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In [[linear algebra]], a '''Vandermonde matrix''', named after [[Alexandre-Théophile Vandermonde]], is a [[matrix (math)|matrix]] with the terms of a [[geometric progression]] in each row, i.e., an ''m'' × ''n'' matrix | |||
:<math>V=\begin{bmatrix} | |||
1 & \alpha_1 & \alpha_1^2 & \dots & \alpha_1^{n-1}\\ | |||
1 & \alpha_2 & \alpha_2^2 & \dots & \alpha_2^{n-1}\\ | |||
1 & \alpha_3 & \alpha_3^2 & \dots & \alpha_3^{n-1}\\ | |||
\vdots & \vdots & \vdots & \ddots &\vdots \\ | |||
1 & \alpha_m & \alpha_m^2 & \dots & \alpha_m^{n-1} | |||
\end{bmatrix}</math> | |||
or | |||
:<math>V_{i,j} = \alpha_i^{j-1} \, </math> | |||
for all indices ''i'' and ''j''.<ref>Roger A. Horn and Charles R. Johnson (1991), ''Topics in matrix analysis,'' Cambridge University Press. ''See Section 6.1''</ref> (Some authors use the [[transpose]] of the above matrix.) | |||
= | The [[determinant]] of a square Vandermonde matrix (where ''m'' = ''n'') can be expressed as: | ||
:<math>\det(V) = \prod_{1\le i<j\le n} (\alpha_j-\alpha_i). </math> | |||
This is called the '''Vandermonde determinant''' or '''[[Vandermonde polynomial]].''' If all the numbers <math>\alpha_i</math> are distinct, then it is non-zero. | |||
The Vandermonde determinant is sometimes called the [[discriminant]], although many sources, including this article, refer to the discriminant as the square of this determinant. Note that the Vandermonde determinant is ''alternating'' in the entries, meaning that permuting the <math>\alpha_i</math> by an [[odd permutation]] changes the sign, while permuting them by an [[even permutation]] does not change the value of the determinant. It thus depends on the order, while its square (the discriminant) does not depend on the order. | |||
= | When two or more α<sub>''i''</sub> are equal, the corresponding [[polynomial interpolation]] problem (see below) is <!-- [[Well-posed problem|ill-posed]] --> [[underdetermined system|underdetermined]]. In that case one may use a generalization called '''confluent Vandermonde matrices''', which makes the matrix <!-- [[positive-definite matrix|positive definite]] --> [[Invertible matrix|non-singular]] while retaining most properties. If α<sub>''i''</sub> = α<sub>''i'' + 1</sub> = ... = α<sub>''i''+''k''</sub> and α<sub>''i''</sub> ≠ α<sub>''i'' − 1</sub>, then the (''i'' + ''k'')th row is given by | ||
:<math> V_{i+k,j} = \begin{cases} 0, & \text{if } j \le k; \\ \frac{(j-1)!}{(j-k-1)!} \alpha_i^{j-k-1}, & \text{if } j > k. \end{cases} </math> | |||
= | The above formula for confluent Vandermonde matrices can be readily derived by letting two parameters <math>\alpha_i</math> and <math>\alpha_j</math> go arbitrarily close to each other. The difference vector between the rows corresponding to <math>\alpha_i</math> and <math>\alpha_j</math> scaled to a constant yields the above equation (for ''k'' = 1). Similarly, the cases ''k'' > 1 are obtained by higher order differences. Consequently, the confluent rows are derivatives of the original Vandermonde row. | ||
==Properties== | |||
Using the [[Leibniz formula (determinant)|Leibniz formula]] for the determinant, | |||
== | :<math> \det(V) = \sum_{\sigma \in S_n} \sgn(\sigma) \prod_{i = 1}^n \alpha_i^{\sigma(i)-1}, </math> | ||
where ''S''<sub>''n''</sub> denotes the set of [[permutation]]s of <math>\mathbb{Z} \cap [1, n]</math>, and sgn(σ) denotes the [[even and odd permutations|signature]] of the permutation ''σ'', we can rewrite the Vandermonde determinant as | |||
:<math>\prod_{1\le i<j\le n} (\alpha_j-\alpha_i) = \sum_{\sigma \in S_n} \sgn(\sigma) \prod_{i = 1}^n \alpha_i^{\sigma(i)-1}. </math> | |||
The Vandermonde polynomial (multiplied with the [[symmetric polynomial]]s) generates all the [[alternating polynomial]]s. | |||
If ''m'' ≤ ''n'', then the matrix ''V'' has maximum [[rank of a matrix|rank]] (''m'') [[if and only if]] all α<sub>''i''</sub> are distinct. A square Vandermonde matrix is thus [[invertible matrix|invertible]] if and only if the α<sub>''i''</sub> are distinct; an explicit formula for the inverse is known.<ref>{{Cite book | |||
| title = Inverse of the Vandermonde matrix with applications | |||
| last = Turner | |||
| first = L. Richard | |||
| url =http://ntrs.nasa.gov/archive/nasa/casi.ntrs.nasa.gov/19660023042_1966023042.pdf | |||
}}</ref><ref>{{Cite journal | |||
| volume = 65 | |||
| issue = 2 | |||
| pages = 95–100 | |||
| last = Macon | |||
| first = N. | |||
| coauthors = A. Spitzbart | |||
