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{{short description|On products of sums of series products}}
{{Unreferenced|date=December 2009}}
In [[algebra]], the '''Binet–Cauchy identity''', named after [[Jacques Philippe Marie Binet]] and [[Augustin Louis Cauchy]], states that
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>
<math display="block">

\left(\sum_{i=1}^n a_i c_i\right)
: <math>
\biggl(\sum_{i=1}^n a_i c_i\biggr)
\left(\sum_{j=1}^n b_j d_j\right) =
\biggl(\sum_{j=1}^n b_j d_j\biggr) =
\left(\sum_{i=1}^n a_i d_i\right)
\biggl(\sum_{i=1}^n a_i d_i\biggr)
\left(\sum_{j=1}^n b_j c_j\right)
\biggl(\sum_{j=1}^n b_j c_j\biggr)
+ \sum_{1\le i < j \le n}
+ \sum_{1\le i < j \le n}
(a_i b_j - a_j b_i )
(a_i b_j - a_j b_i )
(c_i d_j - c_j d_i )
(c_i d_j - c_j d_i )
</math>
</math>

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]]).
Setting ''a<sub>i</sub>''&nbsp;=&nbsp;''c<sub>i</sub>'' and ''b<sub>i</sub>''&nbsp;=&nbsp;''d<sub>i</sub>'', it gives the [[Lagrange's identity]], which is a stronger version of the [[Cauchy–Schwarz inequality]] for the [[Euclidean space]] <math>\scriptstyle\mathbb{R}^n</math>.
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.


==The Binet–Cauchy identity and exterior algebra==
==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 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
<math display="block">(a \cdot c)(b \cdot d) = (a \cdot d)(b \cdot c) + (a \wedge b) \cdot (c \wedge d)</math>
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
<math display="block">(a \wedge b) \cdot (c \wedge d) = (a \cdot c)(b \cdot d) - (a \cdot d)(b \cdot c)\,,</math>
which can be written as
<math display="block">(a \times b) \cdot (c \times d) = (a \cdot c)(b \cdot d) - (a \cdot d)(b \cdot c)</math>
in the {{math|1=''n'' = 3}} case.


In the special case {{math|1='''a''' = '''c'''}} and {{math|1='''b''' = '''d'''}}, the formula yields
:<math>(a \cdot c)(b \cdot d) = (a \cdot d)(b \cdot c) + (a \wedge b) \cdot (c \wedge d)\,</math>
<math display="block">|a \wedge b|^2 = |a|^2|b|^2 - |a \cdot b|^2. </math>


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
When both {{math|'''a'''}} and {{math|'''b'''}} are unit vectors, we obtain the usual relation
<math display="block">\sin^2 \phi = 1 - \cos^2 \phi</math>
where {{math|''φ''}} is the angle between the vectors.


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.
:<math>(a \wedge b) \cdot (c \wedge d) = (a \cdot c)(b \cdot d) - (a \cdot d)(b \cdot c).\,</math>

In the special case of unit vectors ''a=c'' and ''b=d'', the formula yields the usual relation
==Einstein notation==
:<math>1= \cos^2(\phi)+\sin^2(\phi)</math>
A relationship between the [[Levi-Civita symbol|Levi–Cevita symbol]]s and the generalized [[Kronecker delta]] is
where &phi; is the angle between the vectors.
<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>

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
<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>


==Proof==
==Proof==
Expanding the last term,
Expanding the last term,
<math display="block">

\begin{align}
:<math>
\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 ) \\
={}&{}
(a_i b_j - a_j b_i )
(c_i d_j - c_j d_i )
\sum_{1\le i < j \le 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\le i < j \le 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{align}
</math>
</math>
:<math>
=
\sum_{1\le i < j \le 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\le i < j \le 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
</math>

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:
<math display="block">

:<math>
=
=
\sum_{i=1}^n \sum_{j=1}^n
\sum_{i=1}^n \sum_{j=1}^n a_i c_i b_j d_j
a_i c_i b_j d_j
-
-
\sum_{i=1}^n \sum_{j=1}^n
\sum_{i=1}^n \sum_{j=1}^n a_i d_i b_j c_j.
a_i d_i b_j c_j.
</math>
</math>


This completes the proof after factoring out the terms indexed by ''i''. ''[[Q.E.D.|(q. e. d.)]]''
This completes the proof after factoring out the terms indexed by ''i''.


==Generalization==
==Generalization==
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:
Suppose ''A'' is an ''m''&times;''n'' [[matrix (mathematics)|matrix]] and ''B'' is an ''n''&times;''m'' matrix. If ''S'' is a [[subset]] of {1, ..., ''n''} with ''m'' elements, we write ''A<sub>S</sub>'' for the ''m''&times;''m'' matrix whose columns are those columns of ''A'' that have indices from ''S''. Similarly, we write ''B<sub>S</sub>'' for the ''m''&times;''m'' matrix whose ''rows'' are those rows of ''B'' that have indices from ''S''.
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''.
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
:<math>\det(AB) = \sum_{\scriptstyle S\subset\{1,\ldots,n\}\atop\scriptstyle|S|=m} \det(A_S)\det(B_S),</math>
<math display="block">\det(AB) = \sum_{ S\subset\{1,\ldots,n\} \atop |S| = m} \det(A_S)\det(B_S),</math>
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.


We get the original identity as special case by setting
We get the original identity as special case by setting
:<math>
<math display="block">
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
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}.
</math>
</math>


==Notes==
{{DEFAULTSORT:Binet–Cauchy Identity}}
<references/>
[[Category:Mathematical identities]]
==References==
*{{citation
| last = Aitken | first = Alexander Craig
| title = Determinants and Matrices
|publisher=Oliver and Boyd
| year = 1944}}
*{{citation
| last = Harville | first = David A.
| title = Matrix Algebra from a Statistician's Perspective
|publisher=Springer
| year = 2008}}

{{DEFAULTSORT:Binet-Cauchy Identity}}
[[Category:Algebraic identities]]
[[Category:Multilinear algebra]]
[[Category:Multilinear algebra]]
[[Category:Articles containing proofs]]
[[Category:Articles containing proofs]]

[[bs:Binet–Cauchyjev identitet]]

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]
  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

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