In
linear algebraLinear algebra is a branch of mathematics that studies vector spaces, also called linear spaces, along with linear functions that input one vector and output another. Such functions are called linear maps and can be represented by matrices if a basis is given. Thus matrix theory is often...
, the
Schmidt decomposition (named after its originator
Erhard SchmidtErhard Schmidt was a German mathematician whose work significantly influenced the direction of mathematics in the twentieth century. He was born in Tartu, Governorate of Livonia . His advisor was David Hilbert and he was awarded his doctorate from Georg-August University of Göttingen in 1905...
) refers to a particular way of expressing a
vectorIn linear algebra, a coordinate vector is an explicit representation of a vector in an abstract vector space as an ordered list of numbers or, equivalently, as an element of the coordinate space Fn....
in the
tensor productIn mathematics, the tensor product, denoted by ⊗, may be applied in different contexts to vectors, matrices, tensors, vector spaces, algebras, topological vector spaces, and modules, among many other structures or objects. In each case the significance of the symbol is the same: the most general...
of two
inner product spaceIn mathematics, an inner product space is a vector space with an additional structure called an inner product. This additional structure associates each pair of vectors in the space with a scalar quantity known as the inner product of the vectors...
s. It has applications in quantum information theory and
plasticityIn physics and materials science, plasticity describes the deformation of a material undergoing non-reversible changes of shape in response to applied forces. For example, a solid piece of metal being bent or pounded into a new shape displays plasticity as permanent changes occur within the...
.
Theorem
Let

and

be Hilbert spaces of
dimensionIn physics and mathematics, the dimension of a space or object is informally defined as the minimum number of coordinates needed to specify any point within it. Thus a line has a dimension of one because only one coordinate is needed to specify a point on it...
s
n and
m respectively. Assume

. For any vector

in the tensor product

, there exist orthonormal sets

and

such that

, where the scalars

are non-negative and, as a set, uniquely determined by

.
Proof
The Schmidt decomposition is essentially a restatement of the
singular value decompositionIn linear algebra, the singular value decomposition is a factorization of a real or complex matrix, with many useful applications in signal processing and statistics....
in a different context. Fix orthonormal bases

and

. We can identify an elementary tensor

with the matrix

, where

is the
transposeIn linear algebra, the transpose of a matrix A is another matrix AT created by any one of the following equivalent actions:...
of

. A general element of the tensor product
can then be viewed as the
n ×
m matrix
By the singular value decomposition, there exist an
n ×
n unitary
U,
m ×
m unitary
V, and a
positive semidefiniteIn mathematics, positive semidefinite may refer to:* positive-semidefinite matrix* positive-semidefinite function...
diagonal
m ×
m matrix Σ such that
Write

where

is
n ×
m and we have
Let

be the first
m column vectors of

,

the column vectors of
V, and

the diagonal elements of Σ. The previous expression is then
which proves the claim.
Spectrum of reduced states
Consider a vector in the form of Schmidt decomposition
Form the rank 1 matrix
ρ =
v v*. Then the
partial traceIn linear algebra and functional analysis, the partial trace is a generalization of the trace. Whereas the trace is a scalar valued function on operators, the partial trace is an operator-valued function...
of
ρ, with respect to either system
A or
B, is a diagonal matrix whose non-zero diagonal elements are |
αi |
2. In other words, the Schmidt decomposition shows that the reduced state of
ρ on either subsystem have the same spectrum.
In the language of quantum mechanics, a rank 1 projection
ρ is called a pure state. A consequence of the above comments is that, for bipartite pure states, the
von Neumann entropyIn quantum statistical mechanics, von Neumann entropy, named after John von Neumann, is the extension of classical entropy concepts to the field of quantum mechanics....
of either reduced state is a well defined measure of entanglement.
Schmidt rank and entanglement
For an element
w of the tensor product

the strictly positive values

in its Schmidt decomposition are its
Schmidt coefficients. The number of Schmidt coefficients of

is called its
Schmidt rank.
If
w can not be expressed as

then
w is said to be an
entangled stateQuantum entanglement occurs when electrons, molecules even as large as "buckyballs", photons, etc., interact physically and then become separated; the type of interaction is such that each resulting member of a pair is properly described by the same quantum mechanical description , which is...
. From the Schmidt decomposition, we can see that
w is entangled if and only if
w has Schmidt rank strictly greater than 1. Therefore, a bipartite pure state is entangled if and only if its reduced states are mixed states.
Crystal plasticity
In the field of plasticity, crystalline solids such as metals deform plastically primarily along crystal planes. Each plane, defined by its normal vector ν can "slip" in one of several directions, defined by a vector μ. Together a slip plane and direction form a slip system which is described by the Schmidt tensor

. The velocity gradient is a linear combination of these across all slip systems where the scaling factor is the rate of slip along the system.