"자코비 다항식"의 두 판 사이의 차이

수학노트
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16번째 줄: 16번째 줄:
  
 
* [[초기하급수(Hypergeometric series)]]를 통해 정의된다<br><math>P_n^{(\alpha,\beta)}(z)=\frac{(\alpha+1)_n}{n!} \,_2F_1\left(-n,1+\alpha+\beta+n;\alpha+1;\frac{1-z}{2}\right)</math><br>
 
* [[초기하급수(Hypergeometric series)]]를 통해 정의된다<br><math>P_n^{(\alpha,\beta)}(z)=\frac{(\alpha+1)_n}{n!} \,_2F_1\left(-n,1+\alpha+\beta+n;\alpha+1;\frac{1-z}{2}\right)</math><br>
*  다항식표현<br><math>P_n^{(\alpha,\beta)} (z) =  \frac{\Gamma (\alpha+n+1)}{n!\Gamma (\alpha+\beta+n+1)} \sum_{m=0}^n {n\choose m} \frac{\Gamma (\alpha + \beta + n + m + 1)}{\Gamma (\alpha + m + 1)} \left(\frac{z-1}{2}\right)^m</math><br>  <br>
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*  다항식표현<br><math>P_n^{(\alpha,\beta)} (z) =  \frac{\Gamma (\alpha+n+1)}{n!\Gamma (\alpha+\beta+n+1)} \sum_{m=0}^n {n\choose m} \frac{\Gamma (\alpha + \beta + n + m + 1)}{\Gamma (\alpha + m + 1)} \left(\frac{z-1}{2}\right)^m</math><br>
  
 
 
 
 
 
<h5>직교성</h5>
 
 
*  weight함수와 구간<br><math>w(x) = (1-x)^{\alpha} (1+x)^{\beta}</math><br><math>[-1,1]</math><br>
 
* <math>m\neq n</math> 일 때<br><math>\int_{-1}^1 (1-x)^{\alpha} (1+x)^{\beta}  P_m^{(\alpha,\beta)} (x)P_n^{(\alpha,\beta)} (x) \; dx= 0</math><br>
 
* <math>m=n</math> 일 때<br><math>\int_{-1}^1 (1-x)^{\alpha} (1+x)^{\beta}  P_m^{(\alpha,\beta)} (x)P_n^{(\alpha,\beta)} (x) \; dx= \frac{2^{\alpha+\beta+1}}{2n+\alpha+\beta+1} \frac{\Gamma(n+\alpha+1)\Gamma(n+\beta+1)}{\Gamma(n+\alpha+\beta+1)n!} \delta_{nm}</math><br>
 
  
 
 
 
 
40번째 줄: 34번째 줄:
 
<h5>미분방정식</h5>
 
<h5>미분방정식</h5>
  
자코비 다항식은 다음을 만족시킨다<br><math>(1-x^2)y'' + ( \beta-\alpha - (\alpha + \beta + 2)x )y'+ n(n+\alpha+\beta+1) y = 0</math><br>
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자 코비 다항식은 다음을 만족시킨다<br><math>(1-x^2)y'' + ( \beta-\alpha - (\alpha + \beta + 2)x )y'+ n(n+\alpha+\beta+1) y = 0</math><br>
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<h5>직교성</h5>
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 +
*  weight함수와 구간<br><math>w(x) = (1-x)^{\alpha} (1+x)^{\beta}</math><br><math>[-1,1]</math><br>
 +
* <math>m\neq n</math> 일 때<br><math>\int_{-1}^1 (1-x)^{\alpha} (1+x)^{\beta}  P_m^{(\alpha,\beta)} (x)P_n^{(\alpha,\beta)} (x) \; dx= 0</math><br>
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* <math>m=n</math> 일 때<br><math>\int_{-1}^1 (1-x)^{\alpha} (1+x)^{\beta}  P_m^{(\alpha,\beta)} (x)P_n^{(\alpha,\beta)} (x) \; dx= \frac{2^{\alpha+\beta+1}}{2n+\alpha+\beta+1} \frac{\Gamma(n+\alpha+1)\Gamma(n+\beta+1)}{\Gamma(n+\alpha+\beta+1)n!} \delta_{nm}</math><br> 예<br><math>\int_{-1}^1 (1-x)^{\alpha} (1+x)^{\beta}  P_m^{(\alpha,\beta)} (x)P_n^{(\alpha,\beta)} (x) \; dx= \frac{2^{\alpha+\beta+1}}{2n+\alpha+\beta+1} \frac{\Gamma(n+\alpha+1)\Gamma(n+\beta+1)}{\Gamma(n+\alpha+\beta+1)n!} \delta_{nm}</math><br>
  
 
 
 
 
48번째 줄: 50번째 줄:
 
