Add appendix for branes at angles
Signed-off-by: Riccardo Finotello <riccardo.finotello@gmail.com>
This commit is contained in:
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@@ -182,32 +182,58 @@
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%---- frak letters
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\providecommand{\fA}{\ensuremath{\mathfrak{A}}\xspace}
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%---- groups
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351
sec/app/parameters.tex
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sec/app/parameters.tex
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In this appendix we show the computation of the parameters of the hypergeometric functions and their relation with the rotation parameters.
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\subsection{Consistency Conditions of the Monodromy Matrices}
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In the main text we set
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\begin{equation}
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D~
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\rM_{\vb{\infty}}~
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D^{-1}
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=
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e^{-2\pi i \delta_{\vb{\infty}}}\,
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\cL(\vb{n}_{\vb{\infty}}),
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\end{equation}
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where $\cL(\vb{n}_{\vb{\infty}}) \in \SU{2}$.
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The previous equation implies
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\begin{equation}
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\left( D\, \rM_{\vb{\infty}}\, D^{-1} \right)^\dagger
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=
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\left( D\, \rM_{\vb{\infty}}\, D^{-1} \right)^{-1},
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\end{equation}
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which can be rewritten as
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\begin{equation}
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\widetilde{\rM}_{\vb{\infty}}^{-1}~
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\cC^{\dagger}\, D^{\dagger}\, D\, \cC
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=
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\cC^{\dagger}\, D^{\dagger}\, D\, \cC~
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\widetilde{\rM}_{\vb{\infty}}^{-1}.
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\end{equation}
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As $\widetilde{\rM}_{\vb{\infty}}$ is a generic diagonal matrix, the previous equation implies that the off-diagonal elements of $\cC^{\dagger}\, D^{\dagger}\, D\, \cC$ must vanish.
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We therefore have
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\begin{equation}
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\begin{split}
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\abs{K}^{-2}
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& =
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-\frac{\cC_{21}\, \cC^*_{22}}{\cC_{11}\, \cC^*_{12}}
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\\
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& =
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-\frac{1}{\pi^4}\,
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\abs{\gfun{a} \gfun{b} \gfun{c-a} \gfun{c-b}}^2 \times
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\\
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& \times
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\sin(\pi a)\, \sin^*(\pi (c-a))\, (\sin(\pi b)\, \sin^*(\pi (c-b)))^*.
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\end{split}
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\end{equation}
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When $a,\, b,\, c \in \R$ this ultimately means that
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\begin{equation}
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\sin(\pi a)\, \sin(\pi (c-a))\, \sin(\pi b)\, \sin(\pi (c-b)) < 0.
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\label{eq:constraint_from_K^2}
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\end{equation}
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Since the previous equation is invariant under integer shift of any of its parameters, we can consider just the fractional parts $0 \le \{a\},\, \{b\},\, \{c\} < 1$.
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In order to have \U{2} monodromies finally requires
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\begin{equation}
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0 \le \{b\} < \{c\} < \{a\} < 1
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\qq{or}
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0 \le \{a\} < \{c\} < \{b\} <1.
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\label{eq:K_consistency_condition}
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\end{equation}
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Should we request \U{1,1} monodromies as in moving rotated branes then we get:
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\begin{equation}
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\abs{K}^{-2}
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=
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\frac{\cC_{21}\, \cC^*_{22}}{\cC_{11}\, \cC^*_{12}}.
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\end{equation}
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This would then imply
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\begin{equation}
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0 \le \{c\} < \{a\},\, \{b\} < 1
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\qq{or}
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0 \le \{a\},\, \{b\} < \{c\} < 1.
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\end{equation}
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\subsection{Fixing the Parameters}
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We can finally show in details the computation of the parameters of the basis of hypergeometric functions used in the main text.
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The relation between these and the \SU{2} matrices can be computed requiring that the monodromies induced by the choice of the parameters equal the monodromies produced by the rotations of the D-branes.
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The monodromy in $\omega_{\bt-1} = 0$ is simpler to compute given that we choose $\cL(\vb{n}_{\vb{0}})$ and $\cR(\widetilde{\vb{m}}_{\vb{0}})$ to be diagonal.
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We impose:
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\begin{eqnarray}
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\mqty( \dmat{1, e^{-2\pi i c^{(L)}}} )
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& = &
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e^{-2\pi i \delta_{\vb{0}}^{(L)}}\,
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\mqty( \dmat{e^{2\pi i n_{\vb{0}}}, e^{-2\pi i n_{\vb{0}}}} ),
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\\
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\mqty( \dmat{1, e^{-2\pi i c^{(R)}}} )
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& = &
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e^{-2\pi i \delta_{\vb{0}}^{(R)}}\,
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\mqty( \dmat{e^{-2\pi i m_{\vb{0}}}, e^{2\pi i m_{\vb{0}}}} ),
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\end{eqnarray}
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where $n^3_{\vb{0}} = \norm{\vb{n}_{\vb{0}}} = n_{\vb{0}}$ and $m^3_{\vb{0}} = \norm{\vb{m}_{\vb{0}}} = m_{\vb{0}}$ with $0 \le n_{\vb{0}},\, m_{\vb{0}} < 1$ due to the conventions \eqref{eq:maximal_torus_left} and \eqref{eq:maximal_torus_right}.
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We thus have:
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\begin{equation}
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\begin{split}
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\delta_{\vb{0}}^{(L)}
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& =
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n_{\vb{0}} + k_{\delta^{(L)}_{\vb{0}}},
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\qquad
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k_{\delta^{(L)}_{\vb{0}}} \in \Z,
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\\
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c^{(L)}
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& =
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2 n_{\vb{0}} + k_c,
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\qquad
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k_c \in \Z.
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\end{split}
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\label{eq:cL}
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\end{equation}
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Since the determinant of the right hand side is $e^{-4 \pi i \delta_{\vb{0}}^{(L)}}$, the range of definition of $\delta_{\vb{0}}^{(L)}$ is $\alpha \le \delta_{\vb{0}}^{(L)} \le \alpha + \frac{1}{2}$.
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Given that $0 \le n_{\vb{0}} < \frac{1}{2}$ we simply take $\alpha = 0$ and set $\delta_{\vb{0}}^{(L)} = n_{\vb{0}}$.
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Analogous results hold in the right sector.
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Furthermore from the third equation in \eqref{eq:parameters_equality_zero} and from the first equation in \eqref{eq:cL} we can restrict:
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\begin{equation}
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n_{\vb{0}} + m_{\vb{0}} - A \in \Z.
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\end{equation}
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We then need to find $3$ equations to determine $a^{(L)}$, $b^{(L)}$ and $\delta^{(L)}_{\vb{\infty}}$.
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After that we then fix the remaining factors in $B$ and $\abs{K^{(L)}}$.
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The equations follow from~\eqref{eq:parameters_equality_infty}.
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The first two equations for $a^{(L)}$, $b^{(L)}$ and $\delta^{(L)}_{\vb{\infty}}$ follow by considering the trace of~\eqref{eq:parameters_equality_infty}:
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\begin{equation}
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e^{\pi i ( a^{(L)} + b^{(L)} )} \cos(\pi( a^{(L)} - b^{(L)} ) )
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=
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e^{-2\pi i \delta^{(L)}_{\infty}} \cos(2\pi n_{\vb{\infty}}),
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\end{equation}
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which is satisfied by:
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\begin{equation}
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\begin{split}
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\delta^{(L)}_{\vb{\infty}}
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& =
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-
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\frac{1}{2}(a^{(L)} + b^{(L)})
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+
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\frac{1}{2} k_{\delta^{(L)}_{\vb{\infty}}},
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\qquad
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k_{\delta_{\vb{\infty}}} \in \Z,
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\\
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a^{(L)} - b^{(L)}
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& =
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2\, (-1)^{p^{(L)}}\, n_{\vb{\infty}}
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+
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(-1)^{q^{(L)}}\, k_{\delta^{(L)}_{\vb{\infty}}}
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+
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2\, k'_{a b},
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\qquad
|
||||
k'_{ab} \in \Z,
|
||||
\end{split}
|
||||
\end{equation}
|
||||
where $p^{(L)},\, q^{(L)} \in \left\lbrace 0, 1 \right\rbrace$.
|
||||
Notice that changing the value of $p^{(L)}$ corresponds to swapping $a$ and $b$: since the hypergeometric function is symmetric in those parameters we can fix $p^{(L)}=0$.
|
||||
Redefining $k'$ we can always set $q^{(L)}=0$.
|
||||
We therefore have:
|
||||
\begin{equation}
|
||||
a^{(L)} - b^{(L)}
|
||||
=
|
||||
2\, n_{\vb{\infty}}
|
||||
+
|
||||
k_{\delta^{(L)}_{\vb{\infty}}}
|
||||
+
|
||||
2 k_{ab},
|
||||
\qquad
|
||||
k_{a b}\in \Z.
|
||||
\label{eq:aL-bL}
|
||||
\end{equation}
|
||||
The allowed values for $k_{\delta^{(L)}_{\vb{\infty}}}$ follow a construction similar to the monodromy around $\omega_{\bt-1} = 0$.
|
||||
The main difference is given by the fact that $\frac{1}{2}(a^{(L)} + b^{(L)})$ may a priori take values in an interval of width $1$.
|
||||
As in the previous case we have $\alpha \le \delta_{\vb{\infty}}^{(L)} \le \alpha + \frac{1}{2}$ with $\alpha$ technically arbitrary.
|
||||
We cannot thus choose a vanishing $k_{\delta^{(L)}_{\vb{\infty}}}$ but we have to consider $k_{\delta^{(L)}_{\infty}} = 0,\, 1$.
|
||||
|
||||
We find a third relation by considering the entry
|
||||
\begin{equation}
|
||||
\Im\left(
|
||||
e^{+2\pi i \delta_{\vb{\infty}}^{(L)}}\,
|
||||
D^{(L)}\,
|
||||
\rM_{\vb{\infty}}^{(L)}\,
|
||||
\left( D^{(L)} \right)^{-1}
|
||||
\right)_{11}
|
||||
=
|
||||
\Im\left(
|
||||
\cL(n_{\vb{\infty}})
|
||||
\right)_{11}.
|
||||
\end{equation}
|
||||
Using
|
||||
\begin{equation}
|
||||
\det \cC
|
||||
=
|
||||
\frac{\sin(\pi c^{(L)})}{\sin(\pi(a^{(L)}-b^{(L)}))},
|
||||
\end{equation}
|
||||
and the second equation in~\eqref{eq:cL} and~\eqref{eq:aL-bL} leads to:
|
||||
\begin{equation}
|
||||
\cos(\pi( a^{(L)} + b^{(L)} - c^{(L)} ))
|
||||
=
|
||||
(-1)^{k_c+k_{\delta^{(L)}_{\vb{\infty}}} }\, \cos(2\pi \cA^{(L)}),
|
||||
\end{equation}
|
||||
where
|
||||
\begin{equation}
|
||||
\cos(2\pi \cA^{(L)})
|
||||
=
|
||||
\cos(2\pi n_{\vb{0}})\,
|
||||
\cos(2\pi n_{\vb{\infty}})
|
||||
-
|
||||
\sin(2\pi n_{\vb{0}})\,
|
||||
\sin(2\pi n_{\vb{\infty}})\,
|
||||
\frac{n_{\vb{\infty}}^3}{n_{\vb{\infty}}}.
|
||||
\label{eq:cos_n1}
|
||||
\end{equation}
|
||||
This expression is connected with rotation parameter in the third interaction point $\omega_{\bt+1} = 1$.
