Binet–Cauchy identity

On products of sums of series products

In algebra, the Binet–Cauchy identity, named after Jacques Philippe Marie Binet and Augustin-Louis Cauchy, states that[1] ( i = 1 n a i c i ) ( j = 1 n b j d j ) = ( i = 1 n a i d i ) ( j = 1 n b j c j ) + 1 i < j n ( a i b j a j b i ) ( c i d j c j d i ) {\displaystyle \left(\sum _{i=1}^{n}a_{i}c_{i}\right)\left(\sum _{j=1}^{n}b_{j}d_{j}\right)=\left(\sum _{i=1}^{n}a_{i}d_{i}\right)\left(\sum _{j=1}^{n}b_{j}c_{j}\right)+\sum _{1\leq i<j\leq n}(a_{i}b_{j}-a_{j}b_{i})(c_{i}d_{j}-c_{j}d_{i})} 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 R n {\textstyle \mathbb {R} ^{n}} . The Binet-Cauchy identity is a special case of the Cauchy–Binet formula for matrix determinants.

The Binet–Cauchy identity and exterior algebra

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 ( a c ) ( b d ) = ( a d ) ( b c ) + ( a b ) ( c d ) {\displaystyle (a\cdot c)(b\cdot d)=(a\cdot d)(b\cdot c)+(a\wedge b)\cdot (c\wedge d)} 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 ( a b ) ( c d ) = ( a c ) ( b d ) ( a d ) ( b c ) , {\displaystyle (a\wedge b)\cdot (c\wedge d)=(a\cdot c)(b\cdot d)-(a\cdot d)(b\cdot c)\,,} which can be written as ( a × b ) ( c × d ) = ( a c ) ( b d ) ( a d ) ( b c ) {\displaystyle (a\times b)\cdot (c\times d)=(a\cdot c)(b\cdot d)-(a\cdot d)(b\cdot c)} in the n = 3 case.

In the special case a = c and b = d, the formula yields | a b | 2 = | a | 2 | b | 2 | a b | 2 . {\displaystyle |a\wedge b|^{2}=|a|^{2}|b|^{2}-|a\cdot b|^{2}.}

When both a and b are unit vectors, we obtain the usual relation sin 2 ϕ = 1 cos 2 ϕ {\displaystyle \sin ^{2}\phi =1-\cos ^{2}\phi } 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

A relationship between the Levi–Cevita symbols and the generalized Kronecker delta is 1 k ! ε λ 1 λ k μ k + 1 μ n ε λ 1 λ k ν k + 1 ν n = δ ν k + 1 ν n μ k + 1 μ n . {\displaystyle {\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 _{\nu _{k+1}\cdots \nu _{n}}^{\mu _{k+1}\cdots \mu _{n}}\,.}

The ( a b ) ( c d ) = ( a c ) ( b d ) ( a d ) ( b c ) {\displaystyle (a\wedge b)\cdot (c\wedge d)=(a\cdot c)(b\cdot d)-(a\cdot d)(b\cdot c)} form of the Binet–Cauchy identity can be written as 1 ( n 2 ) ! ( ε μ 1 μ n 2 α β   a α   b β ) ( ε μ 1 μ n 2 γ δ   c γ   d δ ) = δ γ δ α β   a α   b β   c γ   d δ . {\displaystyle {\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 _{\gamma \delta }^{\alpha \beta }~a_{\alpha }~b_{\beta }~c^{\gamma }~d^{\delta }\,.}

Proof

Expanding the last term, 1 i < j n ( a i b j a j b i ) ( c i d j c j d i ) = 1 i < j n ( a i c i b j d j + a j c j b i d i ) + i = 1 n a i c i b i d i 1 i < j n ( a i d i b j c j + a j d j b i c i ) i = 1 n a i d i b i c i {\displaystyle {\begin{aligned}&\sum _{1\leq i<j\leq n}(a_{i}b_{j}-a_{j}b_{i})(c_{i}d_{j}-c_{j}d_{i})\\={}&{}\sum _{1\leq i<j\leq n}(a_{i}c_{i}b_{j}d_{j}+a_{j}c_{j}b_{i}d_{i})+\sum _{i=1}^{n}a_{i}c_{i}b_{i}d_{i}-\sum _{1\leq i<j\leq n}(a_{i}d_{i}b_{j}c_{j}+a_{j}d_{j}b_{i}c_{i})-\sum _{i=1}^{n}a_{i}d_{i}b_{i}c_{i}\end{aligned}}} where the second and fourth terms are the same and artificially added to complete the sums as follows: = i = 1 n j = 1 n a i c i b j d j i = 1 n j = 1 n a i d i b j c j . {\displaystyle =\sum _{i=1}^{n}\sum _{j=1}^{n}a_{i}c_{i}b_{j}d_{j}-\sum _{i=1}^{n}\sum _{j=1}^{n}a_{i}d_{i}b_{j}c_{j}.}

This completes the proof after factoring out the terms indexed by i.

Generalization

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 det ( A B ) = S { 1 , , n } | S | = m det ( A S ) det ( B S ) , {\displaystyle \det(AB)=\sum _{S\subset \{1,\ldots ,n\} \atop |S|=m}\det(A_{S})\det(B_{S}),} 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 A = ( a 1 a n b 1 b n ) , B = ( c 1 d 1 c n d n ) . {\displaystyle A={\begin{pmatrix}a_{1}&\dots &a_{n}\\b_{1}&\dots &b_{n}\end{pmatrix}},\quad B={\begin{pmatrix}c_{1}&d_{1}\\\vdots &\vdots \\c_{n}&d_{n}\end{pmatrix}}.}

Notes

  1. ^ Eric W. Weisstein (2003). "Binet-Cauchy identity". CRC concise encyclopedia of mathematics (2nd ed.). CRC Press. p. 228. ISBN 1-58488-347-2.

References

  • Aitken, Alexander Craig (1944), Determinants and Matrices, Oliver and Boyd
  • Harville, David A. (2008), Matrix Algebra from a Statistician's Perspective, Springer