<h5>목록</h5>
 
<h5>목록</h5>
  
P_0(z)=1<br> P_1(z)=1/2 (\[Alpha]-\[Beta]+z (2+\[Alpha]+\[Beta]))<br> P_2(z)=1/2 (1+\[Alpha]) (2+\[Alpha])+1/2 (-1+z) (2+\[Alpha]) (3+\[Alpha]+\[Beta])+1/8 (-1+z)^2 (3+\[Alpha]+\[Beta]) (4+\[Alpha]+\[Beta])<br> P_3(z)=1/6 (1+\[Alpha]) (2+\[Alpha]) (3+\[Alpha])+1/4 (-1+z) (2+\[Alpha]) (3+\[Alpha]) (4+\[Alpha]+\[Beta])+1/8 (-1+z)^2 (3+\[Alpha]) (4+\[Alpha]+\[Beta]) (5+\[Alpha]+\[Beta])+1/48 (-1+z)^3 (4+\[Alpha]+\[Beta]) (5+\[Alpha]+\[Beta]) (6+\[Alpha]+\[Beta])<br> P_4(z)=1/24 (1+\[Alpha]) (2+\[Alpha]) (3+\[Alpha]) (4+\[Alpha])+1/12 (-1+z) (2+\[Alpha]) (3+\[Alpha]) (4+\[Alpha]) (5+\[Alpha]+\[Beta])+1/16 (-1+z)^2 (3+\[Alpha]) (4+\[Alpha]) (5+\[Alpha]+\[Beta]) (6+\[Alpha]+\[Beta])+1/48 (-1+z)^3 (4+\[Alpha]) (5+\[Alpha]+\[Beta]) (6+\[Alpha]+\[Beta]) (7+\[Alpha]+\[Beta])+1/384 (-1+z)^4 (5+\[Alpha]+\[Beta]) (6+\[Alpha]+\[Beta]) (7+\[Alpha]+\[Beta]) (8+\[Alpha]+\[Beta])
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P_0(z)=1<br> P_1(z)=1/2 (a-b+(2+a+b) z)<br> P_2(z)=1/2 (1+a) (2+a)+1/2 (2+a) (3+a+b) (-1+z)+1/8 (3+a+b) (4+a+b) (-1+z)^2<br> P_3(z)=1/6 (1+a) (2+a) (3+a)+1/4 (2+a) (3+a) (4+a+b) (-1+z)+1/8 (3+a) (4+a+b) (5+a+b) (-1+z)^2+1/48 (4+a+b) (5+a+b) (6+a+b) (-1+z)^3<br> P_4(z)=1/24 (1+a) (2+a) (3+a) (4+a)+1/12 (2+a) (3+a) (4+a) (5+a+b) (-1+z)+1/16 (3+a) (4+a) (5+a+b) (6+a+b) (-1+z)^2+1/48 (4+a) (5+a+b) (6+a+b) (7+a+b) (-1+z)^3+1/384 (5+a+b) (6+a+b) (7+a+b) (8+a+b) (-1+z)^4
  
 
 
 
 

2010년 5월 2일 (일) 09:26 판

이 항목의 스프링노트 원문주소

 

 

개요
  • 직교다항식

 

 

정의
  • 초기하급수(Hypergeometric series)를 통해 정의된다
    \(P_n^{(\alpha,\beta)}(z)=\frac{(\alpha+1)_n}{n!} \,_2F_1\left(-n,1+\alpha+\beta+n;\alpha+1;\frac{1-z}{2}\right)\)
  • 다항식표현
    \(P_n^{(\alpha,\beta)} (z) = \frac{\Gamma (\alpha+n+1)}{n!\Gamma (\alpha+\beta+n+1)} \sum_{m=0}^n {n\choose m} \frac{\Gamma (\alpha + \beta + n + m + 1)}{\Gamma (\alpha + m + 1)} \left(\frac{z-1}{2}\right)^m\)

 

 

 

3항 점화식

 

 

 

미분방정식
  • 자 코비 다항식은 다음을 만족시킨다
    \((1-x^2)y'' + ( \beta-\alpha - (\alpha + \beta + 2)x )y'+ n(n+\alpha+\beta+1) y = 0\)

 

 

직교성
  • weight함수와 구간
    \(w(x) = (1-x)^{\alpha} (1+x)^{\beta}\)
    \([-1,1]\)
  • \(m\neq n\) 일 때
    \(\int_{-1}^1 (1-x)^{\alpha} (1+x)^{\beta} P_m^{(\alpha,\beta)} (x)P_n^{(\alpha,\beta)} (x) \; dx= 0\)
  • \(m=n\) 일 때
    \(\int_{-1}^1 (1-x)^{\alpha} (1+x)^{\beta} P_m^{(\alpha,\beta)} (x)P_n^{(\alpha,\beta)} (x) \; dx= \frac{2^{\alpha+\beta+1}}{2n+\alpha+\beta+1} \frac{\Gamma(n+\alpha+1)\Gamma(n+\beta+1)}{\Gamma(n+\alpha+\beta+1)n!} \delta_{nm}\)

    \(\int_{-1}^1 (1-x)^{\alpha} (1+x)^{\beta} P_m^{(\alpha,\beta)} (x)P_n^{(\alpha,\beta)} (x) \; dx= \frac{2^{\alpha+\beta+1}}{2n+\alpha+\beta+1} \frac{\Gamma(n+\alpha+1)\Gamma(n+\beta+1)}{\Gamma(n+\alpha+\beta+1)n!} \delta_{nm}\)

 

목록

P_0(z)=1
P_1(z)=1/2 (a-b+(2+a+b) z)
P_2(z)=1/2 (1+a) (2+a)+1/2 (2+a) (3+a+b) (-1+z)+1/8 (3+a+b) (4+a+b) (-1+z)^2
P_3(z)=1/6 (1+a) (2+a) (3+a)+1/4 (2+a) (3+a) (4+a+b) (-1+z)+1/8 (3+a) (4+a+b) (5+a+b) (-1+z)^2+1/48 (4+a+b) (5+a+b) (6+a+b) (-1+z)^3
P_4(z)=1/24 (1+a) (2+a) (3+a) (4+a)+1/12 (2+a) (3+a) (4+a) (5+a+b) (-1+z)+1/16 (3+a) (4+a) (5+a+b) (6+a+b) (-1+z)^2+1/48 (4+a) (5+a+b) (6+a+b) (7+a+b) (-1+z)^3+1/384 (5+a+b) (6+a+b) (7+a+b) (8+a+b) (-1+z)^4

 

 

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