|
||||
In fact $\cos(2\pi \cA^{(L)}) = \cos(2\pi {n}_{\vb{1}})$.
|
||||
We then write
|
||||
\begin{equation}
|
||||
a^{(L)} + b^{(L)} - c^{(L)}
|
||||
=
|
||||
2\, (-1)^{f^{(L)}}\, n_{\vb{1}}
|
||||
+
|
||||
k_c
|
||||
+
|
||||
k_{\delta^{(L)}_{\vb{\infty}}}
|
||||
+
|
||||
2\, k_{abc},
|
||||
\qquad
|
||||
k_{abc}\in \Z,
|
||||
\end{equation}
|
||||
with $f^{(L)} \in \left\lbrace 0, 1 \right\rbrace$.
|
||||
The request
|
||||
\begin{equation}
|
||||
A
|
||||
+
|
||||
B
|
||||
-
|
||||
n_{\vb{0}}
|
||||
-
|
||||
m_{\vb{0}}
|
||||
-
|
||||
(-1)^{f^{(L)}}\, n_{\vb{1}}
|
||||
-
|
||||
(-1)^{f^{(R)}}\, m_{\vb{1}}
|
||||
\in \Z
|
||||
\end{equation}
|
||||
finally fixes the $B$ parameter in the third equation of~\eqref{eq:parameters_equality_infty}.
|
||||
|
||||
So far we can summarise the results in
|
||||
\begin{eqnarray}
|
||||
a
|
||||
=
|
||||
n_{\vb{0}} + (-1)^{f^{(L)}} n_{\vb{1}} + n_{\vb{\infty}} + m_a,
|
||||
& \qquad &
|
||||
m_a \in \Z,
|
||||
\\
|
||||
b
|
||||
=
|
||||
n_{\vb{0}} + (-1)^{f^{(L)}} n_{\vb{1}} - n_{\vb{\infty}} + m_b,
|
||||
& \qquad &
|
||||
m_b \in \Z,
|
||||
\\
|
||||
c
|
||||
=
|
||||
2\, n_{\vb{0}} + m_c,
|
||||
& \qquad &
|
||||
m_c \in \Z,
|
||||
\\
|
||||
\delta_{\vb{0}}^{(L)}
|
||||
=
|
||||
n_{\vb{0}},
|
||||
\\
|
||||
\delta_{\vb{\infty}}^{(L)}
|
||||
=
|
||||
- n_{\vb{0}} - (-1)^{f^{(L)}} n_{\vb{1}} + m_c + 2\, m_\delta,
|
||||
& \qquad &
|
||||
m_{\delta} \in \Z,
|
||||
\\
|
||||
A
|
||||
=
|
||||
n_{\vb{0}} + m_{\vb{0}} + m_A,
|
||||
& \qquad &
|
||||
m_A \in \Z,
|
||||
\\
|
||||
B
|
||||
=
|
||||
(-1)^{f^{(L)}}\, n_{\vb{1}} + (-1)^{f^{(R)}}\, m_{\vb{1}} + m_B,
|
||||
& \qquad &
|
||||
m_B \in \Z.
|
||||
\end{eqnarray}
|
||||
|
||||
$K^{(L)}$ is finally determined from
|
||||
\begin{equation}
|
||||
\left( D^{(L)}\, \rM_{\vb{\infty}}\, \left( D^{(L)} \right)^{-1} \right)_{21}
|
||||
=
|
||||
e^{-2\pi i \delta_{\vb{\infty}}^{(L)}}\,
|
||||
\left( \cL(n_{\vb{\infty}}) \right)_{21},
|
||||
\label{eq:fixing_K_21}
|
||||
\end{equation}
|
||||
and get:
|
||||
\begin{equation}
|
||||
K^{(L)}
|
||||
=
|
||||
-\frac{(-1)^{m_a + m_b + m_c}}{2 \pi^2}\,
|
||||
\cG( a^{(L)},\, b^{(L)},\, c^{(L)} )\,
|
||||
\sin(2 \pi n_{\vb{0}})
|
||||
\sin(2 \pi n_{\vb{\infty}})
|
||||
\frac{n^1_{\vb{\infty}} + i\, n^2_{\vb{\infty}}}{n_{\vb{\infty}}},
|
||||
\label{eq:app_B_K21}
|
||||
\end{equation}
|
||||
where $\cG( a,\, b,\, c ) = \gfun{1-a}\, \gfun{1-b}\, \gfun{a+1-c}\, \gfun{b+1-c}$.
|
||||
|
||||
|
||||
\subsection{Checking the Consistency of the Solution}
|
||||
|
||||
We check the consistency condition \eqref{eq:K_consistency_condition} using~\eqref{eq:product_in_SU2}.
|
||||
The result is
|
||||
\begin{equation}
|
||||
\begin{split}
|
||||
\left( K^{(L)} \right)^{-1}
|
||||
& =
|
||||
\frac{(-1)^{m_a + m_b + m_c}}{2 \pi^2}\,
|
||||
\cG(1 - a^{(L)},\, 1 - b^{(L)},\, 2 - c^{(L)})\,
|
||||
\\
|
||||
& \times
|
||||
\sin(2 \pi n_{\vb{0}})\,
|
||||
\sin(2 \pi n_{\vb{\infty}})\,
|
||||
\frac{n^1_{\vb{\infty}} -i n^2_{\vb{\infty}}}{n_{\vb{\infty}}},
|
||||
\end{split}
|
||||
\label{eq:app_B_K12}
|
||||
\end{equation}
|
||||
where the function $\cG( a,\, b,\, c )$ was defined at the end of the previous section.
|
||||
Compatibility with~\eqref{eq:app_B_K21} requires
|
||||
\begin{equation}
|
||||
\frac{(n^1_{\vb{\infty}})^2 + (n^2_{\vb{\infty}})^2}{n^2_{\vb{\infty}}}
|
||||
=
|
||||
-4 \frac{\sin(\pi a) \sin(\pi(c-a))\sin(\pi b) \sin(\pi(c-b))}
|
||||
{\sin^2(\pi c) \sin^2(\pi(a-b))}.
|
||||
\label{eq:n12+n22}
|
||||
\end{equation}
|
||||
We can then rewrite~\eqref{eq:cos_n1} as
|
||||
\begin{equation}
|
||||
\frac{(n^3_{\vb{\infty}})^2}{n^2_{\vb{\infty}}}
|
||||
=
|
||||
\frac{(\cos(\pi (a-b)) \cos(\pi c)- \cos(\pi(a+b-c)))^2}
|
||||
{\sin^2(\pi c) \sin^2(\pi(a-b))}.
|
||||
\end{equation}
|
||||
It is then possible to verify that the sum of the left and right hand sides of~\eqref{eq:n12+n22} and the last equation are equal to $1$.
|
||||
The same consistency check can also be performed by computing $K^{(L)}$ from
|
||||
\begin{equation}
|
||||
\left( D^{(L)}\, \rM_{\vb{\infty}}\, \left( D^{(L)} \right)^{-1} \right)_{12}
|
||||
=
|
||||
e^{-2\pi i \delta_{\vb{\infty}}^{(L)}}\,
|
||||
\left( \cL(n_{\vb{\infty}}) \right)_{12},
|
||||
\end{equation}
|
||||
instead of \eqref{eq:fixing_K_21}.
|
||||
|
||||
% vim: ft=tex
|
||||
@@ -23,23 +23,23 @@ We focus on the relative rotations which characterise each D-brane in $\R^4$ wit
|
||||
In total generality, they are non commuting \SO{4} matrices.
|
||||
|
||||
In this paper we study the classical solution of the bosonic string which dominates the behaviour of the correlator of twist fields.
|
||||
Using the path integral approach we can in fact separate the classical contribution from the quantum fluctuations and write the correlators of $N_B$ twist fields $\sigma_{M_{(t)}}( x_{(t)} )$ as:\footnotemark{}
|
||||
Using the path integral approach we can in fact separate the classical contribution from the quantum fluctuations and write the correlators of $N_B$ twist fields $\sigma_{\rM_{(t)}}( x_{(t)} )$ as:\footnotemark{}
|
||||
\footnotetext{%
|
||||
Ultimately $N_B = 3$ in our case.
|
||||
}
|
||||
\begin{equation}
|
||||
\left\langle
|
||||
\finiteprod{t}{1}{N_B}
|
||||
\sigma_{M_{(t)}}(x_{(t)})
|
||||
\sigma_{\rM_{(t)}}(x_{(t)})
|
||||
\right\rangle
|
||||
=
|
||||
\cN
|
||||
\left(
|
||||
\left\lbrace x_{(t)},\, M_{(t)} \right\rbrace_{1 \le t \le N_B}
|
||||
\left\lbrace x_{(t)},\, \rM_{(t)} \right\rbrace_{1 \le t \le N_B}
|
||||
\right)\,
|
||||
e^{-S_E\left( \left\lbrace x_{(t)}, M_{(t)} \right\rbrace_{1 \le t \le N_B} \right)},
|
||||
e^{-S_E\left( \left\lbrace x_{(t)}, \rM_{(t)} \right\rbrace_{1 \le t \le N_B} \right)},
|
||||
\end{equation}
|
||||
where $M_{(t)}$ (for $1 \le t \le N_B$) are the monodromies induced by the twist fields, $N_B$ is the number of D-branes and $x_{(t)}$ are the intersection points on the worldsheet.
|
||||
where $\rM_{(t)}$ (for $1 \le t \le N_B$) are the monodromies induced by the twist fields, $N_B$ is the number of D-branes and $x_{(t)}$ are the intersection points on the worldsheet.
|
||||
Even though quantum corrections are crucial to the complete determination of the normalisation of the correlator, the classical contribution of the Euclidean action represents the leading term of the Yukawa couplings.
|
||||
We focus on its contribution to better address the differences from the usual factorised case and generalise the results to non Abelian rotations of the D-branes.
|
||||
We do not consider the quantum corrections as they cannot be computed with the actual techniques.
|
||||
@@ -115,7 +115,7 @@ The well adapted reference coordinates system is connected to the global $\R^{4}
|
||||
\end{equation}
|
||||
where $R_{(t)}$ represents the rotation of the D-brane $D_{(t)}$ and $g_{(t)} \in \R^4$ its translation with respect to the origin of the global set of coordinates (see \Cref{fig:branes_at_angles} for a two-dimensional example).
|
||||
|
||||
While we could naively consider $R_{(t)} \in \mathrm{SO}(4)$, rotating separately the subset of coordinates parallel and orthogonal to the D-brane does not affect the embedding.
|
||||
While we could naively consider $R_{(t)} \in \SO{4}$, rotating separately the subset of coordinates parallel and orthogonal to the D-brane does not affect the embedding.
|
||||
In fact it just amounts to a trivial redefinition of the initial well adapted coordinates.
|
||||
The rotation $R_{(t)}$ is actually defined in the Grassmannian:
|
||||
\begin{equation}
|
||||
@@ -380,6 +380,7 @@ As a consequence of the geometry of the rotations of the D-branes, a path on the
|
||||
\widetilde{\cU}_{(\bt + t, \bt + 1 + t)}
|
||||
=
|
||||
\1_4.
|
||||
\label{eq:homotopy_rep}
|
||||
\end{equation}
|
||||
The complex plane has therefore branch cuts running between the D-branes at finite as shown in \Cref{fig:finite_cuts}.
