Lectures on String Theory
Lectures on String Theory
Lectures on String Theory
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that of Type IIB supergravity in ten dimensi<strong>on</strong>s. In particular, 35 v are <strong>on</strong>-shell<br />
degrees of freedom of the gravit<strong>on</strong>, two 28 are two anisymmetric tensor fields and<br />
35 s is a rank four antisymmetric self-dual tensor. In additi<strong>on</strong> <strong>on</strong>e has two real scalars.<br />
The fermi<strong>on</strong>ic degrees of freedom are two spin-3/2 gravitinos, 56 c , and two spin-1/2<br />
fermi<strong>on</strong>s. The presence of two gravitinos indicates that the corresp<strong>on</strong>ding theory<br />
has N = 2 supersymmetry. Since the graviti<strong>on</strong>s and the fermi<strong>on</strong>s are of the same<br />
chirality this theory is chiral.<br />
One can make another choice of the GSO projecti<strong>on</strong> by requiring that G = −Ḡ = 1.<br />
This gives the following massless spectrum<br />
]<br />
]<br />
Bos<strong>on</strong>s :<br />
[(1) + (28) + (35) v +<br />
[(8) v + (56) v<br />
]<br />
]<br />
Fermi<strong>on</strong>s :<br />
[(8) c + (56) c +<br />
[(8) s + (56) s .<br />
There are <strong>on</strong>-shell degrees of freedom of the gravit<strong>on</strong> (35 v ), antisymmetric rank three<br />
tensor (56 v ), an antisymmetric rank two tensor (28), <strong>on</strong>e vector 8 v ) and <strong>on</strong>e real<br />
scalar, which is called dilat<strong>on</strong>. The fermi<strong>on</strong>ic degrees of freedom comprise two spin-<br />
3/2 gravitinos and two spin-1/2 fermi<strong>on</strong>s. Graviti<strong>on</strong>s and fermi<strong>on</strong>s are of opposite<br />
chirality. Thus, this theory has N = 2 supersymmetry also but it is n<strong>on</strong>-chiral. This<br />
string theory is called Type IIA, and the corresp<strong>on</strong>ding supergravity is Type IIA<br />
supergravity.