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Gravity and Strings

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684 Index<br />

Wess–Zumino (cont.)<br />

in the string worldsheet action, 432<br />

supersymmetric, 417<br />

for Dp-branes, 435, 443<br />

in the superstring GS action, 416<br />

Wess-Zumino (WZ) term<br />

for p-branes, 507–509<br />

Weyl, 57<br />

axisymmetric vacuum solutions, see solution, Weyl<br />

basis, 162<br />

canonical cordinates, 323<br />

formalism for fermions in curved spacetime, 18, 37, 127, 128,<br />

145, 375<br />

<strong>and</strong> the CSK theory, 131<br />

non-metricity tensor, 431<br />

representation, 396, 617, 624, 625<br />

rescalings, 40, 121, 122, 264, 417, 418<br />

<strong>and</strong> conformal reference frames, 510<br />

<strong>and</strong> tracelessness of the Maxwell energy–momentum<br />

tensor, 219<br />

effect on the curvature, 639<br />

invariance of string action, 410, 433<br />

invariance of the string action, 432<br />

supersymmetric, 414<br />

rescalings <strong>and</strong> massless fields, 123<br />

spinors, 612, 616, 628<br />

equivalent to Majorana in 4d, 151<br />

static axisymmetric electrovacuum solutions, see solution,<br />

Weyl<br />

tensor in 4d, 14, 383, 384, 386<br />

<strong>and</strong> the Einstein–Fokker theory, 56<br />

tensor in higher d, 14<br />

theorem (compactness of Lie groups), 594<br />

Wick rotation, 209, 243, 285<br />

not commuting with electric–magnetic duality, 262<br />

of gamma matrices, 626<br />

of Taub–NUT solution, 271<br />

of the SL(2, R)/SO(2) σ-model<br />

<strong>and</strong> the D-instanton, 540<br />

Wigner’s theorem, 595<br />

Wigner–Inönü contraction, 115, 142, 152, 153, 159, 161,<br />

162, 167<br />

Wilczek, 144<br />

Wilson (G. A.), see solution, Israel–Wilson–Perjés (IWP)<br />

Wilson line, 347<br />

<strong>and</strong> D-branes, 428, 429, 499<br />

mechanism, see Hosotani (or Wilson-line) mechanism<br />

Winicour, see solution, Janis–Newman–Winicour<br />

wire singularities<br />

of Gibbons–Hawking multicenter metrics, see solution, Gibbons<br />

of Taub–NUT solution, see Dirac, string singularities<br />

Witten, 395<br />

condition, 183<br />

effect, 256–258, 261, 362<br />

Hoˇrava–Witten scenario, see Hoˇrava–Witten scenario<br />

Witten–Nester–Israel (WNI) technique, 181, 395, 398<br />

WNI, see Witten–Nester–Israel (WNI) technique<br />

worldsheet parity, 420<br />

Wu–Yang monopole, 254–255<br />

WZ, see Wess–Zumino term<br />

Yang<br />

Wu–Yang monopole, see Wu–Yang monopole<br />

Yang–Mills<br />

Bianchi identity, see Bianchi identities, for Yang–MIlls fields<br />

Cherns–Simons 3-form, see Chern–Simons, 3-form<br />

covariant derivative, 596<br />

equation of motion, 597<br />

field, 274, 391, 438, 470, 471, 478, 596<br />

strength, 273, 597<br />

theories, 127, 134, 137, 139, 595–598<br />

<strong>and</strong> gravity, 140–144, 148<br />

instantons, see solution, BPST instanton<br />

solutions, 391<br />

supersymmetric, 373, 564<br />

Yang–Mills theories, 273<br />

Yau, see Schoen–Yau positive-energy theorem<br />

Zanelli, see solution, BTZ black hole<br />

Zehnbein, 462<br />

Zumino, see Wess–Zumino term<br />

Zwanziger, see Dirac–Schwinger–Zwanziger<br />

Zweibein, 14

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