2018
DOI: 10.1016/j.cam.2018.02.031
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Conditional full stability of positivity-preserving finite difference scheme for diffusion–advection-reaction models

Abstract: The matter of the stability for multidimensional diffusion-advection-reaction problems treated with the semi-discretization method is remaining challenge because when all the stepsizes tend simultaneously to zero the involved size of the problem grows without bounds. Solution of such problems is constructed by starting with a semi-discretization approach followed by a full discretization using exponential time differencing and matrix quadrature rules. Analysis of the time variation of the numerical solution wi… Show more

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Cited by 6 publications
(7 citation statements)
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“…For better approximation the spatial computational domain is chosen as false[5,0.1em5false]×false[5,0.1em5false]$$ \left[-5,5\right]\times \left[-5,5\right] $$ with 150×150$$ 150\times 150 $$ nodes. In Table 3, we compare the results for false(S1,S2false)=false(100,0.1em100false)$$ \left({S}_1,{S}_2\right)=\left(100,100\right) $$ with ones computed by the FD method (with mixed derivative removing transformation) proposed in Company et al [32] and by the high‐order computational (HOC) method of [26]. The option price for other assets' prices are reported in Table 4.…”
Section: Numerical Resultsmentioning
confidence: 99%
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“…For better approximation the spatial computational domain is chosen as false[5,0.1em5false]×false[5,0.1em5false]$$ \left[-5,5\right]\times \left[-5,5\right] $$ with 150×150$$ 150\times 150 $$ nodes. In Table 3, we compare the results for false(S1,S2false)=false(100,0.1em100false)$$ \left({S}_1,{S}_2\right)=\left(100,100\right) $$ with ones computed by the FD method (with mixed derivative removing transformation) proposed in Company et al [32] and by the high‐order computational (HOC) method of [26]. The option price for other assets' prices are reported in Table 4.…”
Section: Numerical Resultsmentioning
confidence: 99%
“…Following the ideas of Company et al [32], we consider the truncated domain normalΩ=[]y1min,0.1emy1max××[]yMmin,0.1emyMmax$$ \Omega =\left[{y}_{1_{\mathrm{min}}},{y}_{1_{\mathrm{max}}}\right]\times \dots \times \left[{y}_{M_{\mathrm{min}}},{y}_{M_{\mathrm{max}}}\right] $$ and introduce the uniform in each dimension mesh yij=yimin+jhi,0.30emhi=1Nifalse(yimaxyiminfalse),2.56804ptj=0,,Ni,2.56804pti=1,,M.$$ {y}_i^j={y}_{i_{\mathrm{min}}}+j{h}_i,\kern0.30em {h}_i=\frac{1}{N_i}\left({y}_{i_{\mathrm{max}}}-{y}_{i_{\mathrm{min}}}\right),j=0,\dots, {N}_i,i=1,\dots, M. $$ …”
Section: Numerical Solutionmentioning
confidence: 99%
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“…This method is easy to implement but computationally expensive and time-consuming to obtain the solution not in one fixed point but in some domain. Therefore, in the present study, the method of exponential time differencing proposed in [14] is employed after applying the mixed derivative terms removing transformation [13] and the semi-discretization technique [16].…”
Section: Numerical Solutionmentioning
confidence: 99%