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:''For "outer product" in [[geometric algebra]], see [[Exterior algebra|exterior product]].''
<br><br>
In [[linear algebra]], the '''outer product''' typically refers to the [[tensor product]] of two [[vector (mathematics)|vectors]].  The result of applying the outer product to a pair of [[coordinate vector]]s is a [[matrix (mathematics)|matrix]].  The name contrasts with the [[inner product]], which takes as input a pair of vectors and produces a [[scalar (mathematics)|scalar]].


The outer product of vectors can be also regarded as a special case of the [[Kronecker product]] of matrices.
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Some authors use the expression "outer product of tensors" as a synonym of "tensor product". The outer product is also a [[higher-order function]] in some computer programming languages such as [[APL programming language|APL]] and [[Mathematica]].
 
==Definition (matrix multiplication)==
{{main|matrix multiplication}}
 
The outer product {{nowrap|'''u''' ⊗ '''v'''}} is equivalent to a matrix multiplication '''uv'''<sup>T</sup>, provided that '''u''' is represented as a {{nowrap|''m'' × 1}} [[column vector]] and '''v''' as a {{nowrap|''n'' × 1}} column vector (which makes '''v'''<sup>T</sup> a row vector).<ref>Linear Algebra (4th Edition), S. Lipcshutz, M. Lipson, Schaum’s Outlines, McGraw Hill (USA), 2009, ISBN 978-0-07-154352-1</ref> For instance, if {{nowrap|1=''m'' = 4}} and {{nowrap|1=''n'' = 3}}, then
:<math>\mathbf{u} \otimes \mathbf{v} = \mathbf{u} \mathbf{v}^\mathrm{T} =
\begin{bmatrix}u_1 \\ u_2 \\ u_3 \\ u_4\end{bmatrix}
\begin{bmatrix}v_1 & v_2 & v_3\end{bmatrix} =
\begin{bmatrix}u_1v_1 & u_1v_2 & u_1v_3 \\ u_2v_1 & u_2v_2 & u_2v_3 \\ u_3v_1 & u_3v_2 & u_3v_3 \\ u_4v_1 & u_4v_2 & u_4v_3\end{bmatrix}.</math>
 
For [[complex numbers|complex]] vectors, it is customary to use the [[conjugate transpose]] of '''v''' (denoted '''v'''<sup>H</sup>):
 
:<math>\mathbf{u} \otimes \mathbf{v} = \mathbf{u} \mathbf{v}^\mathrm{H}.</math>
 
===Contrast with inner product===
 
If {{nowrap|1=''m'' = ''n''}}, then one can take the matrix product the other way, yielding a scalar (or {{nowrap|1 × 1}} matrix):
:<math>\left\langle \mathbf{u}, \mathbf{v}\right\rangle = \mathbf{v}^\mathrm{H} \mathbf{u}</math>
which is the standard [[inner product]] for [[Euclidean vector space]]s, better known as the [[dot product]]. The inner product is the [[trace (linear algebra)|trace]] of the outer product.
 
==Definition (vectors and tensors)==
 
===Vector multiplication===
 
Given the vectors
 
:<math>\begin{align}
\mathbf{u} & =(u_1, u_2, \dots, u_m) \\
\mathbf{v} & = (v_1, v_2, \dots, v_n)
\end{align}</math>
 
their outer product {{nowrap|'''u''' ⊗ '''v'''}} is defined as the {{nowrap|''m'' × ''n''}} matrix '''A''' obtained by multiplying each element of '''u''' by each element of '''v''':<ref>http://mathworld.wolfram.com/KroneckerProduct.html</ref><ref>Encyclopaedia of Physics (2nd Edition), R.G. Lerner, G.L. Trigg, VHC publishers, 1991, (Verlagsgesellschaft) 3-527-26954-1, (VHC Inc.) 0-89573-752-3
</ref>
 
:<math>\mathbf{u} \otimes \mathbf{v} = \mathbf{A} =
\begin{bmatrix}u_1v_1 & u_1v_2 & \dots & u_1v_n \\ u_2v_1 & u_2v_2 & \dots & u_2v_n \\ \vdots & \vdots & \ddots & \vdots\\ u_mv_1 & u_mv_2 & \dots & u_mv_n \end{bmatrix}.</math>
 
For complex vectors, the [[complex conjugate]] of '''v''' (denoted '''v'''<sup>∗</sup> or '''v̅'''). Namely, matrix '''A''' is obtained by multiplying each element of '''u''' by the complex conjugate of each element of '''v'''.
 
===Tensor multiplication===
 
The outer product on tensors is typically referred to as the [[tensor product]]. Given a [[tensor]] '''a''' with [[Tensor rank|rank]] ''q'' and [[Dimension (vector space)|dimension]]s {{nowrap|(''i''<sub>1</sub>, ..., ''i''<sub>''q''</sub>)}}, and a tensor '''b''' with rank ''r'' and dimensions {{nowrap|(''j''<sub>1</sub>, ..., ''j''<sub>''r''</sub>)}}, their outer product '''c''' has rank {{nowrap|''q'' + ''r''}} and dimensions {{nowrap|(''k''<sub>'''1'''</sub>, ..., ''k''<sub>''q''+''r''</sub>)}} which are the ''i''&nbsp; dimensions followed by the ''j''&nbsp; dimensions. It is denoted in coordinate-free notation using ⊗ and components are defined [[index notation]] by:<ref>Mathematical methods for physics and engineering, K.F. Riley, M.P. Hobson, S.J. Bence, Cambridge University Press, 2010, ISBN 978-0-521-86153-3</ref>
 
:<math>\mathbf{c}=\mathbf{a}\otimes\mathbf{b}, \quad c_{ij}=a_ib_j </math>
 
similarly for higher order tensors:
 
