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String Theory Demystified

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274 <strong>String</strong> <strong>Theory</strong> Demystifi ed<br />

i<br />

µ<br />

have induced metrics given by h = g ( x , y ), where i = 12 , µν µν i<br />

for the visible and<br />

hidden branes, respectively. The Randall-Sundrum action is<br />

S dyd x g M 4<br />

= ∫<br />

3 ⎛ ⎞<br />

5<br />

− R− ⎝<br />

⎜ Λ<br />

⎠<br />

⎟ +<br />

2<br />

2<br />

4 () i<br />

() i<br />

∫d<br />

x − h ( Λ + L i matter ) (16.21)<br />

∑<br />

i=<br />

1 i<br />

The index i on the second integral indicates that we integrate over each brane<br />

separately. The additional terms included here are<br />

• M 5 : The Planck mass in fi ve dimensions.<br />

• Λ : The cosmological constant in the bulk.<br />

• Λ and Λ : The cosmological constants on the visible and hidden branes.<br />

1 2<br />

• R: The scalar curvature in fi ve dimensions.<br />

• L i ()<br />

matter:<br />

The lagrangian density for matter fi elds on the visible and hidden<br />

branes. On the visible brane, it is the standard model fi elds but could be<br />

different on the hidden brane.<br />

The dimension y ranges over 0 ≤ y≤π r, where r is a constant and the two<br />

c<br />

c<br />

branes are located at the boundaries. The visible brane is located at y = π r, while<br />

1 c<br />

the hidden brane is located at y = 0.<br />

2<br />

Imposing a requirement that Poincaré invariance is respected, the following<br />

metric is chosen that is a slice of anti-de Sitter space:<br />

The exponential term e ky −2<br />

− ky µ ν<br />

ds = e ηµνdx<br />

dx + dy<br />

2 2 2<br />

(16.22)<br />

is called the warp factor. We will see that the warp<br />

factor connects mass scales in our 3 + 1 dimensional universe to fi ve-dimensional<br />

mass parameters.<br />

It can be shown that the cosmological constants in the bulk and on each of the<br />

branes are given by<br />

3 2<br />

Λ =−6Mk<br />

P<br />

Λ =− Λ<br />

3<br />

=−6Mk<br />

1 2<br />

p<br />

(16.23)<br />

If k < M , this tells us that the space-time curvature of the bulk is small compared<br />

p<br />

to the Planck scale.<br />

The exponential warp factor causes the large gap between the observed Planck<br />

and electroweak scales. Moving to an effective four-dimensional theory, Randall<br />

and Sundrum showed that the Planck mass in four dimensions could be derived<br />

from the fi ve-dimensional Planck mass via<br />

3<br />

πr<br />

2 3 c 2 M5<br />

MP = M5 ∫ dye = 1−e<br />

−πrc<br />

k<br />

( )<br />

− ky −2k<br />

rc<br />

π (16.24)

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