Binet–Cauchy identity: Difference between revisions
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{{short description|On products of sums of series products}} |
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In [[algebra]], the '''Binet–Cauchy identity''', named after [[Jacques Philippe Marie Binet]] and [[Augustin-Louis Cauchy]], states that <ref name=Weisstein> |
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⚫ | In [[algebra]], the '''Binet–Cauchy identity''', named after [[Jacques Philippe Marie Binet]] and [[Augustin-Louis Cauchy]], states that<ref name=Weisstein>{{cite book |title=CRC concise encyclopedia of mathematics |author=Eric W. Weisstein |page=228 |chapter-url=https://books.google.com/books?id=8LmCzWQYh_UC&pg=PA228 |chapter=Binet-Cauchy identity |isbn=1-58488-347-2 |year=2003 |edition=2nd |publisher=CRC Press}}</ref> |
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<math display="block"> |
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</ref> |
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: <math> |
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+ \sum_{1\le i < j \le n} |
+ \sum_{1\le i < j \le n} |
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(a_i b_j - a_j b_i ) |
(a_i b_j - a_j b_i ) |
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(c_i d_j - c_j d_i ) |
(c_i d_j - c_j d_i ) |
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</math> |
</math> |
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for every choice of [[real number|real]] or [[complex number]]s (or more generally, elements of a [[commutative ring]]). |
for every choice of [[real number|real]] or [[complex number]]s (or more generally, elements of a [[commutative ring]]). |
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Setting ''a<sub>i</sub>'' |
Setting {{math|1=''a<sub>i</sub>'' = ''c<sub>i</sub>''}} and {{math|1=''b<sub>j</sub>'' = ''d<sub>j</sub>''}}, it gives [[Lagrange's identity]], which is a stronger version of the [[Cauchy–Schwarz inequality]] for the [[Euclidean space]] <math display="inline">\R^n</math>. The Binet-Cauchy identity is a special case of the [[Cauchy–Binet formula]] for matrix determinants. |
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==The Binet–Cauchy identity and exterior algebra== |
==The Binet–Cauchy identity and exterior algebra== |
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When ''n'' = 3 the first and second terms on the right hand side become the squared magnitudes of [[Dot product|dot]] and [[cross product]]s respectively; in ''n'' dimensions these become the magnitudes of the dot and [[wedge product]]s. We may write it |
When {{math|1=''n'' = 3}}, the first and second terms on the right hand side become the squared magnitudes of [[Dot product|dot]] and [[cross product]]s respectively; in {{math|''n''}} dimensions these become the magnitudes of the dot and [[wedge product]]s. We may write it |
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where {{math|'''a'''}}, {{math|'''b'''}}, {{math|'''c'''}}, and {{math|'''d'''}} are vectors. It may also be written as a formula giving the dot product of two wedge products, as |
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which can be written as |
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<math display="block">(a \times b) \cdot (c \times d) = (a \cdot c)(b \cdot d) - (a \cdot d)(b \cdot c)</math> |
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in the {{math|1=''n'' = 3}} case. |
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When both {{math|'''a'''}} and {{math|'''b'''}} are unit vectors, we obtain the usual relation |
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This is a special case of the [[Exterior algebra#Inner product|Inner product]] on the exterior algebra of a vector space, which is defined on wedge-decomposable elements as the [[Gram matrix#Gram determinant|Gram determinant]] of their components. |
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==Einstein notation== |
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When both vectors are unit vectors, we obtain the usual relation |
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A relationship between the [[Levi-Civita symbol|Levi–Cevita symbol]]s and the generalized [[Kronecker delta]] is |
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<math display="block">\frac{1}{k!}\varepsilon^{\lambda_1\cdots\lambda_k\mu_{k+1}\cdots\mu_{n}} \varepsilon_{\lambda_1\cdots\lambda_k\nu_{k+1}\cdots\nu_{n}} = \delta^{\mu_{k+1}\cdots\mu_{n}}_{\nu_{k+1}\cdots\nu_{n}}\,.</math> |
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The <math>(a \wedge b) \cdot (c \wedge d) = (a \cdot c)(b \cdot d) - (a \cdot d)(b \cdot c)</math> form of the Binet–Cauchy identity can be written as |
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<math display="block">\frac{1}{(n-2)!}\left(\varepsilon^{\mu_1\cdots\mu_{n-2}\alpha\beta} ~ a_{\alpha} ~ b_{\beta} \right)\left( \varepsilon_{\mu_1\cdots\mu_{n-2}\gamma\delta} ~ c^{\gamma} ~ d^{\delta}\right) = \delta^{\alpha\beta}_{\gamma\delta} ~ a_{\alpha} ~ b_{\beta} ~ c^{\gamma} ~ d^{\delta}\,.</math> |
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==Proof== |
==Proof== |
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Expanding the last term, |
Expanding the last term, |
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<math display="block"> |
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\begin{align} |
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:<math> |
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\sum_{1\le i < j \le n} |
&\sum_{1\le i < j \le n} (a_i b_j - a_j b_i ) (c_i d_j - c_j d_i ) \\ |
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={}&{} |
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(a_i b_j - a_j b_i ) |
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(c_i d_j |
\sum_{1\le i < j \le n} (a_i c_i b_j d_j + a_j c_j b_i d_i) |
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\end{align} |
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</math> |
</math> |
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:<math> |
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= |
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\sum_{1\le i < j \le n} |
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(a_i c_i b_j d_j + a_j c_j b_i d_i) |
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- |
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\sum_{1\le i < j \le n} |
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- |
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</math> |
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where the second and fourth terms are the same and artificially added to complete the sums as follows: |
where the second and fourth terms are the same and artificially added to complete the sums as follows: |
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<math display="block"> |
