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String Theory Demystified

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146 <strong>String</strong> <strong>Theory</strong> Demystifi ed<br />

R SECTOR ALGEBRA<br />

In the R sector, the commutation and anticommutation relations are<br />

D 3<br />

[ L , L ] = ( m− n) L + m δ (7.50)<br />

m n m+ n m+ n,<br />

0<br />

8<br />

⎛ m ⎞<br />

[ L , F ] = −n<br />

F<br />

⎝<br />

⎜<br />

2 ⎠<br />

m n ⎟ m+ n<br />

The conditions on the physical states are<br />

(7.51)<br />

D 2<br />

{ F , F} = 2L<br />

+ m δ (7.52)<br />

m n m+ n m+ n,<br />

0<br />

2<br />

( L − a ) ψ = 0<br />

(7.53)<br />

0 R<br />

L ψ = n><br />

0 0 (7.54)<br />

n<br />

F ψ = m≥<br />

0 0 (7.55)<br />

Here, a is the normal-ordering constant for the R sector.<br />

R<br />

EXAMPLE 7.6<br />

Deduce that a R = 0.<br />

SOLUTION<br />

We start with the anticommutation relation satisfi ed by the F m :<br />

Notice that if m= n=0,<br />

we obtain<br />

m<br />

D 2<br />

{ F , F} = 2L<br />

+ m δ<br />

m n m+ n m+ n,<br />

2<br />

2<br />

{ F, F} = FF + FF = 2F= 2L<br />

0 0 0 0 0 0 0<br />

2<br />

⇒ L = F<br />

0 0<br />

The F annihilate physical states ψ . Therefore,<br />

m<br />

F ψ =<br />

0<br />

0<br />

0<br />

0

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