metrics, 282, 647<br />

of coset manifolds, 606, 607<br />

of maximally symmetric spaces, 605<br />

of Minkowski metric, 67<br />

of Minkowski spacetime, 384<br />

of stationary axially symmetric metrics, 268<br />

of the Minkowski metric, 35, 99, 178<br />

spacelike <strong>and</strong> Kaluza–Klein (KK) compactification, 297–299<br />

timelike <strong>and</strong> definition of mass, 179<br />

timelike <strong>and</strong> Killing horizon, 244<br />

timelike <strong>and</strong> staticity, 188<br />

timelike <strong>and</strong> surface gravity, 198<br />

timelike <strong>and</strong> the Schwarzschild metric, 191<br />

translational, 179<br />

versus Killing spinor, 374, 384<br />

KK6-brane, see Kaluza–Klein (KK) monopole, as string–theory<br />

solution (KK6)<br />

KK7M-brane, see Kaluza–Klein (KK) monopole, as M–theory<br />

solution (KK7M)<br />

KK8A-brane, 526<br />

KK9A-brane, 526<br />

KK9M-brane, 465, 524<br />

<strong>and</strong> the M superalgebra, 557<br />

Klein, 290<br />

Kaluza-Klein theories, see Kaluza–Klein<br />

Klein–Gordon equation, 36, 293, 294<br />

Komar’s formula, 180, 221<br />

compared to Abbott–Deser approach, 180<br />

in higher d, 211<br />

Kosmann, 375<br />

Kraichnan, 59<br />

Kretschmann invariant, 190<br />

Lagrange, see Euler–Lagrange<br />

L<strong>and</strong>au<br />

Ginzburg–L<strong>and</strong>au Lagrangian, see Ginzburg–L<strong>and</strong>au<br />

L<strong>and</strong>au–Lifshitz energy–momentum pseudotensor, 173, 174–176<br />

compared with Abbott–Deser approach, 178, 179<br />

Laplace equation, 272, 280, 294, 551, 648, 649<br />

Legendre transformation, 308, 442<br />

Leibniz rule, 5, 6, 376<br />

level operators, 419<br />

Lichnerowicz, 375<br />

Lie<br />

algebra, 5, 43, 591, 592, 595<br />

Abelian, 594<br />

Bianchi classification of 3d real Lie algebras, 602<br />

complexified, 593<br />

de Sitter (anti-), see de Sitter (anti-), algebra<br />

derived subalgebra, 594<br />

Heisenberg, see Heisenberg algebras<br />

invariant subalgebra, 594, 605<br />

nilpotent, 284, 594, 594<br />

of isometry group, 183<br />

Index 677<br />

of GL(d),15<br />

of SO(1, 2), 602<br />

of SO(3), 270<br />

of SO(4) (anti-)self-dual generators, 275<br />

of SO(n+, n−), 600<br />

of SO(n+, n−) (spinorial representation), 601<br />

of SU(2) (SO(3)), 602<br />

of isometries, 371, 379<br />

of the conformal group SO(2, d − 1),40<br />

of the Lorentz group SO(1, d − 1),40<br />

of the Lorentz group SO(1, d − 1) (spinorial representation),<br />

611, 612<br />

of the PoincaréISO(1, d − 1),35<br />

of the PoincaréISO(1, d − 1), 143<br />

of the Poincaré group ISO(1, d − 1), 36, 40, 384<br />

reductive decomposition, 605<br />

semidirect sum, 605<br />

semisimple, 594, 594<br />

simple, 594<br />

solvable, 284, 594, 594<br />

symmetric decomposition, 605<br />

bracket, 5, 80, 592<br />

<strong>and</strong> commutators of matrices, 592<br />

brackets<br />

<strong>and</strong> Ricci rotation coefficients, 15<br />

covariant derivative, 608<br />

derivative, 5,6,8,13, 297, 371, 374, 379, 608<br />

H-covariant, 608<br />

<strong>and</strong> extrinsic curvature, 25<br />

<strong>and</strong> Killing vectors, 20<br />

covariant, 369, 375, 375–378, 379<br />

properties, 5<br />

spinorial, see Lie, Lie–Lorentz derivative<br />

group, 591<br />

ISO(n+, n−), 599<br />

SO(n+, n−), 598<br />

SO(n+, n−),vector representation, 599<br />

SU(2), 603<br />

affine group IGL(d, R),17<br />

<strong>and</strong> N = 1, 2, d = 6 vacua, 390<br />

compact, 593<br />

compact (Weyl theorem), 594<br />

conformal SO(2, d − 1),40<br />

de Sitter (anti-), see de Sitter (anti-), group<br />

invariant subgroup, 594<br />

Lorentz SO(1, d − 1), 17, 32, 142<br />

of isometries, 370<br />

Poincaré ISO(1, d − 1), 17, 26, 32, 46, 48, 49, 52, 96, 108,<br />

114, 127, 132, 134, 137, 140–142, 150<br />

Riemannian geometry, 602–604<br />

semisimple, 594<br />

simple, 594<br />

translation, 145<br />

Lie–Lorentz derivative, 375, 375–377, 384, 608<br />

<strong>and</strong> H-covariant Lie derivative, 381<br />

Lie-Maxwell derivative, 375, 377–378, 608<br />

superalgebra<br />

N = 1, d = 4 Poincaré, 151<br />

supergroup<br />

de Sitter (anti-), see de Sitter (anti-), supergroup<br />

Poincaré, 150<br />

Lie–Lorentz derivative, see Lie, Lie–Lorentz derivative<br />

Lie–Maxwell derivative, see Lie, Lie–Maxwell derivative<br />

Lifshitz, see L<strong>and</strong>au–Lifshitz energy–momentum pseudotensor<br />

Lindquist, see coordinates, Boyer–Lindquist<br />

loop quantization, 138<br />

Lopuszanski, see Haag–Lopuszański–Sohnius theorem<br />

Lorentz<br />

group, see Lie, group, Lorentz<br />

Hilbert–Lorentz gauge, see Hilbert–Lorentz gauge<br />

Lie–Lorentz derivative, see Lie, Lie–Lorentz derivative<br />

Lovelock tensor, 101

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