2021
DOI: 10.1063/5.0044895
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Fast Ewald summation for electrostatic potentials with arbitrary periodicity

Abstract: A unified treatment for fast and spectrally accurate evaluation of electrostatic potentials subject to periodic boundary conditions in any or none of the three space dimensions is presented. Ewald decomposition is used to split the problem into a real space and a Fourier space part, and the FFT based Spectral Ewald (SE) method is used to accelerate the computation of the latter. A key component in the unified treatment is an FFT based solution technique for the free-space Poisson problem in three, two or one d… Show more

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Cited by 12 publications
(23 citation statements)
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“…It has a wide range of applications, including magnetic resonance imaging [17,10,21], computed tomography [12], optical coherence tomography [36], synthetic aperture radar [1], spectral interpolation between grids [20,Sec. 6] [14], and electrostatics in molecular dynamics [24,31]; for reviews see [20,16,3]. Given nonuniform points x j , j = 1, .…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
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“…It has a wide range of applications, including magnetic resonance imaging [17,10,21], computed tomography [12], optical coherence tomography [36], synthetic aperture radar [1], spectral interpolation between grids [20,Sec. 6] [14], and electrostatics in molecular dynamics [24,31]; for reviews see [20,16,3]. Given nonuniform points x j , j = 1, .…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
“…being simpler than either KB or PSWF, yet empirically having the same optimal rate and very similar errors. The ES kernel has since been used to accelerate Spectral Ewald codes for periodic electrostatic sums [31]. Its Fourier transform φES,β (ξ) is not known analytically, yet is easily evaluated by quadrature [3,Sec.…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
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“…The method was extended to the free-space case for all three kernels by [23]. The current paper serves to complete this development, much in the same way as was recently done for electrostatics by [24], by adding the missing pieces (singly periodic case for all three kernels, and doubly periodic case for the stresslet and rotlet), and unifying all periodic cases within a single framework. This opens up the possibility to perform efficient simulations of three-dimensional Stokes flow with arbitrary periodicity (D = 3, 2, 1, 0), using boundary integral and potential methods.…”
Section: Introductionmentioning
confidence: 90%
“…Thus, the FMM will typically be faster for highly nonuniform point distributions (especially in free space), while the SE method may be faster for uniform distributions, as shown e.g. by [23,24]. Yet another alternative method is found in [49], in which the long-range interaction is represented by auxiliary sources.…”
Section: Introductionmentioning
confidence: 99%