:<math>\mathbf{T}=\mathbf{a}\otimes\mathbf{b}\otimes\mathbf{c}, \quad  T_{ijk}=a_ib_jc_k </math>
 
For example, if '''A''' has rank 3 and dimensions {{nowrap|(3, 5, 7)}} and '''B''' has rank 2 and dimensions {{nowrap|(10, 100)}}, their outer product '''c''' has rank 5 and dimensions {{nowrap|(3, 5, 7, 10, 100)}}. If '''A''' has a component {{nowrap|1=''A''<sub>[2, 2, 4]</sub> = 11}} and '''B''' has a component {{nowrap|1=''B''<sub>[8, 88]</sub> = 13}}, then the component of '''C''' formed by the outer product is {{nowrap|1=''C''<sub>[2, 2, 4, 8, 88]</sub> = 143}}.
 
To understand the matrix definition of outer product in terms of the definition of tensor product:
 
# The vector '''v''' can be interpreted as a rank 1 tensor with dimension ''M'', and the vector '''u''' as a rank 1 tensor with dimension ''N''. The result is a rank 2 tensor with dimension {{nowrap|(''M'', ''N'')}}.
# The rank of the result of an [[inner product]] between two tensors of rank ''q'' and ''r'' is the greater of {{nowrap|''q'' + ''r'' − 2}} and 0.  Thus, the inner product of two matrices has the same rank as the outer product (or tensor product) of two vectors. 
# It is possible to add arbitrarily many leading or trailing ''1'' dimensions to a tensor without fundamentally altering its structure.  These ''1'' dimensions would alter the character of operations on these tensors, so any resulting equivalences should be expressed explicitly.
# The inner product of two matrices '''V''' with dimensions {{nowrap|(''d'', ''e'')}} and '''U''' with dimensions {{nowrap|(''e'', ''f'')}} is <math>\sum_{j = 1}^e V_{ij} U_{jk}</math>, where {{nowrap|1=''i'' = 1, 2, ..., ''d''}} and {{nowrap|1=''k'' = 1, 2, ..., ''f''}}. For the case where {{nowrap|1=''e'' = 1}}, the summation is trivial (involving only a single term).
# The outer product of two matrices '''V''' with dimensions {{nowrap|(''m'', ''n'')}} and '''U''' with dimensions {{nowrap|(''p'', ''q'')}} is <math> C_{st} = V_{ij} U_{hk}</math>, where {{nowrap|1=''s'' = 1, 2, ..., ''mp'' − 1, ''mp''}} and {{nowrap|1=''t'' = 1, 2, ..., ''nq'' − ''1'', ''nq''}}.
 
The term "rank" is used here in its [[tensor]] sense, and should not be interpreted as [[Rank (linear algebra)|matrix rank]].
 
==Definition (abstract)==
Let ''V'' and ''W'' be two [[vector space]]s, and let ''W''<sup>∗</sup> be the [[dual space]] of ''W''.
Given a vector {{nowrap|''x'' ∈ ''V''}} and {{nowrap|''y''<sup></sup> ∈ ''W''<sup>∗</sup>}}, then  the tensor product {{nowrap|''y''<sup>∗</sup> ⊗ ''x''}} corresponds to the map {{nowrap|''A'' : W → ''V''}} given by
 
:<math>w \mapsto y^*(w)x.</math>
 
Here ''y''<sup>∗</sup>(''w'') denotes the value of the [[linear functional]] ''y''<sup>∗</sup> (which is an element of the dual space of ''W'') when evaluated at the element {{nowrap|''w'' ∈ ''W''}}. This scalar in turn is multiplied by ''x'' to give as the final result an element of the space ''V''.
 
If ''V'' and ''W'' are finite-dimensional, then the space of all linear transformations from ''W'' to ''V'', denoted {{nowrap|Hom(''W'', ''V'')}}, is generated by such outer products; in fact, the rank of a matrix is the minimal number of such outer products needed to express it as a sum (this is the '''tensor rank''' of a matrix). In this case {{nowrap|Hom(''W'', ''V'')}} is [[isomorphic]] to {{nowrap|''W''<sup>∗</sup> ⊗ ''V''}}.
 
===Contrast with inner product===
{{See also|Inner product space}}
 
If {{nowrap|1=''W'' = ''V''}}, then one can also pair the covector {{nowrap|''w''<sup>∗</sup> ∈ ''V''<sup>∗</sup>}} with the vector {{nowrap|''v'' ∈ ''V''}} via {{nowrap|(''w''<sup>∗</sup>, ''v'') → ''w''<sup>∗</sup>(''v'')}}, which is the duality pairing between ''V'' and its dual, sometimes called the [[inner product]].
 
==Applications==
 
The outer product is useful in computing physical quantities (e.g., the [[Moment of inertia|tensor of inertia]]), and performing transform operations in [[digital signal processing]] and [[digital image processing]]. It is also useful in [[statistical analysis]] for computing the [[covariance]] and auto-covariance matrices for two [[random variables]].
 
==See also==
* [[Linear algebra]]
* [[Norm (mathematics)]]
* [[Scatter matrix]]
* [[Ricci calculus]]
 
===Products===
* [[Cross product]]
* [[Exterior product]]
 
===Duality===
* [[Complex conjugate]]
* [[Conjugate transpose]]
* [[Transpose]]
* [[Bra–ket notation#Outer products|Bra–ket notation for outer product]]
 
==References==
 
{{reflist}}
 
{{Linear algebra}}
 
{{DEFAULTSORT:Outer Product}}
[[Category:Bilinear operators]]
[[Category:Binary operations]]
[[Category:Higher-order functions]]

Revision as of 08:44, 3 March 2014



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