02.06.2013 Views

String Theory Demystified

String Theory Demystified

String Theory Demystified

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

CHAPTER 13 D-Branes 237<br />

We consider the critical point ϕ * = 0 and fi nd<br />

4<br />

λϕ 0 2 2<br />

V = − λϕ ϕ + <br />

0<br />

2<br />

The mass term, which multiplies the quadratic term in the expansion is<br />

m 2<br />

2<br />

=−λϕ0<br />

This is a negative mass. So the critical point ϕ * = 0 corresponds to a tachyon.<br />

Our description of the fascinating topic of D-branes in this chapter barely scratches<br />

the surface, but it should help prepare you for more detailed and/or more advanced<br />

treatments. We have followed the development by Zweibach in this chapter, so you<br />

can see his book for a more detailed analysis, in particular including his discussion<br />

of intersecting D6-branes and his accessible discussion of string charge and<br />

electromagnetic fi elds on D-branes (see References). Another good book to consult<br />

is the Szabo text listed in the References. For a really detailed (and advanced)<br />

description of D-branes, see Clifford V. Johnson’s “D-Brane Primer” Johnson’s.<br />

Quiz<br />

A 2 2 1. Consider a potential given by V(<br />

φ) = ( φ −1)<br />

. What are the critical<br />

points?<br />

6<br />

A 2 2<br />

2. Consider V(<br />

φ) = ( φ −1)<br />

and expand to second order. Then identify the<br />

6<br />

mass in the case of each critical point found in Prob. 1. Are any of these<br />

related to a tachyon?<br />

3. What are the critical points?<br />

4. Which critical point corresponds to a tachyon?<br />

5. If a string is stretched between two parallel D-branes, the ground state<br />

acquires mass. Why is that?<br />

Summary

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!