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:<math> |
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= |
= |
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\sum_{i=1}^n \sum_{j=1}^n |
\sum_{i=1}^n \sum_{j=1}^n a_i c_i b_j d_j |
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a_i c_i b_j d_j |
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- |
- |
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\sum_{i=1}^n \sum_{j=1}^n |
\sum_{i=1}^n \sum_{j=1}^n a_i d_i b_j c_j. |
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a_i d_i b_j c_j. |
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</math> |
</math> |
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==Generalization== |
==Generalization== |
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A general form, also known as the [[Cauchy–Binet formula]], states the following: |
A general form, also known as the [[Cauchy–Binet formula]], states the following: |
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Suppose ''A'' is an ''m'' |
Suppose ''A'' is an ''m''×''n'' [[matrix (mathematics)|matrix]] and ''B'' is an ''n''×''m'' matrix. If ''S'' is a [[subset]] of {1, ..., ''n''} with ''m'' elements, we write ''A<sub>S</sub>'' for the ''m''×''m'' matrix whose columns are those columns of ''A'' that have indices from ''S''. Similarly, we write ''B<sub>S</sub>'' for the ''m''×''m'' matrix whose ''rows'' are those rows of ''B'' that have indices from ''S''. |
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Then the [[determinant]] of the [[matrix product]] of ''A'' and ''B'' satisfies the identity |
Then the [[determinant]] of the [[matrix product]] of ''A'' and ''B'' satisfies the identity |
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<math display="block">\det(AB) = \sum_{ S\subset\{1,\ldots,n\} \atop |S| = m} \det(A_S)\det(B_S),</math> |
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where the sum extends over all possible subsets ''S'' of {1, ..., ''n''} with ''m'' elements. |
where the sum extends over all possible subsets ''S'' of {1, ..., ''n''} with ''m'' elements. |
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We get the original identity as special case by setting |
We get the original identity as special case by setting |
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<math display="block"> |
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A=\begin{pmatrix}a_1&\dots&a_n\\b_1&\dots& b_n\end{pmatrix},\quad |
A = \begin{pmatrix}a_1&\dots&a_n\\b_1&\dots& b_n\end{pmatrix},\quad |
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B=\begin{pmatrix}c_1&d_1\\\vdots&\vdots\\c_n&d_n\end{pmatrix}. |
B = \begin{pmatrix}c_1&d_1\\\vdots&\vdots\\c_n&d_n\end{pmatrix}. |
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</math> |
</math> |
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==Notes== |
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==In-line notes and references== |
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<references/> |
<references/> |
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==References== |
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*{{citation |
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| last = Aitken | first = Alexander Craig |
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| title = Determinants and Matrices |
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|publisher=Oliver and Boyd |
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| year = 1944}} |
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*{{citation |
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| last = Harville | first = David A. |
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| title = Matrix Algebra from a Statistician's Perspective |
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|publisher=Springer |
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| year = 2008}} |
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{{DEFAULTSORT:Binet-Cauchy Identity}} |
{{DEFAULTSORT:Binet-Cauchy Identity}} |
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[[Category: |
[[Category:Algebraic identities]] |
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[[Category:Multilinear algebra]] |
[[Category:Multilinear algebra]] |
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[[Category:Articles containing proofs]] |
[[Category:Articles containing proofs]] |
Latest revision as of 13:54, 2 February 2024
In algebra, the Binet–Cauchy identity, named after Jacques Philippe Marie Binet and Augustin-Louis Cauchy, states that[1] for every choice of real or complex numbers (or more generally, elements of a commutative ring). Setting ai = ci and bj = dj, it gives Lagrange's identity, which is a stronger version of the Cauchy–Schwarz inequality for the Euclidean space . The Binet-Cauchy identity is a special case of the Cauchy–Binet formula for matrix determinants.
The Binet–Cauchy identity and exterior algebra
[edit]When n = 3, the first and second terms on the right hand side become the squared magnitudes of dot and cross products respectively; in n dimensions these become the magnitudes of the dot and wedge products. We may write it where a, b, c, and d are vectors. It may also be written as a formula giving the dot product of two wedge products, as which can be written as in the n = 3 case.
In the special case a = c and b = d, the formula yields
When both a and b are unit vectors, we obtain the usual relation where φ is the angle between the vectors.
This is a special case of the Inner product on the exterior algebra of a vector space, which is defined on wedge-decomposable elements as the Gram determinant of their components.
Einstein notation
[edit]A relationship between the Levi–Cevita symbols and the generalized Kronecker delta is
The form of the Binet–Cauchy identity can be written as
Proof
[edit]Expanding the last term, where the second and fourth terms are the same and artificially added to complete the sums as follows:
This completes the proof after factoring out the terms indexed by i.
Generalization
[edit]A general form, also known as the Cauchy–Binet formula, states the following: Suppose A is an m×n matrix and B is an n×m matrix. If S is a subset of {1, ..., n} with m elements, we write AS for the m×m matrix whose columns are those columns of A that have indices from S. Similarly, we write BS for the m×m matrix whose rows are those rows of B that have indices from S. Then the determinant of the matrix product of A and B satisfies the identity where the sum extends over all possible subsets S of {1, ..., n} with m elements.
We get the original identity as special case by setting
Notes
[edit]- ^ Eric W. Weisstein (2003). "Binet-Cauchy identity". CRC concise encyclopedia of mathematics (2nd ed.). CRC Press. p. 228. ISBN 1-58488-347-2.
References
[edit]- Aitken, Alexander Craig (1944), Determinants and Matrices, Oliver and Boyd
- Harville, David A. (2008), Matrix Algebra from a Statistician's Perspective, Springer