D01AHF | One-dimensional quadrature, adaptive, finite interval, strategy due to Patterson, suitable for well-behaved integrands |

D01AJF | One-dimensional quadrature, adaptive, finite interval, strategy due to Piessens and de Doncker, allowing for badly behaved integrands |

D01AKF | One-dimensional quadrature, adaptive, finite interval, method suitable for oscillating functions |

D01ALF | One-dimensional quadrature, adaptive, finite interval, allowing for singularities at user-specified break-points |

D01ANF | One-dimensional quadrature, adaptive, finite interval, weight function $\mathrm{cos}\left(\omega x\right)$ or $\mathrm{sin}\left(\omega x\right)$ |

D01APF | One-dimensional quadrature, adaptive, finite interval, weight function with end-point singularities of algebraico-logarithmic type |

D01AQF | One-dimensional quadrature, adaptive, finite interval, weight function $1/\left(x-c\right)$, Cauchy principal value (Hilbert transform) |

D01ARF | One-dimensional quadrature, non-adaptive, finite interval with provision for indefinite integrals |

D01ATF | One-dimensional quadrature, adaptive, finite interval, variant of D01AJF efficient on vector machines |

D01AUF | One-dimensional quadrature, adaptive, finite interval, variant of D01AKF efficient on vector machines |

D01BDF | One-dimensional quadrature, non-adaptive, finite interval |

D01DAF | Two-dimensional quadrature, finite region |

D01RAF | One-dimensional quadrature, adaptive, finite interval, multiple integrands, vectorized abscissae, reverse communication |

D01RGF | One-dimensional quadrature, adaptive, finite interval, strategy due to Gonnet, allowing for badly behaved integrands |

D02GAF | Ordinary differential equations, boundary value problem, finite difference technique with deferred correction, simple nonlinear problem |

D02GBF | Ordinary differential equations, boundary value problem, finite difference technique with deferred correction, general linear problem |

D02KAF | Second-order Sturm–Liouville problem, regular system, finite range, eigenvalue only |

D02KDF | Second-order Sturm–Liouville problem, regular/singular system, finite/infinite range, eigenvalue only, user-specified break-points |

D02KEF | Second-order Sturm–Liouville problem, regular/singular system, finite/infinite range, eigenvalue and eigenfunction, user-specified break-points |

D02RAF | Ordinary differential equations, general nonlinear boundary value problem, finite difference technique with deferred correction, continuation facility |

D03EBF | Elliptic PDE, solution of finite difference equations by SIP, five-point two-dimensional molecule, iterate to convergence |

D03ECF | Elliptic PDE, solution of finite difference equations by SIP for seven-point three-dimensional molecule, iterate to convergence |

D03EDF | Elliptic PDE, solution of finite difference equations by a multigrid technique |

D03NCF | Finite difference solution of the Black–Scholes equations |

D03PCF | General system of parabolic PDEs, method of lines, finite differences, one space variable |

D03PHF | General system of parabolic PDEs, coupled DAEs, method of lines, finite differences, one space variable |

D03PPF | General system of parabolic PDEs, coupled DAEs, method of lines, finite differences, remeshing, one space variable |

D03RAF | General system of second-order PDEs, method of lines, finite differences, remeshing, two space variables, rectangular region |

D03RBF | General system of second-order PDEs, method of lines, finite differences, remeshing, two space variables, rectilinear region |

D03UAF | Elliptic PDE, solution of finite difference equations by SIP, five-point two-dimensional molecule, one iteration |

D03UBF | Elliptic PDE, solution of finite difference equations by SIP, seven-point three-dimensional molecule, one iteration |

D06CBF | Generates a sparsity pattern of a Finite Element matrix associated with a given mesh |

© The Numerical Algorithms Group Ltd, Oxford UK. 2013