|
||||
We thus translated the rotations of the D-branes encoded in the matrices $R_{(t)}$ in terms of $\cU_{(t,\, t+1)}$ and $\widetilde{\cU}_{(t,\, t+1)}$ which are matrix representations of the homotopy group of the complex plane with the described branch cut structure.
|
||||
@@ -443,7 +444,7 @@ In what follows we use the isomorphism
|
||||
\end{equation}
|
||||
to map the problem of finding a $4$-dimensional real solution to the \eom to a quest for a $2 \times 2$ complex matrix.
|
||||
Such matrix is a linear superposition of tensor products of vectors in the fundamental representation of two different \SU{2} groups.
|
||||
These vectors are solutions to second order differential equations with three Fuchsian points, that is the hypergeometric equation.
|
||||
These vectors are solutions to second order differential equations with three Fuchsian points, possibly the hypergeometric equation.
|
||||
The task is then to find the parameters of the hypergeometric functions producing the spinor representation of the monodromies in~\eqref{eq:top_monodromy} and \eqref{eq:bottom_monodromy}.
|
||||
|
||||
|
||||
@@ -544,9 +545,9 @@ It is possible to show that the closed loop $x_t + \eta \pm i\, 0^+ \mapsto x_t
|
||||
|
||||
|
||||
\subsubsection{Special Form of Matrices for D-Branes at Angles}
|
||||
\label{sect:special_SO4}
|
||||
\label{sec:special_SO4}
|
||||
|
||||
The $\SU{2}$ matrices involved in this scenario with D-branes intersecting at angles have a particular form.
|
||||
The \SU{2} matrices involved in this scenario with D-branes intersecting at angles have a particular form.
|
||||
In the left sector (i.e.\ $\SU{2}_L$ matrices) we have:
|
||||
\begin{equation}
|
||||
\cL_{(t,\, t+1)}
|
||||
@@ -575,7 +576,428 @@ The right sector clearly follows the same discussion.
|
||||
|
||||
In fact \cS in~\eqref{eq:reflection_S} can be represented as $U_{L} = U_{R} = i\, \sigma_1$.
|
||||
Then any matrix $U_{L}(\vb{n}_{(t)})$ is of the form $U_{L}(\vb{n}_{(t)}) = i\, U(\vb{r}_{(t)}) \cdot \sigma_1 \cdot U^\dagger(\vb{r}_{(t)})$, for some $\vb{r}_{(t)}$ as follows from~\eqref{eq:Umatrices}.
|
||||
Such matrix has vanishing trace and squares to $-\1_2$ hence the term proportional to two-dimensional unit matrix in the expression of the generic $\mathrm{SU}(2)$ element given in \Cref{sec:isomorphism} vanishes.
|
||||
As a consequence $n_{(t)} = \frac{1}{4}$ such that \eqref{eq:special_UL_brane_t} follows.
|
||||
Such matrix has vanishing trace and squares to $-\1_2$ hence the term proportional to two-dimensional unit matrix in the expression of the generic \SU{2} element given in \Cref{sec:isomorphism} vanishes.
|
||||
As a consequence $n_{(t)} = \frac{1}{4}$ such that~\eqref{eq:special_UL_brane_t} follows.
|
||||
|
||||
% vim ft=tex
|
||||
|
||||
\subsection{The Classical Solution}
|
||||
|
||||
In the previous sections we defined the principal tools to study the non Abelian embedding of the D-branes.
|
||||
In what follows we start the investigation of the relation between the hypergeometric solutions and the monodromies due to the geometry of the D-branes.
|
||||
|
||||
|
||||
\subsubsection{The Choice of Hypergeometric Functions}
|
||||
|
||||
We build the spinorial representation with \SU{2} matrices and solutions of Fuchsian equations with $N_B$ regular singular points.
|
||||
We are specifically interested in a solution with $N_B = 3$.
|
||||
We fix the usual \SL{2}{\R} invariance by mapping the three intersection points $x_{(\bt-1)}$, $x_{(\bt+1)}$ and $x_{(\bt)}$ to $\omega_{\bt-1} = \omega_{x_{(\bt-1)}} = 0$, $\omega_{\bt+1} = \omega_{x_{(\bt+1)}} = 1$ and $\omega_{\bt} = \omega_{x_{(\bt)}} = \infty$ respectively through:
|
||||
\begin{equation}
|
||||
\omega_{u}
|
||||
=
|
||||
\frac{u - x_{(\bt-1)}}{u - x_{(\bt)}}
|
||||
\cdot
|
||||
\frac{x_{(\bt+1)} - x_{(\bt-1)}}{x_{(\bt+1)} - x_{(\bt)}}
|
||||
\label{eq:def_omega}
|
||||
\end{equation}
|
||||
The cut structure for this choice is presented in~\Cref{fig:hypergeometric_cuts}.
|
||||
The map also defines $\arg(\omega_t - \omega_z) \in \left[ 0,\, 2\pi \right)$ for $t = \bt-1,\, \bt+1$.
|
||||
We choose $\bt = 1$ in what follows.
|
||||
|
||||
\begin{figure}[tbp]
|
||||
\centering
|
||||
\def\svgwidth{0.35\linewidth}
|
||||
\import{img/}{threebranes_plane.pdf_tex}
|
||||
\caption{%
|
||||
Fixing the \SL{2}{\R} invariance for $N_B = 3$ and $\bt = 1$ leads to a cut structure with all the cuts defined on the real axis towards $\omega_{\bt} = \infty$.}
|
||||
\label{fig:hypergeometric_cuts}
|
||||
\end{figure}
|
||||
|
||||
The map~\eqref{eq:def_omega} moves the generic Fuchsian singularities to known points on the complex plane.
|
||||
The functions reproducing the necessary monodromies are basis of hypergeometric functions.
|
||||
We define:
|
||||
\begin{equation}
|
||||
\hyp{a}{b}{c}{z}
|
||||
=
|
||||
\zeroinfsum{k}\,
|
||||
\frac{\poch{a}{k}\poch{b}{k}}{\gfun{c+k}}~
|
||||
\frac{z^k}{k!}
|
||||
=
|
||||
\frac{1}{\gfun{c}}~
|
||||
\tensor[_2]{F}{_1}(a,\, b;\, c;\, z),
|
||||
\end{equation}
|
||||
where $\tensor[_2]{F}{_1}(a,\, b;\, c;\, z)$ is the Gauss hypergeometric function and $\gfun{s}$ is the Euler Gamma function.
|
||||
The function \hyp{a}{b}{c}{z} is well defined for any value of its parameters.\footnotemark{}
|
||||
\footnotetext{%
|
||||
It is not necessary to require $c \in \Z_+$ as in the definition of the Gauss hypergeometric function.
|
||||
}
|
||||
We define a vector of independent hypergeometric functions:
|
||||
\begin{equation}
|
||||
B_{\vb{0}}(z)
|
||||
=
|
||||
\mqty(
|
||||
\hyp{a}{b}{c}{z}
|
||||
\\
|
||||
(-z)^{1-c}~\hyp{a+1-c}{b+1-c}{2-c}{z}
|
||||
)
|
||||
\label{eq:basis_0}
|
||||
\end{equation}
|
||||
as basis of functions around $z = 0$ with a branch cut on the interval $\left[ 0, +\infty \right)$.
|
||||
The choice of the branch cuts follows from the cut on $\left[ 1, +\infty \right)$ coming from $\hyp{a}{b}{c}{z}$ which has a singularity at $z = 1$ and the cut on $\left[ 0, +\infty \right)$ from $(-z)^{1-c}$.
|
||||
|
||||
As argued in~\eqref{eq:homotopy_rep}, the homotopy group of the complex plane with the branch cut structure of~\Cref{fig:hypergeometric_cuts} is such that a closed loop around all the singularities is homotopically trivial.
|
||||
The corresponding product of the monodromy matrices~\eqref{eq:homotopy_rep} is the unit matrix.
|
||||
Let for instance $\cM_{\omega_z}^{\pm}$ be the monodromy matrix which represents a closed loop around $\omega_z$ (the $+$ sign represents a path starting in $\ccH$, while $-$ is a path with base point in $\overline{\ccH}$).
|
||||
The triviality property is realised through:
|
||||
\begin{equation}
|
||||
\cM_{\vb{0}}^+\,
|
||||
\cM_{\vb{1}}^+\,
|
||||
\cM_{\vb{\infty}}^+
|
||||
=
|
||||
\cM_{\vb{\infty}}^-\,
|
||||
\cM_{\vb{1}}^-\,
|
||||
\cM_{\vb{0}}^-
|
||||
=
|
||||
\1_2
|
||||
\label{eq:monodromy_relations}
|
||||
\end{equation}
|
||||
The monodromy matrix $\omega_{\bt+1} = 1$ can thus be recovered as a product of monodromies around $0$ and $\infty$ given the properties
|
||||
\begin{equation}
|
||||
\begin{split}
|
||||
\cM_{\vb{0}}^+
|
||||
& =
|
||||
\cM_{\vb{0}}^-
|
||||
=
|
||||
\cM_{\vb{0}},
|
||||
\\
|
||||
\cM_{\vb{\infty}}^+
|
||||
& =
|
||||
\cM_{\vb{\infty}}^-
|
||||
=
|
||||
\cM_{\vb{\infty}},
|
||||
\end{split}
|
||||
\end{equation}
|
||||
which encode the peculiar branch cut structure due to the doubling trick gluing the intervals on one arbitrary D-brane.
|
||||
These matrices are an abstract representation of the monodromy group since they are in an arbitrary basis.
|
||||
|
||||
Using the basis in $z = 0$~\eqref{eq:basis_0} it is straightforward to find the explicit representation $\rM_{\vb{0}}$ of the abstract monodromy $\cM_{\vb{0}}$:
|
||||
\begin{equation}
|
||||
\rM_{\vb{0}}( c ) = \mqty( \dmat{1, e^{-2\pi i c}} ).
|
||||
\label{eq:monodromy_zero}
|
||||
\end{equation}
|
||||
The computation of the monodromy matrix $\rM_{\vb{\infty}}$ representing the monodromy in $\omega_z =\infty$ in the basis \eqref{eq:basis_0} requires to first compute the monodromy representation $\widetilde{\rM}_{\vb{\infty}}$ of the abstract monodromy $\cM_{\vb{\infty}}$ in the basis of hypergeometric functions around $z = \infty$:
|
||||
\begin{equation}
|
||||
B_{\vb{\infty}}(z)
|
||||
=
|
||||
\mqty(
|
||||
(-z)^{-a}~\hyp{a}{a+1-c}{a+1-b}{z^{-1}}
|
||||
\\
|
||||
(-z)^{-b}~\hyp{b}{b+1-c}{b+1-a}{z^{-1}}
|
||||
).
|
||||
\end{equation}
|
||||
This basis is connected to~\eqref{eq:basis_0} through the transition matrix
|
||||
\begin{equation}
|
||||
\cC( a,\, b,\, c )
|
||||
=
|
||||
\frac{\pi}{\sin(\pi(a-b))}
|
||||
\mqty(
|
||||
\frac{1}{\gfun{b}\gfun{c-a}}
|
||||
&
|
||||
-\frac{1}{\gfun{a} \gfun{c-b}}
|
||||
\\
|
||||
\frac{1}{\gfun{1-a}\gfun{b+1-c}}
|
||||
&
|
||||
-\frac{1}{\gfun{1-b}\gfun{a+1-c}}
|
||||
),
|
||||
\label{eq:transition_matrix}
|
||||
\end{equation}
|
||||
as $B_{\vb{0}}(z) = \cC(a,\, b,\, c)~B_{\vb{\infty}}(z)$.
