Since 12 August, 2008. 

Supersymmetric StringsA consistent quantum field theory of superstrings exists only in 10 spacetime dimensions! Otherwise there are quantum effects which render the theory inconsistent or 'anomalous'. In 10 spacetime dimensions the effects can precisely cancel leaving the theory anomaly free. It may seem to be a problem to have 10 spacetime dimensions instead of the 4 spacetime dimensions that we observe, but we will see that in getting from 10 to 4 we actually find some interesting physics. In terms of weak coupling perturbation theory there appear to be only
five different consistent superstring theories known as Type
I SO(32), Type IIA, Type IIB, SO(32) Heterotic
and E8 x E8 Heterotic.
This is a theory which contains open superstrings. It has one (N=1) supersymmetry in 10 dimensions. Open strings can carry gauge degrees of freedom at their endpoints, and cancellation of anomalies uniquely constrains the gauge group to be SO(32). It contains Dbranes with 1, 5, and 9 spatial dimensions. This is a theory of closed superstrings which has two (N=2) supersymmetries in ten dimensions. The two gravitini (superpartners to the graviton) move in opposite directions on the closed string world sheet and have opposite chiralities under the 10 dimensional Lorentz group, so this is a nonchiral theory. There is no gauge group. It contains Dbranes with 0, 2, 4, 6, and 8 spatial dimensions. This is also a closed superstring theory with N=2 supersymmetry. However in this case the two gravitini have the same chiralities under the 10 dimensional Lorentz group, so this is a chiral theory. Again there is no gauge group, but it contains Dbranes with 1, 1, 3, 5, and 7 spatial dimensions. This is a closed string theory with worldsheet fields moving in one direction on the world sheet which have a supersymmetry and fields moving in the opposite direction which have no supersymmetry. The result is N=1 supersymmetry in 10 dimensions. The nonsupersymmetric fields contribute massless vector bosons to the spectrum which by anomaly cancellation are required to have an SO(32) gauge symmetry. This theory is identical to the SO(32) Heterotic string, except that the gauge group is E8 X E8 which is the only other gauge group allowed by anomaly cancellation. It is worthwhile to note that the E8 x E8 Heterotic string has historically been considered to be the most promising string theory for describing the physics beyond the Standard Model. It was discovered in 1987 by Gross, Harvey, Martinec, and Rohm and for a long time it was thought to be the only string theory relevant for describing our universe. This is because the SU(3) x SU(2) x U(1) gauge group of the standard model can fit quite nicely within one of the E8 gauge groups. The matter under the other E8 would not interact except through gravity, and might provide a answer to the Dark Matter problem in astrophysics. Due to our lack of a full understanding of string theory, answers to questions such as how is supersymmetry broken and why are there only 3 generations of particles in the Standard Model have remained unanswered. Most of these questions are related to the issue of compactification (discussed on the next page). What we have learned is that string theory contains all the essential elements to be a successful unified theory of particle interactions, and it is virtually the only candidate which does so. However, we don't yet know how these elements specifically come together to describe the physics that we currently observe. Contents 