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Wang Yu; Zhang Rongpei; Han Zijian; Wang Zhen, E-mail: rongpeizhang@163.com2019
AbstractAbstract
[en] It is well-known that reaction–diffusion systems are used to describe the pattern formation models. In this paper, we will investigate the pattern formation generated by the fractional reaction–diffusion systems. We first explore the mathematical mechanism of the pattern by applying the linear stability analysis for the fractional Gierer–Meinhardt system. Then, an efficient high-precision numerical scheme is used in the numerical simulation. The proposed method is based on an exponential time differencing Runge–Kutta method in temporal direction and a Fourier spectral method in spatial direction. This method has the advantages of high precision, better stability, and less storage. Numerical simulations show that the system control parameters and fractional order exponent have decisive influence on the generation of patterns. Our numerical results verify our theoretical results. (paper)
Source
Available from http://dx.doi.org/10.1088/1674-1056/28/5/050503; Country of input: International Atomic Energy Agency (IAEA)
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Journal Article
Journal
Chinese Physics. B; ISSN 1674-1056;
; v. 28(5); [7 p.]

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AbstractAbstract
[en] General numerical methods for ordinary differential equations (ODE) initial-value problems are surveyed, with emphasis on second-order ODE's. Issues include truncation and roundoff error, stability, and starting/stopping. For nonstiff systems, predictor-corrector Adams methods, with variable step and order, are best overall. (author)
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Workshop on orbital dynamics and applications to accelerators; Berkeley, CA (USA); 7-12 Mar 1985
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Journal Article
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Böckmann, C; Pornsawad, P, E-mail: bockmann@rz.uni-potsdam.de, E-mail: pornsawa@rz.uni-potsdam.de2008
AbstractAbstract
[en] We present a regularization method for solving nonlinear ill-posed problems by applying the family of Runge–Kutta methods to an initial value problem, in particular, to the asymptotical regularization method. We prove that the developed iterative regularization method converges to a solution under certain conditions and with a general stopping rule. Some particular iterative regularization methods are numerically implemented. Numerical results of the examples show that the developed Runge–Kutta-type regularization methods yield stable solutions and that particular implicit methods are very efficient in saving iteration steps
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S0266-5611(08)59127-1; Available from http://dx.doi.org/10.1088/0266-5611/24/2/025002; Country of input: International Atomic Energy Agency (IAEA)
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Journal Article
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Nirmala, V; Parimala, V; Rajarajeswari, P, E-mail: nirmalaucet@gmail.com, E-mail: parimalavp@gmail.com, E-mail: p.rajarajrswari29@gmail.com2018
AbstractAbstract
[en] The present study is aimed to discuss multiple numerical solutions to first order ordinary differential equation which is intuitionistic fuzzy in nature, under the concept of generalised differentiability. The first order intuitionistic fuzzy differential equation which has been taken for the present study, is changed into four systems of ordinary differential equations by the (α, β)-cut representation of an intuitionistic fuzzy set. After the transformation, each system contains two pair of equations; one is for membership function and the other for non-membership function. Then, the fourth order Runge-Kutta method is applied in each pair and the competence of the method over Euler method and Modified Euler method are shown by solving a real time problem. (paper)
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International Conference on Applied and Computational Mathematics; Tamilnadu (India); 10 Aug 2018; Available from http://dx.doi.org/10.1088/1742-6596/1139/1/012012; Country of input: International Atomic Energy Agency (IAEA)
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Journal Article
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Conference
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Journal of Physics. Conference Series (Online); ISSN 1742-6596;
; v. 1139(1); [8 p.]

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Tselios, Kostas; Simos, T.E., E-mail: tsimos@mail.ariadne-t.gr2007
AbstractAbstract
[en] In this Letter a new explicit fourth-order seven-stage Runge-Kutta method with a combination of minimal dispersion and dissipation error and maximal accuracy and stability limit along the imaginary axes, is developed. This method was produced by a general function that was constructed to satisfy all the above requirements and, from which, all the existing fourth-order six-stage RK methods can be produced. The new method is more efficient than the other optimized methods, for acoustic computations
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S0375-9601(06)01695-1; Copyright (c) 2006 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved.; Country of input: International Atomic Energy Agency (IAEA)
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Journal Article
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Loehner, Rainald, E-mail: rlohner@gmu.edu2004
AbstractAbstract
[en] A multistep advective predictor has been developed within the context of projection schemes for incompressible flows. The key idea is to integrate with schemes of different order the different regions of the domain. In regions where advection dominates, multistepping yields a considerable benefit. In those regions where viscosity dominates, the scheme reverts naturally to the original one-step scheme. Several examples show savings of the order of 1:3-1:10 as compared with standard projection schemes, even for transient problems. Given that these benefits can be achieved with a very modest change in existing codes, the proposed multistage advective predictor should be widely applicable
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S002199910300514X; Copyright (c) 2003 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved.; Country of input: International Atomic Energy Agency (IAEA)
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Journal Article
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AbstractAbstract
[en] For the measurement of the time profile and the contrast information of the ultrashort laser pulse, based on the third-order intensity correlation principle, using optical pulse replication, a measurement method is proposed. Theoretical analysis is made about the measurement method. The simulation was done with split-step Fourier and Runge-Kutta methods. By measuring the pulse with pieces of windows and piecing the windows together, the measuring range can be enlarged. Thus a high resolution and large window measurement is achieved. The pre-pulse and main pulse are separated into different windows to avoid the use of gradient attenuator, and provides high-contrast measurement capability. (authors)
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8 figs., 23 refs.; http://dx.doi.org/10.11884/HPLPB201426.051016
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Journal Article
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High Power Laser and Particle Beams; ISSN 1001-4322;
; v. 26(5); [6 p.]