|
||||
Through the loop $z \mapsto z e^{-2\pi i}$ we find:
|
||||
\begin{equation}
|
||||
\widetilde{\rM}_{\vb{\infty}}( a,\, b )
|
||||
=
|
||||
\mqty( \dmat{e^{2\pi i a}, e^{2\pi i b}} ).
|
||||
\end{equation}
|
||||
Finally we can build the desired monodromy:
|
||||
\begin{equation}
|
||||
\rM_{\vb{\infty}}
|
||||
=
|
||||
\cC(a,\, b,\, c)\,
|
||||
\widetilde{\rM}_{\vb{\infty}}(a,\, b)\,
|
||||
\cC^{-1}(a,\, b,\, c).
|
||||
\label{eq:monodromy_infty}
|
||||
\end{equation}
|
||||
|
||||
|
||||
\subsubsection{The Monodromy Factors}
|
||||
|
||||
With the previous definitions we reproduce the monodromies of the doubling field in its spinor representation~\eqref{eq:top_spinor_monodromy}.\footnotemark{}
|
||||
\footnotetext{%
|
||||
In general we do not need to consider~\eqref{eq:bottom_spinor_monodromy} since they are the same monodromies.
|
||||
}
|
||||
These monodromies are tensor products of two basis of hypergeometric functions: the first basis reproduces the monodromies defined as $\cL$ and the second one those defined as $\cR$ in~\eqref{eq:top_spinor_monodromy}.
|
||||
Since in principle there can be several combinations of parameters of the hypergeometric function yielding the same monodromy, we consider the full solution to be a linear superposition of all possible contributions:
|
||||
\begin{equation}
|
||||
\ipd{z} \cX(z)
|
||||
=
|
||||
\pdv{\omega_z}{z}\,
|
||||
\sum\limits_{l,\, r}
|
||||
c_{lr}\,
|
||||
\ipd{z} \cX_{l,r}(\omega_z),
|
||||
\label{eq:formal_solution}
|
||||
\end{equation}
|
||||
where we drop the index representing the spinorial representation to lighten the notation.
|
||||
We write any possible solution in a factorised form as
|
||||
\begin{equation}
|
||||
\ipd{z} \cX_{l,\,r}(\omega_z)
|
||||
=
|
||||
(-\omega_z)^{A_{lr}}\,
|
||||
(1-\omega_z)^{B_{lr}}\,
|
||||
\cB_{\vb{0},\, l}^{(L)}(\omega_z)
|
||||
\left( \cB_{\vb{0},\, r}^{(R)}(\omega_z) \right)^T,
|
||||
\label{eq:formal_solution_lr}
|
||||
\end{equation}
|
||||
where $l$ and $r$ label the parameters associates with the left and right sectors of the hypergeometric function.
|
||||
We introduce the left basis element
|
||||
\begin{equation}
|
||||
\begin{split}
|
||||
\cB_{\vb{0},\, l}^{(L)}(\omega_z)
|
||||
& =
|
||||
D^{(L)}_l~
|
||||
B_{\vb{0},\,l}^{(L)}(\omega_z)
|
||||
\\
|
||||
& =
|
||||
\mqty( 1 & 0 \\ 0 & K_l^{(L)} )\,
|
||||
\mqty(
|
||||
\hyp{a_l}{b_l}{c_l}{\omega_z}
|
||||
\\
|
||||
(-z)^{(1-c_l)}\,
|
||||
\hyp{a_l+1-c_l}{b_l+1-c_l}{2-c_l}{\omega_z}
|
||||
)
|
||||
\end{split}
|
||||
\end{equation}
|
||||
where $D_l^{(L)} \in \GL{2}{\C}$ is a relative normalisation matrix weighting differently the components of the basis.\footnotemark{}
|
||||
\footnotetext{%
|
||||
In general they can be different for each solution.
|
||||
}
|
||||
The right sector follows in a similar way.
|
||||
Notice that the matrices $D^{(L)}_l$ do not fix the absolute normalisation contained in $c_{lr}$.
|
||||
|
||||
|
||||
\subsubsection{Parameters of the Trivial Monodromy}
|
||||
|
||||
Using the previous relations we can determine the possible $\ipd{z} \cX_{l,r}(\omega_z)$ with the desired monodromies.
|
||||
In this section we study the case of the most general \SU{2} matrices despite the fact that in~\Cref{sec:special_SO4} we argued that they have a specific form.
|
||||
|
||||
First of all consider the matrices in \eqref{eq:monodromy_zero} and \eqref{eq:monodromy_infty}.
|
||||
We impose:
|
||||
\begin{eqnarray}
|
||||
&&\begin{cases}
|
||||
D^{(L)}\,
|
||||
\rM_{\vb{0}}^{(L)}\,
|
||||
\left( D^{(L)} \right)^{-1}
|
||||
=
|
||||
e^{-2\pi i \delta_{\vb{0}}^{(L)}}\,
|
||||
\cL(\vb{n}_{\vb{0}})
|
||||
\\
|
||||
D^{(R)}\,
|
||||
\rM_{\vb{0}}^{(R)}\,
|
||||
\left( D^{(R)} \right)^{-1}
|
||||
=
|
||||
e^{-2\pi i \delta_{\vb{0}}^{(R)}}\,
|
||||
\cR^*(\vb{m}_{\vb{0}})
|
||||
=
|
||||
e^{-2\pi i \delta_{\vb{0}}^{(R)}}\,
|
||||
\cR(\widetilde{\vb{m}}_{\vb{0}})
|
||||
\\
|
||||
e^{2\pi i ( A_{lr} - \delta_{\vb{0}}^{(L)} -
|
||||
\delta_{\vb{0}}^{(R)} )}
|
||||
=
|
||||
1
|
||||
\end{cases},
|
||||
\label{eq:parameters_equality_zero}
|
||||
\\
|
||||
&&\begin{cases}
|
||||
D^{(L)},
|
||||
\rM_{\vb{\infty}}^{(L)}\,
|
||||
\left( D^{(L)} \right)^{-1}
|
||||
=
|
||||
e^{-2\pi i \delta_{\vb{\infty}}^{(L)}}\,
|
||||
\cL(\vb{n}_{\vb{\infty}})
|
||||
\\
|
||||
D^{(R)}\,
|
||||
\rM_{\vb{\infty}}^{(R)}\,
|
||||
\left( D^{(R)} \right)^{-1}
|
||||
=
|
||||
e^{-2\pi i \delta_{\vb{\infty}}^{(R)}}\,
|
||||
\cR^*(\vb{m}_{\vb{\infty}})
|
||||
=
|
||||
e^{-2\pi i \delta_{\vb{\infty}}^{(R)}}\,
|
||||
\cR(\widetilde{\vb{m}}_{\vb{\infty}})
|
||||
\\
|
||||
e^{2\pi i ( A_{lr} + B_{lr} - \delta_{\vb{\infty}}^{(L)} -
|
||||
\delta_{\vb{\infty}}^{(R)} )}
|
||||
=
|
||||
1
|
||||
\end{cases},
|
||||
\label{eq:parameters_equality_infty}
|
||||
\end{eqnarray}
|
||||
where we defined
|
||||
\begin{eqnarray}
|
||||
\cL(\vb{n}_{\vb{0}})
|
||||
& = &
|
||||
\cL_{(\bt-1,\,\bt)}
|
||||
=
|
||||
U_L(\vb{n}_{(\bt)})\,
|
||||
U_L^{\dagger}(\vb{n}_{(\bt-1)}),
|
||||
\\
|
||||
\cL(\vb{n}_{\vb{\infty}})
|
||||
& = &
|
||||
\cL_{(\bt,\, \bt+1)}
|
||||
=
|
||||
U_L(\vb{n}_{(\bt+1)})
|
||||
U_L^{\dagger}(\vb{n}_{(\bt)}),
|
||||
\\
|
||||
\cR(\vb{m}_{\vb{0}})
|
||||
& = &
|
||||
\cR_{(\bt-1,\, \bt)}
|
||||
=
|
||||
U_R(\vb{n}_{(\bt)})
|
||||
U_R^{\dagger}(\vb{n}_{(\bt-1)}),
|
||||
\\
|
||||
\cR(\vb{m}_{\vb{\infty}})
|
||||
& = &
|
||||
\cR_{(\bt,\, \bt+1)}
|
||||
=
|
||||
U_R(\vb{n}_{(\bt+1)})
|
||||
U_R^{\dagger}(\vb{n}_{(\bt)}).
|
||||
\end{eqnarray}
|
||||
The range of $\delta_{\vb{0}}^{(L)}$ is
|
||||
\begin{equation}
|
||||
\alpha \le \delta_{\vb{0}}^{(L)} \le \alpha + \frac{1}{2},
|
||||
\end{equation}
|
||||
that is the width of the range is only $\frac{1}{2}$ and not $1$ as one would naively expect.
|
||||
This is a consequence of the fact that $e^{- 4 \pi i \delta_{\vb{0}}^{(L)}}$ is the determinant of the right hand side of the first equation in \eqref{eq:parameters_equality_zero}.
|
||||
We then choose $\alpha = 0$ for simplicity.
|
||||
The same considerations hold true for all the other additional parameters $\delta_{\vb{0}}^{(R)}$ and $\delta_{\vb{\infty}}^{(L,\,R)}$.
|
||||
|
||||
Since we are interested in relative rotations of the D-branes, we choose the
|
||||
rotation in $\omega_{\bt-1} = 0$ in the maximal torus of $\SU{2}_L \times \SU{2}_R$ without loss of generality: as we have two independent groups, we can in fact fix the orientation of both vectors $\vb{n}_{\vb{0}}$ and $\vb{m}_{\vb{0}}$.
|
||||
In particular we set:
|
||||
\begin{eqnarray}
|
||||
\vb{n}_{\vb{0}}
|
||||
=
|
||||
( 0,\, 0,\, n_{\vb{0}}^3 ) \in \R^3,
|
||||
& \qquad &
|
||||
0 < n_{\vb{0}}^3 < \frac{1}{2},
|
||||
\label{eq:maximal_torus_left}
|
||||
\\
|
||||
\widetilde{\vb{m}}_{\vb{0}}
|
||||
=
|
||||
( 0,\, 0,\, -m_{\vb{0}}^3 ) \in \R^3,
|
||||
& \qquad &
|
||||
0 < m_{\vb{0}}^3 < \frac{1}{2},
|
||||
\label{eq:maximal_torus_right}
|
||||
\end{eqnarray}
|
||||
where $n_{\vb{0}}^3 = 0$ is excluded to avoid considering a trivial rotation.
|
||||
We then define the parameters of the rotation in $\omega_{\bt} = \infty$ to be the most general
|
||||
\begin{equation}
|
||||
\begin{split}
|
||||
\vb{n}_{\vb{\infty}}
|
||||
& =
|
||||
( n_{\vb{\infty}}^1,\, n_{\vb{\infty}}^2,\, n_{\vb{\infty}}^3 ),
|
||||
\\
|
||||
\widetilde{\vb{m}}_{\vb{\infty}}
|
||||
& =
|
||||
( -m_{\vb{\infty}}^1,\, m_{\vb{\infty}}^2,\, -m_{\vb{\infty}}^3 ),
|
||||
\end{split}
|
||||
\end{equation}
|
||||
We could actually set $n_{\vb{\infty}}^2 = m_{\vb{\infty}}^2 = 0$ since the choice of the ``gauge''~\eqref{eq:maximal_torus_left} and~\eqref{eq:maximal_torus_right} is preserved by \U{1} rotations mixing $n_{\vb{\infty}}^1$ and $n_{\vb{\infty}}^2$.
