Update references and typo
Signed-off-by: Riccardo Finotello <riccardo.finotello@gmail.com>
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		| @@ -1280,7 +1280,7 @@ The field $\cA^a$ forms a vector representation of the group \SO{D-1-p} and from | ||||
| \end{figure} | ||||
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| It is also possible to add non dynamical degrees of freedom (\dof) to the open string endpoints. | ||||
| They are known as \emph{Chan-Paton factors}~\cite{Paton:1969:GeneralizedVenezianoModel}. | ||||
| They are known as \emph{Chan-Paton factors}~\cite{Chan:1969:GeneralizedVenezianoModel}. | ||||
| They have no dynamics and do not spoil Poincaré or conformal invariance in the action of the string. | ||||
| Each state can then be labelled by $i$ and $j$ running from $1$ to $N$. | ||||
| Matrices $\tensor{\lambda}{^a_{ij}}$ thus form a basis for expanding wave functions and states: | ||||
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