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String Theory and M-Theory

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6.5 World-volume actions for D-branes 237<br />

manner. However, a quicker method is to note that they can be obtained<br />

by dimensional reduction of the gauge-fixed D9-brane action in Eq. (6.127).<br />

Dimensional reduction simply means dropping the dependence of the worldvolume<br />

fields on 9 − p of the coordinates. This works for both even <strong>and</strong> odd<br />

values of p. For example, dimensional reduction of Eq. (6.127) to four dimensions<br />

gives an exactly supersymmetric nonlinear extension of N = 4 super<br />

Maxwell theory. The supersymmetry transformations are complicated, because<br />

the gauge-fixing procedure contributes induced κ transformations to<br />

the original ε transformations of the fields.<br />

Bosonic D-brane actions with background fields<br />

The D-brane actions obtained in the previous section are of interest as they<br />

describe D-branes in flat space. However, one frequently needs a generalization<br />

that describes the D-brane in a more general background in which<br />

the various bosonic massless supergravity fields are allowed to take arbitrary<br />

values. These actions exhibit interesting features, that we shall now address.<br />

The abelian case<br />

The background fields in the NS–NS sector are the space-time metric gµν,<br />

the two-form Bµν <strong>and</strong> the dilaton Φ. These can be pulled back to the world<br />

volume<br />

P [g + B]αβ = (gµν + Bµν)∂αX µ ∂βX ν . (6.128)<br />

Henceforth, for ease of writing, pullbacks are implicit, <strong>and</strong> this is denoted<br />

gαβ + Bαβ. Note that this gαβ is the bosonic restriction of the quantity<br />

that was called Gαβ previously. With this definition, the DBI term in static<br />

gauge takes the form<br />

<br />

SDp = −TDp<br />

d p+1 σe −Φ0<br />

<br />

− det (gαβ + Bαβ + k 2 ∂αΦ i ∂βΦ i + kFαβ).<br />

(6.129)<br />

Since the string coupling constant gs is already included in the tension TDp,<br />

the dilaton field is shifted by a constant so that it has vanishing expectation<br />

value (Φ = log gs + Φ0). This is the significance of the subscript. Note that<br />

invariance under a two-form gauge transformation<br />

δB = dΛ (6.130)<br />

requires a compensating shift of the gauge field A.<br />

The possibility of R–R background fields should also be considered. They<br />

do not contribute to the DBI action, but they play an important role in

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