|
||||
We nevertheless keep the general expression in order to check the computations.
|
||||
|
||||
Solving~\eqref{eq:parameters_equality_zero} and~\eqref{eq:parameters_equality_infty} connects the parameters of the hypergeometric function to the parameter of the rotations (see \Cref{sec:parameters}) thus reproducing the boundary conditions of the intersecting D-branes through the non trivial monodromies of the basis of hypergeometric functions.
|
||||
We find:
|
||||
\begin{eqnarray}
|
||||
a_l^{(L)}
|
||||
=
|
||||
n_{\vb{0}}
|
||||
+
|
||||
(-1)^{f^{(L)}}\, n_{\vb{1}}
|
||||
+
|
||||
n_{\vb{\infty}}
|
||||
+
|
||||
\ffa^{(L)}_l,
|
||||
& \qquad &
|
||||
\ffa^{(L)}_l \in \Z,
|
||||
\\
|
||||
b_l^{(L)}
|
||||
=
|
||||
n_{\vb{0}}
|
||||
+
|
||||
(-1)^{f^{(L)}}\, n_{\vb{1}}
|
||||
-
|
||||
n_{\vb{\infty}}
|
||||
+
|
||||
\ffb^{(L)}_l,
|
||||
& \qquad &
|
||||
\ffb^{(L)}_l \in \Z,
|
||||
\\
|
||||
c_l^{(L)}
|
||||
=
|
||||
2\, n_{\vb{0}}
|
||||
+
|
||||
\ffc^{(L)}_l,
|
||||
& \qquad &
|
||||
\ffc^{(L)}_l \in \Z,
|
||||
\\
|
||||
\delta_{\vb{0}}^{(L)}
|
||||
=
|
||||
n_{\vb{0}},
|
||||
\\
|
||||
\delta_{\vb{\infty}}^{(L)}
|
||||
=
|
||||
-
|
||||
n_{\vb{0}}
|
||||
-
|
||||
(-1)^{f^{(L)}}\, n_{\vb{1}},
|
||||
\\
|
||||
K^{(L)}_l
|
||||
=
|
||||
-\frac{1}{2 \pi^2}\,
|
||||
\cG(a_l^{(L)},\, b_l^{(L)},\, c_l^{(L)})\,
|
||||
\cF(a_l^{(L)},\, b_l^{(L)},\, c_l^{(L)})\,
|
||||
\frac{n^1_{\vb{\infty}}+ i\, n^2_{\vb{\infty}}}{n_{\vb{\infty}}},
|
||||
\label{eq:K_factor_value}
|
||||
\end{eqnarray}
|
||||
where $f^{(L)} \in \left\lbrace 0,\, 1 \right\rbrace$.
|
||||
For the sake of brevity we defined two auxiliary functions, namely $\cG(a,\, b,\, c) = \gfun{1-a}\, \gfun{1-b}\, \gfun{a+1-c}\, \gfun{b+1-c}$ and $\cF(a,\, b,\, c) = \sin(\pi c)\, \sin(\pi(a-b))$.
|
||||
We also introduced the norm $n_{\vb{1}} = \norm{\vb{n}_{\vb{1}}}$ of the rotation vector around $\omega_{\bt+1} = 1$.
|
||||
Its dependence on the other parameters is encoded in~\eqref{eq:monodromy_relations}, where $\rM^+_{\vb{1}} = \rM^{-1}_{\vb{0}}\, \rM^{-1}_{\vb{\infty}}$, and the composition rule~\eqref{eq:product_in_SU2}:
|
||||
\begin{equation}
|
||||
\cos(2\pi n_{\vb{1}})
|
||||
=
|
||||
\cos(2\pi n_{\vb{0}})\,
|
||||
\cos(2\pi n_{\vb{\infty}})
|
||||
-
|
||||
\sin(2\pi n_{\vb{0}})\,
|
||||
\sin(2\pi n_{\vb{\infty}})\,
|
||||
\frac{n_{\vb{\infty}}^3}{n_{\vb{\infty}}}.
|
||||
\label{eq:dependent_monodromy_main_text}
|
||||
\end{equation}
|
||||
Relations for the right sector follow under the interchange of $(L)$ with $(R)$ and $\vb{n} \leftrightarrow \vb{m}$.
|
||||
|
||||
Parameters $A_{lr}$ and $B_{lr}$ follow the previous results and equations~\eqref{eq:parameters_equality_zero} and \eqref{eq:parameters_equality_infty}:
|
||||
\begin{eqnarray}
|
||||
A_{lr}
|
||||
=
|
||||
n_{\vb{0}} + m_{\vb{0}} + \ffA_{lr},
|
||||
& \qquad &
|
||||
\ffA_{lr} \in \Z,
|
||||
\\
|
||||
B_{lr}
|
||||
(-1)^{f^{(L)}}\, n_{\vb{1}} + (-1)^{f^{(R)}}\, m_{\vb{1}} + \ffB_{lr},
|
||||
& \qquad &
|
||||
\ffB_{lr} \in \Z.
|
||||
\end{eqnarray}
|
||||
|
||||
|
||||
% vim: ft=tex
|
||||
|
||||
@@ -1 +1 @@
|
||||
% vim ft=tex
|
||||
% vim: ft=tex
|
||||
|
||||
@@ -1354,4 +1354,4 @@ Consider for example the simple \cy factorised manifold $T^6 = T^2 \times T^2 \t
|
||||
Even though the lines might never intersect on a plane, they can come across on a torus due to the identifications~\cite{Zwiebach::FirstCourseString}.
|
||||
Since each intersections supports a different set of fermions with different spectrum, the angles of the intersecting branes can be calibrated to reproduce the separation in mass of the families of quarks and leptons in the \sm.
|
||||
|
||||
% vim ft=tex
|
||||
% vim: ft=tex
|
||||
|
||||
@@ -1 +1 @@
|
||||
% vim ft=tex
|
||||
% vim: ft=tex
|
||||
|
||||
@@ -1 +1 @@
|
||||
% vim ft=tex
|
||||
% vim: ft=tex
|
||||
|
||||
160
thesis.bib
160
thesis.bib
@@ -1,7 +1,7 @@
|
||||
|
||||
@article{Abel:2003:FlavourChangingNeutral,
|
||||
title = {Flavour {{Changing Neutral Currents}} in {{Intersecting Brane Models}}},
|
||||
author = {Abel, S. and Masip, M. and Santiago, J.},
|
||||
author = {Abel, Steven A. and Masip, Manuel and Santiago, Jose},
|
||||
date = {2003-04-30},
|
||||
journaltitle = {Journal of High Energy Physics},
|
||||
shortjournal = {J. High Energy Phys.},
|
||||
@@ -13,13 +13,13 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {hep-ph/0303087},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/abel_et_al_2003_flavour_changing_neutral_currents_in_intersecting_brane_models.pdf;/home/riccardo/.local/share/zotero/storage/U4DUJK6P/0303087.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/abel_et_al_2003_flavour_changing_neutral_currents_in_intersecting_brane_models.pdf},
|
||||
number = {04}
|
||||
}
|
||||
|
||||
@article{Abel:2005:OneloopYukawasIntersecting,
|
||||
title = {One-Loop {{Yukawas}} on {{Intersecting Branes}}},
|
||||
author = {Abel, S. A. and Schofield, B. W.},
|
||||
author = {Abel, Steven A. and Schofield, Ben W.},
|
||||
date = {2005-06-28},
|
||||
journaltitle = {Journal of High Energy Physics},
|
||||
shortjournal = {J. High Energy Phys.},
|
||||
@@ -31,7 +31,7 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {hep-th/0412206},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/abel_schofield_2005_one-loop_yukawas_on_intersecting_branes5.pdf;/home/riccardo/.local/share/zotero/storage/2LCUN7BE/0412206.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/abel_schofield_2005_one-loop_yukawas_on_intersecting_branes5.pdf},
|
||||
number = {06}
|
||||
}
|
||||
|
||||
@@ -49,14 +49,14 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {hep-th/0612110},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/abel_goodsell_2007_realistic_yukawa_couplings_through_instantons_in_intersecting_brane_worlds8.pdf;/home/riccardo/.local/share/zotero/storage/5HFIE6GC/0612110.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/abel_goodsell_2007_realistic_yukawa_couplings_through_instantons_in_intersecting_brane_worlds8.pdf},
|
||||
number = {10}
|
||||
}
|
||||
|
||||
@article{Aldazabal:2000:DBranesSingularitiesBottomUp,
|
||||
title = {D-{{Branes}} at {{Singularities}} : {{A Bottom}}-{{Up Approach}} to the {{String Embedding}} of the {{Standard Model}}},
|
||||
shorttitle = {D-{{Branes}} at {{Singularities}}},
|
||||
author = {Aldazabal, G. and Ibanez, L. E. and Quevedo, F. and Uranga, A. M.},
|
||||
author = {Aldazabal, Gerardo and Ibanez, Luis E. and Quevedo, Fernando and Uranga, Angel M.},
|
||||
date = {2000-08-01},
|
||||
journaltitle = {Journal of High Energy Physics},
|
||||
shortjournal = {J. High Energy Phys.},
|
||||
@@ -68,7 +68,7 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {hep-th/0005067},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/aldazabal_et_al_2000_d-branes_at_singularities.pdf;/home/riccardo/.local/share/zotero/storage/BTI6TASA/0005067.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/aldazabal_et_al_2000_d-branes_at_singularities.pdf},
|
||||
number = {08}
|
||||
}
|
||||
|
||||
@@ -76,15 +76,12 @@
|
||||
title = {On Closed-String Twist-Field Correlators and Their Open-String Descendants},
|
||||
author = {Anastasopoulos, Pascal and Bianchi, Massimo and Richter, Robert},
|
||||
date = {2011-10-24},
|
||||
url = {http://arxiv.org/abs/1110.5359},
|
||||
urldate = {2020-09-09},
|
||||
abstract = {In a recent paper we have proposed the possibility that the lightest massive string states could be identified with open strings living at intersections of D-branes forming small angles. In this note, we reconsider the relevant twist-field correlation functions and perform the analysis of the sub-dominant physical poles in the various channels. Our derivation is new in that it is based on the algebraic procedure for the construction of open string models starting from their closed-string `parents' rather than on the stress-tensor method. We also indicate possible generalizations and diverse applications of our approach.},
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {1110.5359},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/anastasopoulos_et_al_2011_on_closed-string_twist-field_correlators_and_their_open-string_descendants5.pdf;/home/riccardo/.local/share/zotero/storage/FNUNE3XD/1110.html},
|
||||
keywords = {⛔ No DOI found},
|
||||
primaryClass = {hep-th}
|
||||
file = {/home/riccardo/.local/share/zotero/files/anastasopoulos_et_al_2011_on_closed-string_twist-field_correlators_and_their_open-string_descendants5.pdf},
|
||||
keywords = {⛔ No DOI found}
|
||||
}
|
||||
|
||||
@article{Anastasopoulos:2012:LightStringyStates,
|
||||
@@ -101,7 +98,7 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {1110.5424},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/anastasopoulos_et_al_2012_light_stringy_states5.pdf;/home/riccardo/.local/share/zotero/storage/V9K88VXH/1110.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/anastasopoulos_et_al_2012_light_stringy_states5.pdf},
|
||||
number = {3}
|
||||
}
|
||||
|
||||
@@ -119,7 +116,7 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {1305.7166},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/anastasopoulos_et_al_2013_three-_and_four-point_correlators_of_excited_bosonic_twist_fields9.pdf;/home/riccardo/.local/share/zotero/storage/I9E3VKI4/1305.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/anastasopoulos_et_al_2013_three-_and_four-point_correlators_of_excited_bosonic_twist_fields9.pdf},
|
||||
number = {10}
|
||||
}
|
||||
|
||||
@@ -136,7 +133,7 @@
|
||||
|
||||
@article{Angelantonj:2000:TypeIStringsMagnetised,
|
||||
title = {Type-{{I}} Strings on Magnetised Orbifolds and Brane Transmutation},
|
||||
author = {Angelantonj, C. and Antoniadis, I. and Dudas, E. and Sagnotti, A.},
|
||||
author = {Angelantonj, Carlo and Antoniadis, Ignatios and Dudas, Emilian and Sagnotti, Augusto},
|
||||
date = {2000-09},
|
||||
