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Heterotic string symmetry down to the point where the hadrons and leptons of more conventional theories are recovered. Viewed from a distance, the symmetry-broken Heterotic strings look just like familiar point particles - but without the infinities and anomalies of the particle approach. In order to maintain conformal invariance (i.e., the world sheet should remain unchanged by relabeling), these 6 extra-dimensions have to curl up in a particular way - a more promising one is the Calabi-Yau manifold (see more in "Compactification") as shown in Figure 12, where each point stands for a 3-D space. | |
Figure 12 Calabi-Yau Space |
different vibrational modes correspond to different particles. Calculations show that the massless closed (bosonic) strings can be either scalar (spin 0) particles, or gravitons. The massless open (bosonic) strings can assume the role of scalar particles or vector particles (such as photons or gluons). Since the next level of massive strings have mass in the order of 1019 Gev, all particles in the Standard Model with mass < 10 Tev can be considered as massless. String theory with | |
Figure 13 Superstring Theories [view large image] |
supersymmetry enables the introduction of ferminonic strings (with spin 1/2) to accompany the bosonic ones (in both the closed and open varieties). Not all superstring theories contain open |
are fermionic and bosonic states respectively. The operator Qi is called supersymmetry (SUSY) generator (also known as supercharge), which transforms these states into each other. The SUSY generators number N characterizes the effect of supersymmetry on the standard model or other theories such as the theory of string. The altered theory is then adjusted to remain invariant under the SUSY transformation - resulting in new fields and particles. | |
Figure 14 Superpartners |
For example, N = 1 generates the supermultiplets as shown in Table 02 below : |
Supermultiplet | Particle | h | Helicity | CPT-Conjugate Helicity |
Degeneracy |
---|---|---|---|---|---|
Chiral | Higgs, Squark, Slepton |
1/2 | 0 | 0 | 1 |
Chiral | Quark, Lepton, Higgsino |
1/2 | 1/2 | -1/2 | 1 |
Vector | Gaugino | 1 | 1/2 | -1/2 | 1 |
Vector | Gauge Boson | 1 | 1 | -1 | 1 |
Gravitino | 3/2 | 1 | -1 | 1 | |
Gravitino | 3/2 | 3/2 | -3/2 | 1 | |
Gravity | Gravitino | 2 | 3/2 | -3/2 | 1 |
Gravity | Graviton | 2 | 2 | -2 | 1 |
Supermultiplet | h | Helicity | CPT-Conjugate Helicity |
Degeneracy |
---|---|---|---|---|
Hyper | 1/2 | -1/2 | 1 | |
Hyper | 1/2 | 0 | 2 | |
Hyper | 1/2 | 1/2 | 1 | |
Vector | 1 | 0 | 0 | 1 |
Vector | 1 | 1/2 | -1/2 | 2 |
Vector | 1 | 1 | -1 | 1 |
Supergravity | 2 | 1 | -1 | 1 |
Supergravity | 2 | 3/2 | -3/2 | 2 |
Supergravity | 2 | 2 | -2 | 1 |
conservation of momentum (of the particle). The gauge transformation is more abstract, it is the rotation in an "internal space". The invariance of the Dirac equation under this transformation implies the existence of force (called gauge force) associated with the spin 1/2 particle described by this equation (Figure 15). In the Standard Model, there are three kinds of gauge forces associated with three different kinds of "internal rotation" represented by mathematical object called "group". The U(1) group has only one phase angle corresponding to one boson - the photon for the electromagnetic interaction. The SU(2) group has three phase angles | ||
Figure 15 Gauge Invariance [view large image] |
Figure 16 Gauge Bosons |
corresponding to three bosons - the W, and Z for the weak interaction. The SU(3) group has eight phase angles corresponding to eight bosons - the eight gluons for the strong interaction (Figure 16). |
of manoeuvres we can smoothly and continuously move from one string theory to any other. Thus, all the 5 string theories involve 2-D membranes, which become apparent in the strong coupling limit and show up in the 11th dimension. Thus the five superstring theories are nothing but different solutions of a single theory, called "M-theory". In this revised picture, the various string theories merely provide different windows to this M-theory. It is suggested that the "true home" of the | ||
Figure 18 11th Dimension [view large image] |
Figure 19 World Path Dimensions |
theory may actually be in the 11th dimension, where we find new, exotic objects, such as the branes. |
only one modulus, which is the radius. A one hole torus requires three moduli to specify the size, shape, and twist as shown in Figure 20. But a typical Calabi-Yau has hundreds, and it becomes more troublesome as the moduli can vary from one point to another in the compactified space as if a force (a massless scalar field) is acting on it. Since the mass and charge of particle is determined by the moduli, thus these fundamental constants are not constant | ||
Figure 20 Moduli of a Torus [view large image] |
Figure 21 Vacuum Energy |
anymore contrary to observation in the real world. Fortunately, M theory provides the flux and brane to resolve the problem. |