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arXiv 2103.11841math.NAcs.NA
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具有弱端点奇异性的切比雪夫多项式逼近的渐近系数和误差:不同基的影响

Asymptotic Coefficients and Errors for Chebyshev Polynomial Approximations with Weak Endpoint Singularities: Effects of Different Bases

Xiaolong Zhang, John P. Boyd

摘要:

当通过谱方法求解微分方程时,通常方便的是从具有系数$a_{n}$的切比雪夫多项式$T_{n}(x)$转移到包含边界条件的修改的基函数。对于齐次Dirichlet边界条件$u(\pm 1)=0$,流行的选择包括“切比雪夫差分基”,$ς_{n}(x) \equiv T_{n+2}(x) - T_{n}(x)$,其系数在这里表示为$b_{n}$,以及“二次因子基函数”$\varrho_{n}(x) \equiv (1-x^{2}) T_{n}(x)$,其系数为$c_{n}$。如果$u(x)$在边界处是弱奇异的,则对于某个正常数$κ$,$a_{n}$将与$\mathcal{O}(A(n)/n^κ)$成比例地减小,其中$A(n)$是对数或常数。我们证明了切比雪夫差分系数$b_{n}$下降更慢的$1/n$的一个因素,而二次因子系数$c_{n}$下降更慢仍然作为$\mathcal{O}(A(n)/n^{κ-2})$。在$n=N$阶截断的无约束Chebyshev级数的误差在内部为$\mathcal{O}(|A(N)|/N^κ)$,但在靠近每个端点的窄边界层中,其误差要差一个$N$的幂。尽管具有几乎相同的误差\emph{norms},切比雪夫基的误差集中在两个端点附近的边界层中,而在二次因子和差分基组中的误差在$x$的整个区间上几乎是均匀振荡的。同时,对于Chebyshev多项式和二次因子基,其导数在端点的值为$\mathcal{O}(N^{2})$,而对于差基,其导数在端点的值仅为$\mathcal{O}(N)$.

英文摘要:

When solving differential equations by a spectral method, it is often convenient to shift from Chebyshev polynomials $T_{n}(x)$ with coefficients $a_{n}$ to modified basis functions that incorporate the boundary conditions. For homogeneous Dirichlet boundary conditions, $u(\pm 1)=0$, popular choices include the ``Chebyshev difference basis", $ς_{n}(x) \equiv T_{n+2}(x) - T_{n}(x)$ with coefficients here denoted $b_{n}$ and the ``quadratic-factor basis functions" $\varrho_{n}(x) \equiv (1-x^{2}) T_{n}(x)$ with coefficients $c_{n}$. If $u(x)$ is weakly singular at the boundaries, then $a_{n}$ will decrease proportionally to $\mathcal{O}(A(n)/n^κ)$ for some positive constant $κ$, where the $A(n)$ is a logarithm or a constant. We prove that the Chebyshev difference coefficients $b_{n}$ decrease more slowly by a factor of $1/n$ while the quadratic-factor coefficients $c_{n}$ decrease more slowly still as $\mathcal{O}(A(n)/n^{κ-2})$. The error for the unconstrained Chebyshev series, truncated at degree $n=N$, is $\mathcal{O}(|A(N)|/N^κ)$ in the interior, but is worse by one power of $N$ in narrow boundary layers near each of the endpoints. Despite having nearly identical error \emph{norms}, the error in the Chebyshev basis is concentrated in boundary layers near both endpoints, whereas the error in the quadratic-factor and difference basis sets is nearly uniform oscillations over the entire interval in $x$. Meanwhile, for Chebyshev polynomials and the quadratic-factor basis, the value of the derivatives at the endpoints is $\mathcal{O}(N^{2})$, but only $\mathcal{O}(N)$ for the difference basis.

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