fix doxygen errors

diff --git a/include/deal.II/grid/manifold.h b/include/deal.II/grid/manifold.h
index a4651a243f370a81dee70a054973fe3648e0b0fe..f40a2e40e5aafc6f5aa78accbc7d81e2a79662e5 100644 (file)
--- a/include/deal.II/grid/manifold.h
+++ b/include/deal.II/grid/manifold.h
@@ -409,7 +409,7 @@ public:
    * @p weights.
    *
    * In its default implementation, this function simply calls get_new_point()
-   * on each row of @weights and appends those points to the output vector
+   * on each row of @p weights and appends those points to the output vector
    * @p new_points. However, this function is more efficient if multiple new
    * points need to be generated like in MappingQGeneric and the manifold does
    * expensive transformations between a chart space and the physical space,

diff --git a/include/deal.II/grid/tensor_product_manifold.h b/include/deal.II/grid/tensor_product_manifold.h
index 75bc3b8c6dc04a6b1c064a1ee1b8c1a6be4c2d4d..950e6be97e5edda3b46089db8838a9a22ff2fafb 100644 (file)
--- a/include/deal.II/grid/tensor_product_manifold.h
+++ b/include/deal.II/grid/tensor_product_manifold.h
@@ -30,7 +30,7 @@ DEAL_II_NAMESPACE_OPEN
  *
  * This manifold will combine the ChartManifolds @p A and @p B given in the
  * constructor to form a new ChartManifold by building the tensor product
- * $A\cross B$. The first @p spacedim_A dimensions in the real space and the
+ * $A\otimes B$. The first @p spacedim_A dimensions in the real space and the
  * first @p chartdim_A dimensions of the chart will be given by manifold @p A,
  * while the remaining coordinates are given by @p B. The manifold is to be
  * used by a <tt>Triangulation@<dim, space_dim_A+space_dim_B@></tt>.

diff --git a/include/deal.II/physics/elasticity/standard_tensors.h b/include/deal.II/physics/elasticity/standard_tensors.h
index e34f1784a1157eb00e21b4fcf70899ae46aac270..4c63fdef11e72bbbecb9aafad7a91cfef78cddfa 100644 (file)
--- a/include/deal.II/physics/elasticity/standard_tensors.h
+++ b/include/deal.II/physics/elasticity/standard_tensors.h
@@ -132,12 +132,12 @@ namespace Physics
        *  \mathcal{P} : \{ \bullet \}
        *  := \{ \bullet \} - \frac{1}{\textrm{dim}} \left[ \{ \bullet \} : \mathbf{I} \right]\mathbf{I}
        *   = \mathcal{P}^{T} : \{ \bullet \}
-       *   = \texttt{dev_P} \left( \{ \bullet \} \right)
+       *   = \texttt{dev\_P} \left( \{ \bullet \} \right)
        * @f]
        * and, therefore,
        * @f[
-       * \texttt{dev_P} \left( \{ \bullet \} \right) : \mathbf{I}
-       *   = \textrm{trace}(\texttt{dev_P} \left( \{ \bullet \} \right)) = 0 \, .
+       * \texttt{dev\_P} \left( \{ \bullet \} \right) : \mathbf{I}
+       *   = \textrm{trace}(\texttt{dev\_P} \left( \{ \bullet \} \right)) = 0 \, .
        * @f]
        *
        * This definition aligns with the fourth-order symmetric tensor that
@@ -173,11 +173,11 @@ namespace Physics
        * @f[
        *  \{ \bullet \} : \hat{\mathcal{P}}
        *    := J^{-2/\textrm{dim}} \left[ \{ \bullet \} - \frac{1}{\textrm{dim}}\left[\mathbf{C} : \{ \bullet \}\right] \mathbf{C}^{-1} \right]
-       *    = \texttt{Dev_P} \left( \{ \bullet \} \right) \, .
+       *    = \texttt{Dev\_P} \left( \{ \bullet \} \right) \, .
        * @f]
        * It can therefore be readily shown that
        * @f[
-       *  \texttt{Dev_P} \left( \{ \bullet \} \right) : \mathbf{C} = 0 \, .
+       *  \texttt{Dev\_P} \left( \{ \bullet \} \right) : \mathbf{C} = 0 \, .
        * @f]
        *
        * @note It may be observed that we have defined the tensor as the
@@ -214,7 +214,7 @@ namespace Physics
        * @f[
        *  \hat{\mathcal{P}}^{T} : \{ \bullet \}
        *    = J^{-2/\textrm{dim}} \left[ \{ \bullet \} - \frac{1}{\textrm{dim}} \left[\mathbf{C}^{-1} : \{ \bullet \}\right] \mathbf{C} \right]
-       *    = \texttt{Dev_P_T} \{ \bullet \}
+       *    = \texttt{Dev\_P\_T} \{ \bullet \}
        * @f]
        */
       template <typename Number>