journaltitle = {Physics Letters B},
|
||||
shortjournal = {Physics Letters B},
|
||||
@@ -148,7 +145,7 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {hep-th/0007090},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/angelantonj_et_al_2000_type-i_strings_on_magnetised_orbifolds_and_brane_transmutation.pdf;/home/riccardo/.local/share/zotero/storage/3T3IDPLZ/0007090.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/angelantonj_et_al_2000_type-i_strings_on_magnetised_orbifolds_and_brane_transmutation.pdf},
|
||||
number = {1-2}
|
||||
}
|
||||
|
||||
@@ -178,14 +175,14 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {hep-th/9606139},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/berkooz_et_al_1996_branes_intersecting_at_angles5.pdf;/home/riccardo/.local/share/zotero/storage/A5B8IC2L/9606139.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/berkooz_et_al_1996_branes_intersecting_at_angles5.pdf},
|
||||
number = {1-2}
|
||||
}
|
||||
|
||||
@article{Berkooz:2004:ClosedStringsMisner,
|
||||
title = {Closed {{Strings}} in {{Misner Space}}: {{Stringy Fuzziness}} with a {{Twist}}},
|
||||
shorttitle = {Closed {{Strings}} in {{Misner Space}}},
|
||||
author = {Berkooz, M. and Durin, B. and Pioline, B. and Reichmann, D.},
|
||||
author = {Berkooz, Micha and Durin, Bruno and Pioline, Boris and Reichmann, Dori},
|
||||
date = {2004-10-02},
|
||||
journaltitle = {Journal of Cosmology and Astroparticle Physics},
|
||||
shortjournal = {J. Cosmol. Astropart. Phys.},
|
||||
@@ -197,7 +194,7 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {hep-th/0407216},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/berkooz_et_al_2004_closed_strings_in_misner_space8.pdf;/home/riccardo/.local/share/zotero/storage/FLJKNMJR/0407216.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/berkooz_et_al_2004_closed_strings_in_misner_space8.pdf},
|
||||
number = {10}
|
||||
}
|
||||
|
||||
@@ -215,7 +212,7 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {hep-th/0512067},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/bertolini_et_al_2006_brane_world_effective_actions_for_d-branes_with_fluxes5.pdf;/home/riccardo/.local/share/zotero/storage/DP7XCH8F/0512067.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/bertolini_et_al_2006_brane_world_effective_actions_for_d-branes_with_fluxes5.pdf},
|
||||
number = {1-2}
|
||||
}
|
||||
|
||||
@@ -233,7 +230,7 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {hep-th/0502147},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/bianchi_trevigne_2005_the_open_story_of_the_magnetic_fluxes5.pdf;/home/riccardo/.local/share/zotero/storage/NH9MPEJT/0502147.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/bianchi_trevigne_2005_the_open_story_of_the_magnetic_fluxes5.pdf},
|
||||
number = {08}
|
||||
}
|
||||
|
||||
@@ -295,13 +292,13 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {hep-th/0004134},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/bousso_polchinski_2000_quantization_of_four-form_fluxes_and_dynamical_neutralization_of_the.pdf;/home/riccardo/.local/share/zotero/storage/2LKAEYI3/0004134.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/bousso_polchinski_2000_quantization_of_four-form_fluxes_and_dynamical_neutralization_of_the.pdf},
|
||||
number = {06}
|
||||
}
|
||||
|
||||
@article{Brown:1988:NeutralizationCosmologicalConstant,
|
||||
title = {Neutralization of the Cosmological Constant by Membrane Creation},
|
||||
author = {Brown, J.David and Teitelboim, Claudio},
|
||||
author = {Brown, David J. and Teitelboim, Claudio},
|
||||
date = {1988-02},
|
||||
journaltitle = {Nuclear Physics B},
|
||||
shortjournal = {Nuclear Physics B},
|
||||
@@ -318,7 +315,7 @@
|
||||
|
||||
@article{Burwick:1991:GeneralYukawaCouplings,
|
||||
title = {General {{Yukawa}} Couplings of Strings on Orbifolds},
|
||||
author = {Burwick, T.T. and Kaiser, R.K. and Müller, H.F.},
|
||||
author = {Burwick, Thomas T. and Kaiser, Ralf K. and Müller, H. F.},
|
||||
date = {1991-05},
|
||||
journaltitle = {Nuclear Physics B},
|
||||
shortjournal = {Nuclear Physics B},
|
||||
@@ -340,7 +337,8 @@
|
||||
date = {1957},
|
||||
volume = {12},
|
||||
pages = {78--89},
|
||||
doi = {10.1515/9781400879915-006}
|
||||
doi = {10.1515/9781400879915-006},
|
||||
file = {/home/riccardo/.local/share/zotero/files/calabi_1957_on_kähler_manifolds_with_vanishing_canonical_class.pdf}
|
||||
}
|
||||
|
||||
@article{Candelas:1985:VacuumConfigurationsSuperstrings,
|
||||
@@ -361,7 +359,7 @@
|
||||
|
||||
@article{Chamoun:2004:FermionMassesMixing,
|
||||
title = {Fermion Masses and Mixing in Intersecting Brane Scenarios},
|
||||
author = {Chamoun, N. and Khalil, S. and Lashin, E.},
|
||||
author = {Chamoun, Nidal and Khalil, Shaaban and Lashin, Elsayed},
|
||||
date = {2004-05-26},
|
||||
journaltitle = {Physical Review D},
|
||||
shortjournal = {Phys. Rev. D},
|
||||
@@ -380,7 +378,7 @@
|
||||
|
||||
@article{Chen:2008:RealisticWorldIntersecting,
|
||||
title = {A {{Realistic World}} from {{Intersecting D6}}-{{Branes}}},
|
||||
author = {Chen, Ching-Ming and Li, Tianjun and Mayes, V. E. and Nanopoulos, Dimitri V.},
|
||||
author = {Chen, Ching-Ming and Li, Tianjun and Mayes, van Eric and Nanopoulos, Dimitri V.},
|
||||
date = {2008-07},
|
||||
journaltitle = {Physics Letters B},
|
||||
shortjournal = {Physics Letters B},
|
||||
@@ -392,13 +390,13 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {hep-th/0703280},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/chen_et_al_2008_a_realistic_world_from_intersecting_d6-branes.pdf;/home/riccardo/.local/share/zotero/storage/3MKTIA92/0703280.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/chen_et_al_2008_a_realistic_world_from_intersecting_d6-branes.pdf},
|
||||
number = {4}
|
||||
}
|
||||
|
||||
@article{Chen:2008:RealisticYukawaTextures,
|
||||
title = {Realistic {{Yukawa Textures}} and {{SUSY Spectra}} from {{Intersecting Branes}}},
|
||||
author = {Chen, Ching-Ming and Li, Tianjun and Mayes, V. E. and Nanopoulos, D. V.},
|
||||
author = {Chen, Ching-Ming and Li, Tianjun and Mayes, van Eric and Nanopoulos, Dimitri V.},
|
||||
date = {2008-06-20},
|
||||
journaltitle = {Physical Review D},
|
||||
shortjournal = {Phys. Rev. D},
|
||||
@@ -410,7 +408,7 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {0711.0396},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/chen_et_al_2008_realistic_yukawa_textures_and_susy_spectra_from_intersecting_branes.pdf;/home/riccardo/.local/share/zotero/storage/3CUNZ86H/0711.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/chen_et_al_2008_realistic_yukawa_textures_and_susy_spectra_from_intersecting_branes.pdf},
|
||||
number = {12}
|
||||
}
|
||||
|
||||
@@ -427,7 +425,7 @@
|
||||
|
||||
@article{Cremades:2003:YukawaCouplingsIntersecting,
|
||||
title = {Yukawa Couplings in Intersecting {{D}}-Brane Models},
|
||||
author = {Cremades, D. and Ibanez, L. E. and Marchesano, F.},
|
||||
author = {Cremades, Daniel and Ibanez, Luis E. and Marchesano, Fernando},
|
||||
date = {2003-07-16},
|
||||
journaltitle = {Journal of High Energy Physics},
|
||||
shortjournal = {J. High Energy Phys.},
|
||||
@@ -439,7 +437,7 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {hep-th/0302105},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/cremades_et_al_2003_yukawa_couplings_in_intersecting_d-brane_models5.pdf;/home/riccardo/.local/share/zotero/storage/49DFN84N/0302105.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/cremades_et_al_2003_yukawa_couplings_in_intersecting_d-brane_models5.pdf},
|
||||
number = {07}
|
||||
}
|
||||
|
||||
@@ -457,7 +455,7 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {0905.1694},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/cvetič_et_al_2010_branes_and_instantons_intersecting_at_angles.pdf;/home/riccardo/.local/share/zotero/storage/H2QKB4Y5/0905.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/cvetič_et_al_2010_branes_and_instantons_intersecting_at_angles.pdf},
|
||||
number = {1}
|
||||
}
|
||||
|
||||
@@ -475,13 +473,13 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {hep-th/0305081},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/d'appollonio_kiritsis_2003_string_interactions_in_gravitational_wave_backgrounds5.pdf;/home/riccardo/.local/share/zotero/storage/RDEYCNST/0305081.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/d'appollonio_kiritsis_2003_string_interactions_in_gravitational_wave_backgrounds5.pdf},
|
||||
number = {1-2}
|
||||
}
|
||||
|
||||
@article{DAppollonio:2005:DbranesBCFTHppwave,
|
||||
title = {D-Branes and {{BCFT}} in {{Hpp}}-Wave Backgrounds},
|
||||
author = {D'Appollonio, G. and Kiritsis, E.},
|
||||
author = {D'Appollonio, Giuseppe and Kiritsis, Elias},
|
||||
date = {2005-04},
|
||||
journaltitle = {Nuclear Physics B},
|
||||
shortjournal = {Nuclear Physics B},
|
||||
@@ -493,7 +491,7 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {hep-th/0410269},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/d'appollonio_kiritsis_2005_d-branes_and_bcft_in_hpp-wave_backgrounds5.pdf;/home/riccardo/.local/share/zotero/storage/JEE8EF46/0410269.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/d'appollonio_kiritsis_2005_d-branes_and_bcft_in_hpp-wave_backgrounds5.pdf},
|
||||
number = {3}
|
||||
}
|
||||
|
||||
@@ -511,7 +509,7 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {hep-th/0007235},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/david_2000_tachyon_condensation_in_the_d0-d4_system.pdf;/home/riccardo/.local/share/zotero/storage/2U52Z9Q4/0007235.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/david_2000_tachyon_condensation_in_the_d0-d4_system.pdf},
|
||||
number = {10}
|
||||
}
|
||||
|
||||
@@ -529,7 +527,7 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {hep-th/0012089},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/david_2001_tachyon_condensation_using_the_disc_partition_function5.pdf;/home/riccardo/.local/share/zotero/storage/VRQZCMVC/0012089.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/david_2001_tachyon_condensation_using_the_disc_partition_function5.pdf},