| title = Inverses of Vandermonde Matrices | |||
| journal = The American Mathematical Monthly | |||
| date = February 1958 | |||
| jstor = 2308881 | |||
| doi = 10.2307/2308881 | |||
| publisher = The American Mathematical Monthly, Vol. 65, No. 2 | |||
}}</ref><ref>[http://www.proofwiki.org/wiki/Inverse_of_Vandermonde%27s_Matrix Inverse of Vandermonde Matrix (ProofWiki)]</ref> | |||
==Applications== | |||
The Vandermonde matrix ''evaluates'' a polynomial at a set of points; formally, it transforms ''coefficients'' of a polynomial <math>a_0+a_1x+a_2x^2+\cdots+a_{n-1}x^{n-1}</math> to the ''values'' the polynomial takes at the points <math>\alpha_i.</math> The non-vanishing of the Vandermonde determinant for distinct points <math>\alpha_i</math> shows that, for distinct points, the map from coefficients to values at those points is a one-to-one correspondence, and thus that the polynomial interpolation problem is solvable with unique solution; this result is called the ''[[unisolvence theorem]].'' | |||
They are thus useful in [[polynomial interpolation]], since solving the [[system of linear equations]] ''Vu'' = ''y'' for ''u'' with ''V'' an ''m'' × ''n'' Vandermonde matrix is equivalent to finding the [[coefficient]]s ''u''<sub>''j''</sub> of the polynomial(s) | |||
:<math> P(x)=\sum_{j=0}^{n-1} u_j x^j </math> | |||
of degree ≤ ''n'' − 1 which has (have) the property | |||
:<math> P(\alpha_i) = y_i \quad\text{for } i=1,\ldots, m. \, </math> | |||
The Vandermonde matrix can easily be inverted in terms of Lagrange basis polynomials:<ref>{{Cite book |last1=Press|first1=WH|last2=Teukolsky|first2=SA|last3=Vetterling|first3=WT|last4=Flannery|first4=BP|year=2007|title=Numerical Recipes: The Art of Scientific Computing|edition=3rd|publisher=Cambridge University Press| publication-place=New York|isbn=978-0-521-88068-8|chapter=Section 2.8.1. Vandermonde Matrices|chapter-url=http://apps.nrbook.com/empanel/index.html?pg=94 |postscript=<!-- Bot inserted parameter. Either remove it; or change its value to "." for the cite to end in a ".", as necessary. -->{{inconsistent citations}}}}</ref> each ''column'' is the coefficients of the Lagrange basis polynomial, with terms in increasing order going down. The resulting solution to the interpolation problem is called the [[Lagrange polynomial]]. | |||
The Vandermonde determinant plays a central role in the [[Induced representation|Frobenius formula]], which gives the [[character theory|character]] of [[conjugacy class]]es of [[representation theory of the symmetric group|representation]]s of the [[symmetric group]].<ref>{{Fulton-Harris}} ''Lecture 4 reviews the representation theory of symmetric groups, including the role of the Vandermonde determinant''.</ref> | |||
When the values <math>\alpha_k</math> range over powers of a [[finite field]], then the determinant | |||
<!-- is more commonly known as the [[Moore determinant]], which --> | |||
has a number of interesting properties: for example, in proving the properties of a [[BCH code]]. | |||
Confluent Vandermonde matrices are used in [[Hermite interpolation]]. | |||
A commonly known special Vandermonde matrix is the [[discrete Fourier transform]] matrix ([[DFT matrix]]), where the numbers α<sub>''i''</sub> are chosen to be the ''m'' different ''m''th [[root of unity|roots of unity]]. | |||
The Vandermonde matrix diagonalizes the [[companion matrix]]. | |||
The Vandermonde matrix is used in some forms of [[Reed–Solomon error correction]] codes. | |||
==See also== | |||
* [[Alternant matrix]] | |||
* [[Lagrange polynomial]] | |||
* [[Wronskian]] | |||
* [[List of matrices]] | |||
* [[Moore determinant over a finite field]] | |||
==References== | |||
{{reflist}} | |||
==Further reading== | |||
*{{Citation |last=Ycart |first=Bernard |title=A case of mathematical eponymy: the Vandermonde determinant |journal=Revue d'histoire des mathématiques |volume=13 |year=2013 |arxiv=1204.4716}}. To be published. | |||
==External links== | |||
{{ProofWiki|id=Vandermonde_Determinant|title=Vandermonde Determinant}} | |||
{{Numerical linear algebra}} | |||
[[Category:Matrices]] | |||
[[Category:Determinants]] | |||
[[Category:Numerical linear algebra]] |
Latest revision as of 12:30, 31 December 2013
In linear algebra, a Vandermonde matrix, named after Alexandre-Théophile Vandermonde, is a matrix with the terms of a geometric progression in each row, i.e., an m × n matrix
or
for all indices i and j.[1] (Some authors use the transpose of the above matrix.)
