Journal Article10.1145/362041.362216
Remark on algorithm 406
1
TL;DR: This investigation was part of the research program of the "Stichting voor Fundamental Onderzoek der Materie (F.O.M.)," which is financially supported by the "Nederlandse Organisatie voor Zuiver Wetenschappelijk Onderzosek (Z.W.O.)".
read more
Abstract: Submittal of an algorithm for consideration for publication in Communications of the ACM implies unrestricted use of the algorithm within a computer is permissible. General permission to republish, but not for profit, all or part of this material is granted provided that ACM's copyright notice is given and that reference is made to the publication, to its date of issue, and to the fact that reprinting privileges were granted by permission of the Association for Computing Machinery. The procedure Coulomb can be used very weU to generate the Coulomb wave functions FL and GL and their derivatives, needed in elastic scattering calculations in nuclear physics. When the procedure is used many times for many values of rho and eta, it is not only very useful but also necessary to have in each instance an indication about the accuracy of the results. It is obvious to use the Wronskian relations FL'GL-FLGL' ~ l for the purpose of checking the results, as Fr6berg [1] states after formula (3.4). However, one has to be very careful in using these relations. The most significant check is given later on, but first it is shown what can go wrong. K61big pointed out already in the certification that Lutz and Karvelis [2] failed to notice discrepancies exceeding 100 units in the sixth significant digit in their tables although they state \"when all the functions are generated we test to see how closely the Wron-skian relation FL'GL-FLGL' = 1 is obeyed.\" The way Lutz and Karvelis generate the functions goes as follows. First they calculate Go and Go'; then they use recurrence relations to get GL and GL' for L > 0; and lastly them use backward recurrence This investigation was part of the research program of the \"Stichting voor Fundamental Onderzoek der Materie (F.O.M.),\" which is financially supported by the \"Nederlandse Organisatie voor Zuiver Wetenschappelijk Onderzoek (Z.W.O.)\". relations together with the relation FoG~-GoF1 = (n 2 + I)-~ to get FL and FL' for all L. This last relation is in fact a di:::rent form of the Wronskian relation, see e.g. Fr6berg [1] formula (3.5). The use of the Wronskian relations to check the results now gives information only about the stability in the use of the recurrence relations, not about the accuracy of the Coulomb wave functions. As an independent check on the function values, the following procedure can be used. It is easy to …
read more
Chat with Paper
AI Agents for this Paper
Find similar papers on Google Scholar, PubMed and Arxiv
Write a critical review of this paper
Analyze citations of this paper to find unaddressed research gaps
Citations
A PC-based 3D imaging system: algorithms, software, and hardware considerations.
TL;DR: It is demonstrated that with an appropriate choice of approaches and a proper design of algorithms and software, it is possible to develop a low-cost 3D imaging system that can provide a level of performance sufficient to meet the daily case load in an individual or even group-practice situation.
42
References
Numerical calculation of Coulomb wave functions for repulsive Coulomb fields
H.F. Lutz,M.D. Karvelis +1 more
TL;DR: In this article, a table of Coulomb functions for selected values of the Coulomb parameter η over the range of 1 to 25 is presented, and a description of the numerical calculation of these functions used in scattering and reaction calculations is given.
27
Numerical Treatment of Coulomb Wave Functions
TL;DR: In this paper, a number of methods suitable for computation of Coulomb wave functions with high accuracy are collected, most of them previously well known, and it is shown that the regions where these methods can be used, together cover all positive values of $\ensuremath{\rho}$ and $\enuremath{eta}$ in the case $L=0.