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[Licence| Download | New Version Template] aeti_v2_0.tar.gz(508 Kbytes) | ||
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Manuscript Title: New version of hex-ecs, the B-spline implementation of
exterior complex scaling method for solution of electron-hydrogen scattering | ||

Authors: Jakub Benda, Karel Houfek | ||

Program title: hex-ecs | ||

Catalogue identifier: AETI_v2_0Distribution format: tar.gz | ||

Journal reference: Comput. Phys. Commun. 204(2016)216 | ||

Programming language: C++11. | ||

Computer: Any recent CPU, preferably 64-bit. Computationally intensive parts
can be run on GPU (tested on AMD Tahiti and NVidia TitanX models). | ||

Operating system: Tested on Windows 10 and various Linux distributions. | ||

RAM: Depends on the problem solved and particular setup; KPA test run uses
apx. 300 MiB. | ||

Keywords: Electron-hydrogen scattering, Exterior complex scaling. | ||

Classification: 2.4. | ||

External routines: GSL [1], UMFPACK [2], BLAS and LAPACK (ideally
threaded OpenBLAS [3]). | ||

Does the new version supersede the previous version?: Yes | ||

Nature of problem:Solution of the two-particle Schrödinger equation in central field. | ||

Solution method:The two-electron states are expanded into angular momentum eigenstates, which gives rise to the coupled bi-radial equations. The bi-radially dependent solution is then represented in a B-spline product basis, which transforms the set of equations into a large matrix equation in this basis. The boundary condition is of Dirichlet type, thanks to the use of the exterior complex scaling method, which extends the coordinates into the complex plane. The matrix equation is then solved by preconditioned conjugated orthogonal conjugate gradient method (PCOCG) [4]. | ||

Reasons for new version:The original program has been updated to achieve better performance. Also, some external dependencies have been removed (HDF5, FFTW3), which simplifies deployment. | ||

Summary of revisions:We implemented a new preconditioner introduced in [5], both for general CPU and also for an arbitrary OpenCL device (e.g. GPU) conforming to the OpenCL 2.0 specification. Furthermore, many other minor improvements have been made, particularly with the intention of reducing the memory requirements. With appropriate switches the program now doesn't precompute the used matrices and only calculates their elements on the fly. This is aided also by the vectorized B-spline evaluation function, which can now make use of AVX instructions when a single B-spline is being evaluated at several points. The accompanying tools hex-db and hex-dwba [6] have been also updated to use the shared code base. | ||

Running time:KPA test run - apx. 2 minutes on Intel i7-4790K (4 threads) | ||

References: | ||

[1] | Galassi M. et al, GNU Scientific Library: Reference Manual, Network Theory Ltd., 2003. | |

[2] | Davis T. A., Algorithm 832: UMFPACK, an unsymmetric-pattern multifrontal method, ACM Trans. Math. Softw. 30 (2004) 196-199. | |

[3] | Xianyi Z. et al, Model-driven Level 3 BLAS Performance Optimization on Loongson 3A Processor, 2012 IEEE 18th International Conference on Parallel and Distributed Systems (ICPADS), 17-19 Dec. 2012. | |

[4] | van der Vorst H. A., Melissen J. B. M., A Petrov-Galerkin type method for solving Ax = b, where A is symmetric complex, IEEE Trans. Magn. 26 (1990) 706-708. | |

[5] | Bar-On at al, Parallel solution of the multidimensional Helmholtz / Schroedinger equation using high order methods, Appl. Num. Math. 33 (2000) 95-104. | |

[6] | Benda J., Houfek K., Collisions of electrons with hydrogen atoms I. Package outline and high energy code, Comput. Phys. Commun. 185 (2014) 2893-2902. |

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