opalt.asciidoc

@@ -203,9 +203,9 @@ to the entrance of that element.
 Denoting with latexmath:[i] a beam line element, one can compute
 latexmath:[\mathbf{v}_i] and latexmath:[\mathcal{W}_i] by the
 recurrence relations 
+
 [latexmath]
 ++++
-\label{eq:surv}
 \mathbf{v}_i = \mathcal{W}_{i-1}\mathbf{r}_i + \mathbf{v}_{i-1}, \qquad
 \mathcal{W}_i = \mathcal{W}_{i-1}\mathcal{S}_i,
 ++++
@@ -896,12 +896,15 @@ b_z (z) = B_z (-z) \qquad B_x (z) = - B_x (-z) \qquad B_s (z) = - B_s (-z)
 ++++
 
 The most general form of the expansion is
+
+.Equation 1
+[#eq-01]
 [latexmath]
 ++++
 \begin{aligned}
-         B_z & = \sum_{i,k=0}^{\infty} b_{i,k} x^i z^{2k} \label{eq:01} \\
-         B_x & = z \sum_{i,k=0}^{\infty} a_{i,k} x^i z^{2k} \label{eq:02}\\
-         B_s & = z \sum_{i,k=0}^{\infty} c_{i,k} x^i z^{2k} \label{eq:03}
+         B_z & = \sum_{i,k=0}^{\infty} b_{i,k} x^i z^{2k}  \\
+         B_x & = z \sum_{i,k=0}^{\infty} a_{i,k} x^i z^{2k} \\
+         B_s & = z \sum_{i,k=0}^{\infty} c_{i,k} x^i z^{2k}
     \end{aligned}
 ++++
 
@@ -924,8 +927,8 @@ yield
         \end{aligned}
 ++++
 
-The substitution of ([eq:01]), ([eq:02]) and
-([eq:03]) into Maxwell’s equations allows for the derivation of
+The substitution of (<<eq-01, 1>>)
+into Maxwell’s equations allows for the derivation of
 recursion relations. ([eq:23]) gives
 
 [latexmath]
@@ -1007,7 +1010,7 @@ _(variable radius of curvature)_
 The difference between this case and the above is that
 latexmath:[\rho] is now a function of latexmath:[s],
 latexmath:[\rho(s)]. We can obtain the same result starting with the
-same functional forms for the field ([eq:01]), ([eq:02]), ([eq:03]). The
+same functional forms for the field (<<eq-01, 1>>). The
 result of the previous section also holds in this case since no
 derivative latexmath:[\frac{\partial}{\partial s}] is applied to the
 scale factor latexmath:[h_s]. If the radius of curvature is set to be