|
||||
number = {07}
|
||||
}
|
||||
|
||||
@@ -547,13 +545,13 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {hep-th/0111212},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/david_et_al_2002_closed_string_tachyon_condensation_on_twisted_circles5.pdf;/home/riccardo/.local/share/zotero/storage/LVI9CWIS/0111212.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/david_et_al_2002_closed_string_tachyon_condensation_on_twisted_circles5.pdf},
|
||||
number = {02}
|
||||
}
|
||||
|
||||
@article{DellaSelva:1970:SimpleExpressionSciuto,
|
||||
title = {A Simple Expression for the {{Sciuto}} Three-Reggeon Vertex-Generating Duality},
|
||||
author = {Della Selva, A. and Saito, S.},
|
||||
author = {Della Selva, Angelo and Saito, Satoru},
|
||||
date = {1970-10},
|
||||
journaltitle = {Lettere al Nuovo Cimento},
|
||||
shortjournal = {Lett. Nuovo Cimento},
|
||||
@@ -599,7 +597,7 @@
|
||||
@inproceedings{DiVecchia:1999:DbranesStringTheory,
|
||||
title = {D-Branes in String Theory {{II}}},
|
||||
booktitle = {{{YITP}} Workshop on Developments in Superstring and {{M}} Theory},
|
||||
author = {Di Vecchia, P. and Liccardo, Antonella},
|
||||
author = {Di Vecchia, Paolo and Liccardo, Antonella},
|
||||
date = {1999-12},
|
||||
pages = {7--48},
|
||||
archivePrefix = {arXiv},
|
||||
@@ -624,13 +622,15 @@
|
||||
number = {NORDITA-1999-77-HE}
|
||||
}
|
||||
|
||||
@article{DiVecchia:2006:BoundaryStateMagnetized,
|
||||
@inproceedings{DiVecchia:2006:BoundaryStateMagnetized,
|
||||
title = {Boundary {{State}} for {{Magnetized D9 Branes}} and {{One}}-{{Loop Calculation}}},
|
||||
booktitle = {Sense of {{Beauty}} in {{Physics}}: {{Miniconference}} in {{Honor}} of {{Adriano Di Giacomo}} on His 70th {{Birthday}}},
|
||||
author = {Di Vecchia, Paolo and Liccardo, Antonella and Marotta, Raffaele and Pezzella, Franco and Pesando, Igor},
|
||||
date = {2006-01},
|
||||
url = {http://arxiv.org/abs/hep-th/0601067},
|
||||
abstract = {We construct the boundary state describing magnetized D9 branes in R\^\{3,1\} x T\^6 and we use it to compute the annulus and Moebius amplitudes. We derive from them, by using open/closed string duality, the number of Landau levels on the torus T\^d.},
|
||||
annotation = {ZSCC: 0000007},
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {hep-th/0601067},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/di_vecchia_et_al_2006_boundary_state_for_magnetized_d9_branes_and_one-loop_calculation.pdf}
|
||||
}
|
||||
|
||||
@@ -657,7 +657,7 @@
|
||||
|
||||
@article{DiVecchia:2011:OpenStringsSystem,
|
||||
title = {Open Strings in the System {{D5}}/{{D9}}},
|
||||
author = {Di Vecchia, P. and Marotta, R. and Pesando, I. and Pezzella, F.},
|
||||
author = {Di Vecchia, Paolo and Marotta, Raffaele and Pesando, Igor and Pezzella, Franco},
|
||||
date = {2011-06-17},
|
||||
journaltitle = {Journal of Physics A: Mathematical and Theoretical},
|
||||
shortjournal = {J. Phys. A: Math. Theor.},
|
||||
@@ -669,7 +669,7 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {1101.0120},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/di_vecchia_et_al_2011_open_strings_in_the_system_d5-d5.pdf;/home/riccardo/.local/share/zotero/storage/5AHE9Z2W/1101.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/di_vecchia_et_al_2011_open_strings_in_the_system_d5-d5.pdf},
|
||||
number = {24}
|
||||
}
|
||||
|
||||
@@ -687,13 +687,13 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {0709.1805},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/duo_et_al_2007_new_twist_field_couplings_from_the_partition_function_for_multiply_wrapped5.pdf;/home/riccardo/.local/share/zotero/storage/V7S6EP95/0709.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/duo_et_al_2007_new_twist_field_couplings_from_the_partition_function_for_multiply_wrapped5.pdf},
|
||||
number = {12}
|
||||
}
|
||||
|
||||
@article{Erler:1993:HigherTwistedSector,
|
||||
title = {Higher {{Twisted Sector Couplings}} of \${{Z}}\_{{N}}\$ {{Orbifolds}}},
|
||||
author = {Erler, J. and Jungnickel, D. and Spalinski, M. and Stieberger, S.},
|
||||
title = {Higher {{Twisted Sector Couplings}} of {{ZN Orbifolds}}},
|
||||
author = {Erler, Jens and Jungnickel, Dirk-U. and Spaliński, Michał and Stieberger, Stephan},
|
||||
date = {1993-05},
|
||||
journaltitle = {Nuclear Physics B},
|
||||
shortjournal = {Nuclear Physics B},
|
||||
@@ -705,7 +705,7 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {hep-th/9207049},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/erler_et_al_1993_higher_twisted_sector_couplings_of_$z_n$_orbifolds.pdf;/home/riccardo/.local/share/zotero/storage/R797YJWK/9207049.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/erler_et_al_1993_higher_twisted_sector_couplings_of_$z_n$_orbifolds.pdf},
|
||||
number = {1-2}
|
||||
}
|
||||
|
||||
@@ -742,7 +742,7 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {1802.05136},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/forste_liyanage_2018_yukawa_couplings_from_magnetized_d-brane_models_on_non-factorisable_tori.pdf;/home/riccardo/.local/share/zotero/storage/6I8WLCI5/1802.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/forste_liyanage_2018_yukawa_couplings_from_magnetized_d-brane_models_on_non-factorisable_tori.pdf},
|
||||
number = {8}
|
||||
}
|
||||
|
||||
@@ -760,7 +760,7 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {hep-th/0011186},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/frampton_kephart_2001_classification_of_conformality_models_based_on_nonabelian_orbifolds5.pdf;/home/riccardo/.local/share/zotero/storage/JDK2473W/0011186.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/frampton_kephart_2001_classification_of_conformality_models_based_on_nonabelian_orbifolds5.pdf},
|
||||
number = {8}
|
||||
}
|
||||
|
||||
@@ -797,7 +797,7 @@
|
||||
|
||||
@article{Gava:1997:BoundStatesBranes,
|
||||
title = {On the {{Bound States}} of P- and (P+2)-{{Branes}}},
|
||||
author = {Gava, E. and Narain, K. S. and Sarmadi, M. H.},
|
||||
author = {Gava, Edi and Narain, Kumar S. and Sarmadi, Hossein M.},
|
||||
date = {1997-10},
|
||||
journaltitle = {Nuclear Physics B},
|
||||
shortjournal = {Nuclear Physics B},
|
||||
@@ -809,7 +809,7 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {hep-th/9704006},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/gava_et_al_1997_on_the_bound_states_of_p-_and_(p+2)-branes.pdf;/home/riccardo/.local/share/zotero/storage/UP983WKN/9704006.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/gava_et_al_1997_on_the_bound_states_of_p-_and_(p+2)-branes.pdf},
|
||||
number = {1-2}
|
||||
}
|
||||
|
||||
@@ -826,7 +826,7 @@
|
||||
|
||||
@article{Goddard:1973:QuantumDynamicsMassless,
|
||||
title = {Quantum Dynamics of a Massless Relativistic String},
|
||||
author = {Goddard, P. and Goldstone, J. and Rebbi, C. and Thorn, C.B.},
|
||||
author = {Goddard, Peter and Goldstone, Jeffrey and Rebbi, Claudio and Thorn, Charles B.},
|
||||
date = {1973-05},
|
||||
journaltitle = {Nuclear Physics B},
|
||||
shortjournal = {Nuclear Physics B},
|
||||
@@ -899,7 +899,7 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {hep-th/9702155},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/greene_1997_string_theory_on_calabi-yau_manifolds.pdf;/home/riccardo/.local/share/zotero/storage/R7F26ND6/9702155.html}
|
||||
file = {/home/riccardo/.local/share/zotero/files/greene_1997_string_theory_on_calabi-yau_manifolds.pdf}
|
||||
}
|
||||
|
||||
@article{Grimm:2005:EffectiveActionType,
|
||||
@@ -933,7 +933,7 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {hep-th/0303204},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/hashimoto_nagaoka_2003_recombination_of_intersecting_d-branes_by_local_tachyon_condensation5.pdf;/home/riccardo/.local/share/zotero/storage/8I2UAHW2/0303204.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/hashimoto_nagaoka_2003_recombination_of_intersecting_d-branes_by_local_tachyon_condensation5.pdf},
|
||||
number = {06}
|
||||
}
|
||||
|
||||
@@ -994,7 +994,7 @@
|
||||
|
||||
@article{Inoue:1987:NonAbelianOrbifolds,
|
||||
title = {Non-{{Abelian Orbifolds}}},
|
||||
author = {Inoue, K. and Sakamoto, M. and Takano, H.},
|
||||
author = {Inoue, Kenzo and Sakamoto, Makoto and Takano, Hiroshi},
|
||||
date = {1987-10-01},
|
||||
journaltitle = {Progress of Theoretical Physics},
|
||||
shortjournal = {Progress of Theoretical Physics},
|
||||
@@ -1011,7 +1011,7 @@
|
||||
|
||||
@article{Inoue:1990:StringInteractionsNonAbelian,
|
||||
title = {String {{Interactions}} on {{Non}}-{{Abelian Orbifold}}},
|
||||
author = {Inoue, K. and Nima, S.},
|
||||
author = {Inoue, Kenzo and Nima, Shuij},
|
||||
date = {1990-10-01},
|
||||
journaltitle = {Progress of Theoretical Physics},
|
||||
shortjournal = {Progress of Theoretical Physics},
|
||||
@@ -1019,7 +1019,6 @@
|
||||
pages = {702--727},
|
||||
issn = {0033-068X, 1347-4081},
|
||||
doi = {10.1143/ptp/84.4.702},
|
||||
annotation = {http://web.archive.org/web/20200909163702/https://academic.oup.com/ptp/article/84/4/702/1892630},
|
||||
file = {/home/riccardo/.local/share/zotero/files/inoue_nima_1990_string_interactions_on_non-abelian_orbifold.pdf},
|
||||
keywords = {archived},
|
||||
langid = {english},
|
||||
@@ -1075,13 +1074,13 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {hep-th/0301240},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/kachru_et_al_2003_de_sitter_vacua_in_string_theory.pdf;/home/riccardo/.local/share/zotero/storage/AABMA8ED/0301240.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/kachru_et_al_2003_de_sitter_vacua_in_string_theory.pdf},
|
||||
number = {4}
|
||||
}
|
||||
|
||||
@article{Kiritsis:1994:StringPropagationGravitational,
|
||||
