Lines Matching refs:B

57 - Basis (Dofs-to-Qpts) evaluator $\bm{B}$
60 …t and trial space differ, they get their own versions of $\bm{P}$, $\bm{\mathcal{E}}$ and $\bm{B}$.
158 Since the global operator $\bm{A}$ is just a series of variational restrictions with $\bm{B}$, $\bm…
163 …r portions of it) and evaluate the actions of $\bm{P}$, $\bm{\mathcal{E}}$ and $\bm{B}$ on-the-fly.
164 …uadrature points on *quad* and *hex* elements to perform the action of $\bm{B}$ without storing it…
173 …m{\mathcal{E}}$ and $\bm{B}$, the operator evaluation is decoupled  on their ranges, so $\bm{P}$, …
177 …B}$ and $\bm{D}$ clearly separate the MPI parallelism in the operator ($\bm{P}$) from the unstruct…
178 …athcal{E}}$, dense/structured linear algebra (tensor contractions) for $\bm{B}$ and parallel point…
191 …lly describes in the *frontend* the operators $\bm{\bm{\mathcal{E}}}$, $\bm{B}$, and $\bm{D}$ and …
197 …bCEED Operators, through backend implementations of $\bm{\bm{\mathcal{E}}}$, $\bm{B}$, and $\bm{D}$
215 - $\bm{B}$ is represented as variable of type {ref}`CeedBasis`.
217 - the overall operator $\bm{\mathcal{E}}^T \bm{B}^T \bm{D} \bm{B} \bm{\mathcal{E}}$ is represented …
232 Specific combination of $\bm{\bm{\mathcal{E}}}$, $\bm{B}$, $\bm{D}$, and input/output vectors corre…
288 The $\bm{B}$ operators for the mesh nodes, `basis_x`, and the unknown field, `basis_u`, are defined…
324 These operations, $\bm{\mathcal{E}}$, $\bm{B}$, and $\bm{D}$, are combined with a {ref}`CeedOperato…
326 separately with a matching field name, basis ($\bm{B}$), element restriction ($\bm{\mathcal{E}}$), …