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Lectures on String Theory

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– 118 –<br />

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.

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