title = {String {{Propagation}} in {{Gravitational Wave Backgrounds}}},
|
||||
author = {Kiritsis, E. and Kounnas, C.},
|
||||
author = {Kiritsis, Elias and Kounnas, Costas},
|
||||
date = {1994-01},
|
||||
journaltitle = {Physics Letters B},
|
||||
shortjournal = {Physics Letters B},
|
||||
@@ -1093,7 +1092,7 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {hep-th/9310202},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/kiritsis_kounnas_1994_string_propagation_in_gravitational_wave_backgrounds5.pdf;/home/riccardo/.local/share/zotero/storage/JKGFBSHR/9310202.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/kiritsis_kounnas_1994_string_propagation_in_gravitational_wave_backgrounds5.pdf},
|
||||
number = {3-4}
|
||||
}
|
||||
|
||||
@@ -1129,7 +1128,7 @@
|
||||
|
||||
@article{Paton:1969:GeneralizedVenezianoModel,
|
||||
title = {Generalized {{Veneziano}} Model with Isospin},
|
||||
author = {Paton, J.E. and {Chan Hong-Mo}},
|
||||
author = {Paton, Jack E. and {Chan Hong-Mo}},
|
||||
date = {1969-05},
|
||||
journaltitle = {Nuclear Physics B},
|
||||
shortjournal = {Nuclear Physics B},
|
||||
@@ -1172,7 +1171,7 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {0910.2576},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/pesando_2010_open_and_closed_string_vertices_for_branes_with_magnetic_field_and_t-duality5.pdf;/home/riccardo/.local/share/zotero/storage/7G2ISTM4/0910.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/pesando_2010_open_and_closed_string_vertices_for_branes_with_magnetic_field_and_t-duality5.pdf},
|
||||
number = {2}
|
||||
}
|
||||
|
||||
@@ -1180,13 +1179,11 @@
|
||||
title = {The Generating Function of Amplitudes with {{N}} Twisted and {{M}} Untwisted States},
|
||||
author = {Pesando, Igor},
|
||||
date = {2011-07-27},
|
||||
url = {http://arxiv.org/abs/1107.5525},
|
||||
urldate = {2020-09-09},
|
||||
abstract = {We show that the generating function of all amplitudes with N twisted and M untwisted states, i.e. the Reggeon vertex for magnetized branes on R\^2 can be computed once the correlator of N non excited twisted states and the corresponding Green function are known and we give an explicit expression as a functional of the these objects},
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {1107.5525},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/pesando_2011_the_generating_function_of_amplitudes_with_n_twisted_and_m_untwisted_states.pdf;/home/riccardo/.local/share/zotero/storage/RFT279XA/1107.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/pesando_2011_the_generating_function_of_amplitudes_with_n_twisted_and_m_untwisted_states.pdf},
|
||||
keywords = {⛔ No DOI found},
|
||||
primaryClass = {hep-th}
|
||||
}
|
||||
@@ -1205,7 +1202,7 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {1101.5898},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/pesando_2011_strings_in_an_arbitrary_constant_magnetic_field_with_arbitrary_constant_metric5.pdf;/home/riccardo/.local/share/zotero/storage/5WS8IWA9/1101.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/pesando_2011_strings_in_an_arbitrary_constant_magnetic_field_with_arbitrary_constant_metric5.pdf},
|
||||
number = {6}
|
||||
}
|
||||
|
||||
@@ -1244,7 +1241,7 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {1305.2710},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/pesando_2013_light_cone_quantization_and_interactions_of_a_new_closed_bosonic_string5.pdf;/home/riccardo/.local/share/zotero/storage/YUJ2G4EN/1305.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/pesando_2013_light_cone_quantization_and_interactions_of_a_new_closed_bosonic_string5.pdf},
|
||||
number = {1}
|
||||
}
|
||||
|
||||
@@ -1262,7 +1259,7 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {1407.4627},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/pesando_2014_canonical_quantization_of_a_string_describing_$n$_branes_at_angles.pdf;/home/riccardo/.local/share/zotero/storage/IXMFPPX9/1407.html}
|
||||
file = {/home/riccardo/.local/share/zotero/files/pesando_2014_canonical_quantization_of_a_string_describing_$n$_branes_at_angles.pdf}
|
||||
}
|
||||
|
||||
@article{Pesando:2014:CorrelatorsArbitraryUntwisted,
|
||||
@@ -1280,7 +1277,7 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {1401.6797},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/pesando_2014_correlators_of_arbitrary_untwisted_operators_and_excited_twist_operators_for_n.pdf;/home/riccardo/.local/share/zotero/files/pesando_2014_correlators_of_arbitrary_untwisted_operators_and_excited_twist_operators_for_n2.pdf},
|
||||
file = {/home/riccardo/.local/share/zotero/files/pesando_2014_correlators_of_arbitrary_untwisted_operators_and_excited_twist_operators_for_n2.pdf},
|
||||
primaryClass = {hep-th}
|
||||
}
|
||||
|
||||
@@ -1299,7 +1296,7 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {1512.07920},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/pesando_2016_towards_a_fully_stringy_computation_of_yukawa_couplings_on_non_factorized_tori.pdf;/home/riccardo/.local/share/zotero/files/pesando_2016_towards_a_fully_stringy_computation_of_yukawa_couplings_on_non-factorized_tori.pdf},
|
||||
file = {/home/riccardo/.local/share/zotero/files/pesando_2016_towards_a_fully_stringy_computation_of_yukawa_couplings_on_non_factorized_tori.pdf},
|
||||
primaryClass = {hep-th}
|
||||
}
|
||||
|
||||
@@ -1367,6 +1364,7 @@
|
||||
pages = {207--210},
|
||||
issn = {03702693},
|
||||
doi = {10.1016/0370-2693(81)90743-7},
|
||||
file = {/home/riccardo/.local/share/zotero/files/polyakov_1981_quantum_geometry_of_bosonic_strings2.pdf},
|
||||
keywords = {archived},
|
||||
langid = {english},
|
||||
number = {3}
|
||||
@@ -1374,7 +1372,7 @@
|
||||
|
||||
@article{Sciuto:1969:GeneralVertexFunction,
|
||||
title = {The General Vertex Function in Dual Resonance Models},
|
||||
author = {Sciuto, S.},
|
||||
author = {Sciuto, Stefano},
|
||||
date = {1969-09},
|
||||
journaltitle = {Lettere al Nuovo Cimento},
|
||||
shortjournal = {Lett. Nuovo Cimento},
|
||||
@@ -1389,7 +1387,7 @@
|
||||
|
||||
@article{Sheikh-Jabbari:1998:ClassificationDifferentBranes,
|
||||
title = {Classification of {{Different Branes}} at {{Angles}}},
|
||||
author = {Sheikh-Jabbari, M. M.},
|
||||
author = {Sheikh-Jabbari, Mohammad M.},
|
||||
date = {1998-02},
|
||||
journaltitle = {Physics Letters B},
|
||||
shortjournal = {Physics Letters B},
|
||||
@@ -1401,14 +1399,14 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {hep-th/9710121},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/sheikh-jabbari_1998_classification_of_different_branes_at_angles.pdf;/home/riccardo/.local/share/zotero/storage/8IXE34EP/9710121.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/sheikh-jabbari_1998_classification_of_different_branes_at_angles.pdf},
|
||||
number = {3-4}
|
||||
}
|
||||
|
||||
@article{Stieberger:1992:YukawaCouplingsBosonic,
|
||||
title = {Yukawa {{Couplings}} for {{Bosonic}} \${{Z}}\_{{N}}\$ {{Orbifolds}}: {{Their Moduli}} and {{Twisted Sector Dependence}}},
|
||||
title = {Yukawa {{Couplings}} for {{Bosonic ZN Orbifolds}}: {{Their Moduli}} and {{Twisted Sector Dependence}}},
|
||||
shorttitle = {Yukawa {{Couplings}} for {{Bosonic}} \${{Z}}\_{{N}}\$ {{Orbifolds}}},
|
||||
author = {Stieberger, S. and Jungnickel, D. and Lauer, J. and Spalinski, M.},
|
||||
author = {Stieberger, Stephan and Jungnickel, Dirk-U. and Lauer, Juergen and Spaliński, Michał},
|
||||
date = {1992-10-30},
|
||||
journaltitle = {Modern Physics Letters A},
|
||||
shortjournal = {Mod. Phys. Lett. A},
|
||||
@@ -1420,7 +1418,7 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {hep-th/9204037},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/stieberger_et_al_1992_yukawa_couplings_for_bosonic_$z_n$_orbifolds.pdf;/home/riccardo/.local/share/zotero/storage/7UDTMVHY/9204037.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/stieberger_et_al_1992_yukawa_couplings_for_bosonic_zn_orbifolds.pdf},
|
||||
number = {33}
|
||||
}
|
||||
|
||||
@@ -1468,13 +1466,13 @@
|
||||
archivePrefix = {arXiv},
|
||||
eprint = {gr-qc/9310026},
|
||||
eprinttype = {arxiv},
|
||||
file = {/home/riccardo/.local/share/zotero/files/hooft_2009_dimensional_reduction_in_quantum_gravity.pdf;/home/riccardo/.local/share/zotero/storage/XXKQV4D9/9310026.html},
|
||||
file = {/home/riccardo/.local/share/zotero/files/hooft_2009_dimensional_reduction_in_quantum_gravity.pdf},
|
||||
options = {useprefix=true}
|
||||
}
|
||||
|
||||
@article{Uranga:2003:ChiralFourdimensionalString,
|
||||
title = {Chiral Four-Dimensional String Compactifications with Intersecting {{D}}-Branes},
|
||||
author = {Uranga, Angel M},
|
||||
author = {Uranga, Angel M.},
|
||||
date = {2003-06-21},
|
||||
journaltitle = {Classical and Quantum Gravity},
|
||||
shortjournal = {Class. Quantum Grav.},
|
||||
|
||||
11
thesis.tex
11
thesis.tex
@@ -31,6 +31,11 @@
|
||||
\newcommand{\ap}{\ensuremath{\alpha'}}
|
||||
\newcommand{\cy}{\textsc{CY}\xspace}
|
||||
|
||||
%---- functions
|
||||
\newcommand{\hyp}[4]{\ensuremath{\mathrm{F}\left( #1,\, #2;\, #3;\, #4 \right)}}
|
||||
\newcommand{\poch}[2]{\ensuremath{\left( #1 \right)_{#2}}}
|
||||
\newcommand{\gfun}[1]{\ensuremath{\Gamma\left( #1 \right)}}
|
||||
|
||||
%---- derivatives
|
||||
\newcommand{\pd}{\ensuremath{\partial}}
|
||||
\newcommand{\bpd}{\ensuremath{\overline{\partial}}}
|
||||
@@ -113,12 +118,16 @@
|
||||
\input{sec/part3/introduction.tex}
|
||||
|
||||
%---- APPENDIX
|
||||
\cleardoubleplainpage{}
|
||||
\thesispart{Appendix}
|
||||
\appendix
|
||||
\section{The Isomorphism in Details}
|
||||
\label{sec:isomorphism}
|
||||
\input{sec/app/isomorphism.tex}
|
||||
|
||||
\section{The Parameters of the Hypergeometric Function}
|
||||
\label{sec:parameters}
|
||||
\input{sec/app/parameters.tex}
|
||||
|
||||
|
||||
%---- BIBLIOGRAPHY
|
||||
\cleardoubleplainpage{}
|
||||
|
||||
Reference in New Issue
Block a user