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Nath, D.; Kalra, M.S.; Munshi, P., E-mail: dnath@iitk.ac.in, E-mail: msk@iitk.ac.in, E-mail: pmunshi@iitk.ac.in
Nuclear the next generation. 34th Annual Canadian Nuclear Society conference and 37th CNS/CNA student conference2013
Nuclear the next generation. 34th Annual Canadian Nuclear Society conference and 37th CNS/CNA student conference2013
AbstractAbstract
[en] A large number of numerical schemes have been developed for the integration of the hyperbolic system of partial differential equations (PDEs) arising in the magnetohydrodynamic (MHD) simulation of plasmas. These schemes can be based on either the combined space and time discretization such as the Lax-Wendroff type schemes, or one may perform first a separate space discretization leading to a semidiscretized set of ordinary differential equations (ODEs), which are then separately integrated in time. In this work, a comparative study of two schemes based on simultaneous discretization of space and time (Richtmyer two-step Lax-Wendroff scheme and MacCormack scheme) and one scheme based on centered-space semidiscretization followed by time integration by the fourth-order Runge-Kutta method, is presented. Particular attention is paid to the applicability of the linear stability criteria to the numerical integration of nonlinear MHD equations with geometry and field components of a linear θ-pinch. (author)
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Canadian Nuclear Society, Toronto, Ontario (Canada); 78 Megabytes; ISBN 978-1-926773-13-1;
; 2013; [12 p.]; 34. Annual Canadian Nuclear Society conference; Toronto, Ontario (Canada); 9-12 Jun 2013; 37. CNS/CNA student conference; Toronto, Ontario (Canada); 9-12 Jun 2013; Available from the Canadian Nuclear Society, Toronto, Ontario (Canada); 9 refs., 10 figs.

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Miscellaneous
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Alomari, A K; Noorani, M S M; Nazar, R, E-mail: abdomari2008@yahoo.com2010
AbstractAbstract
[en] In this paper, the numerical-analytical solution for the hyperchaotic Chen system is obtained via the multistage homotopy analysis method (MSHAM). An analytical form of the solution within each time interval is given, which is not possible using standard numerical methods. The numerical results obtained by the MSHAM and the classical fourth-order Runge-Kutta (RK4) method are in complete agreement. Moreover, the residual error for the MSHAM solution is given for each time interval.
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Available from http://dx.doi.org/10.1088/0031-8949/81/04/045005; Country of input: International Atomic Energy Agency (IAEA)
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Journal Article
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Physica Scripta (Online); ISSN 1402-4896;
; v. 81(4); [7 p.]

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Kavitha, L.; Sathishkumar, P.; Saravanan, M.; Gopi, D., E-mail: louiskavitha@yahoo.co.in
Abdus Salam International Centre for Theoretical Physics, Trieste (Italy)2010
Abdus Salam International Centre for Theoretical Physics, Trieste (Italy)2010
AbstractAbstract
[en] Switching the magnetization of a magnetic bit through flipping of soliton offers the possibility of developing a new innovative approach for data storage technologies. The spin dynamics of a site-dependent ferromagnet with antisymmetric Dzyaloshinskii-Moriya interaction is governed by a generalized inhomogeneous higher order nonlinear Schroedinger equation. We demonstrate the magnetization reversal through flipping of soliton in the ferromagnetic medium by solving the two coupled evolution equations for the velocity and amplitude of the soliton using the fourth order Runge-Kutta method numerically. We propose a new approach to induce the flipping behaviour of soliton in the presence of inhomogeneity by tuning the parameter associated with Dzyaloshinskii-Moriya interaction which causes the soliton to move with constant velocity and amplitude along the spin lattice. (author)
Primary Subject
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Jun 2010; 20 p; GRANT UGC F. NO.34-26/2008(SR); Also available at: http://users.ictp.it/~pub_off/preprints-sources/2010/IC2010041P.pdf; 33 refs, 7 figs
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