The determinant of a square Vandermonde matrix (where m = n) can be expressed as:
This is called the Vandermonde determinant or Vandermonde polynomial. If all the numbers are distinct, then it is non-zero.
The Vandermonde determinant is sometimes called the discriminant, although many sources, including this article, refer to the discriminant as the square of this determinant. Note that the Vandermonde determinant is alternating in the entries, meaning that permuting the by an odd permutation changes the sign, while permuting them by an even permutation does not change the value of the determinant. It thus depends on the order, while its square (the discriminant) does not depend on the order.
When two or more αi are equal, the corresponding polynomial interpolation problem (see below) is underdetermined. In that case one may use a generalization called confluent Vandermonde matrices, which makes the matrix non-singular while retaining most properties. If αi = αi + 1 = ... = αi+k and αi ≠ αi − 1, then the (i + k)th row is given by
The above formula for confluent Vandermonde matrices can be readily derived by letting two parameters and go arbitrarily close to each other. The difference vector between the rows corresponding to and scaled to a constant yields the above equation (for k = 1). Similarly, the cases k > 1 are obtained by higher order differences. Consequently, the confluent rows are derivatives of the original Vandermonde row.
Properties
Using the Leibniz formula for the determinant,
where Sn denotes the set of permutations of , and sgn(σ) denotes the signature of the permutation σ, we can rewrite the Vandermonde determinant as
The Vandermonde polynomial (multiplied with the symmetric polynomials) generates all the alternating polynomials.
If m ≤ n, then the matrix V has maximum rank (m) if and only if all αi are distinct. A square Vandermonde matrix is thus invertible if and only if the αi are distinct; an explicit formula for the inverse is known.[2][3][4]
Applications
The Vandermonde matrix evaluates a polynomial at a set of points; formally, it transforms coefficients of a polynomial to the values the polynomial takes at the points The non-vanishing of the Vandermonde determinant for distinct points shows that, for distinct points, the map from coefficients to values at those points is a one-to-one correspondence, and thus that the polynomial interpolation problem is solvable with unique solution; this result is called the unisolvence theorem.
They are thus useful in polynomial interpolation, since solving the system of linear equations Vu = y for u with V an m × n Vandermonde matrix is equivalent to finding the coefficients uj of the polynomial(s)
of degree ≤ n − 1 which has (have) the property
The Vandermonde matrix can easily be inverted in terms of Lagrange basis polynomials:[5] each column is the coefficients of the Lagrange basis polynomial, with terms in increasing order going down. The resulting solution to the interpolation problem is called the Lagrange polynomial.
The Vandermonde determinant plays a central role in the Frobenius formula, which gives the character of conjugacy classes of representations of the symmetric group.[6]
When the values range over powers of a finite field, then the determinant has a number of interesting properties: for example, in proving the properties of a BCH code.
Confluent Vandermonde matrices are used in Hermite interpolation.
A commonly known special Vandermonde matrix is the discrete Fourier transform matrix (DFT matrix), where the numbers αi are chosen to be the m different mth roots of unity.
The Vandermonde matrix diagonalizes the companion matrix.
The Vandermonde matrix is used in some forms of Reed–Solomon error correction codes.
See also
- Alternant matrix
- Lagrange polynomial
- Wronskian
- List of matrices
- Moore determinant over a finite field
References
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Template:Numerical linear algebra
- ↑ Roger A. Horn and Charles R. Johnson (1991), Topics in matrix analysis, Cambridge University Press. See Section 6.1
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My blog: http://www.primaboinca.com/view_profile.php?userid=5889534 - ↑ Template:Fulton-Harris Lecture 4 reviews the representation theory of symmetric groups, including the role of the Vandermonde determinant.