In mathematics, the Cauchy–Schwarz inequality is a useful inequality encountered in many different settings, such as linear algebra, analysis, probability theory, and other areas. It is considered to be one of the most important inequalities in all of mathematics.^{[1]} It has a number of generalizations, among them Hölder's inequality.
The inequality for sums was published by AugustinLouis Cauchy (1821), while the corresponding inequality for integrals was first proved by Viktor Bunyakovsky (1859). The modern proof of the integral inequality was given by Hermann Amandus Schwarz (1888).^{[1]}
Statement of the inequality
The Cauchy–Schwarz inequality states that for all vectors x and y of an inner product space it is true that

\langle x,y\rangle ^2 \leq \langle x,x\rangle \cdot \langle y,y\rangle,
where \langle\cdot,\cdot\rangle is the inner product also known as dot product. Equivalently, by taking the square root of both sides, and referring to the norms of the vectors, the inequality is written as

\langle x,y\rangle \leq \x\ \cdot \y\.\, ^{[2]}
Moreover, the two sides are equal if and only if x and y are linearly dependent (or, in a geometrical sense, they are parallel or one of the vectors' magnitude is zero).
If x_1,\ldots, x_n\in\mathbb C and y_1,\ldots, y_n\in\mathbb C have an imaginary component, the inner product is the standard inner product and the bar notation is used for complex conjugation then the inequality may be restated more explicitly as

x_1 \bar{y}_1 + \cdots + x_n \bar{y}_n^2 \leq (x_1^2 + \cdots + x_n^2) (y_1^2 + \cdots + y_n^2).
When viewed in this way the numbers x_{1}, ..., x_{n}, and y_{1}, ..., y_{n} are the components of x and y with respect to an orthonormal basis of V.
Even more compactly written:

\left \sum_{i=1}^n x_i \bar{y}_i \right^2 \leq \sum_{j=1}^n x_j^2 \sum_{k=1}^n y_k^2 .
Equality holds if and only if x and y are linearly dependent, that is, one is a scalar multiple of the other (which includes the case when one or both are zero).
The finitedimensional case of this inequality for real vectors was proven by Cauchy in 1821, and in 1859 Cauchy's student Bunyakovsky noted that by taking limits one can obtain an integral form of Cauchy's inequality. The general result for an inner product space was obtained by Schwarz in the year 1888.
Proof
Let u, v be arbitrary vectors in a vector space V over F with an inner product, where F is the field of real or complex numbers. We prove the inequality

\big \langle u,v \rangle \big \leq \left\u\right\ \left\v\right\,
and the fact that equality holds only when u and v are linearly dependent (the fact that conversely one has equality if u and v are linearly dependent is immediate from the properties of the inner product).
If v = 0 it is clear that we have equality, and in this case u and v are also linearly dependent (regardless of u). We henceforth assume that v is nonzero. We also assume that \langle u, v \rangle \ne 0 otherwise the inequality is obviously true, because neither \left\ u \right\ nor \left\ v \right\ can be negative.
Let

z= u\frac {\langle u, v \rangle} {\langle v, v \rangle} v.
Then, by linearity of the inner product in its first argument, one has

\langle z, v \rangle = \left\langle u \frac {\langle u, v \rangle} {\langle v, v \rangle} v, v\right\rangle = \langle u, v \rangle  \frac {\langle u, v \rangle} {\langle v, v \rangle} \langle v, v \rangle = 0,
i.e., z is a vector orthogonal to the vector v (Indeed, z is the projection of u onto the plane orthogonal to v.). We can thus apply the Pythagorean theorem to

u= \frac {\langle u, v \rangle} {\langle v, v \rangle} v+z,
which gives

\left\u\right\^2 = \left\frac{\langle u, v \rangle}{\langle v, v \rangle}\right^2 \left\v\right\^2 + \left\z\right\^2 = \frac{\langle u, v \rangle^2}{\left\v\right\^2} + \left\z\right\^2 \geq \frac{\langle u, v \rangle^2}{\left\v\right\^2},
and, after multiplication by v^{2}, the Cauchy–Schwarz inequality. Moreover, if the relation '≥' in the above expression is actually an equality, then z^{2} = 0 and hence z = 0; the definition of z then establishes a relation of linear dependence between u and v. This establishes the theorem.
Alternative Proof
Let u, v be arbitrary vectors in a vector space V over F with an inner product, where F is the field of real or complex numbers.
If \langle u, v \rangle = 0, the theorem holds trivially.
If not, then u \ne 0, v \ne 0. Choose \lambda = \frac{\langle u, v \rangle}{\langle u, v \rangle}. Then \lambda = 1, and

0 \le \left\\frac{\lambda u}{\u\}  \frac{v}{\v\}\right\^2 = \lambda^2 \frac{\u\^2}{\u\^2}  2 \text{Re}\left(\left\langle \frac{\lambda u}{\u\}, \frac{v}{\v\} \right\rangle\right) + \frac{\v\^2}{\v\^2} = 2  2 \frac{\text{Re}\left(\lambda \langle u, v \rangle\right)}{\u\\v\}
It follows that

\langle u, v \rangle = \text{Re}\left(\lambda \langle u, v \rangle\right) \le \u\\v\
Special cases
R^{n}
In Euclidean space \mathbb R ^n with the standard inner product, the Cauchy–Schwarz inequality is

\left(\sum_{i=1}^n x_i y_i\right)^2\leq \left(\sum_{i=1}^n x_i^2\right) \left(\sum_{i=1}^n y_i^2\right).
To prove this form of the inequality, consider the following quadratic polynomial in z.

(x_1 z + y_1)^2 + \cdots + (x_n z + y_n)^2 = \left( \sum ( x_i^2) \right) \cdot z^2 + 2 \cdot \left( \sum ( x_i \cdot y_i) \right) \cdot z + \sum ( y_i^2)
Since it is nonnegative it has at most one real root in z, whence its discriminant is less than or equal to zero, that is,

\left(\sum ( x_i \cdot y_i ) \right)^2  \sum {x_i^2} \cdot \sum {y_i^2} \le 0,
which yields the Cauchy–Schwarz inequality.
An equivalent proof for \mathbb R ^n starts with the summation below.
Expanding the brackets we have:

\sum_{i=1}^n \sum_{j=1}^n \left( x_i y_j  x_j y_i \right)^2 = \sum_{i=1}^n x_i^2 \sum_{j=1}^n y_j^2 + \sum_{j=1}^n x_j^2 \sum_{i=1}^n y_i^2  2 \sum_{i=1}^n x_i y_i \sum_{j=1}^n x_j y_j,
collecting together identical terms (albeit with different summation indices) we find:

\frac{1}{2} \sum_{i=1}^n \sum_{j=1}^n \left( x_i y_j  x_j y_i \right)^2 = \sum_{i=1}^n x_i^2 \sum_{i=1}^n y_i^2  \left( \sum_{i=1}^n x_i y_i \right)^2.
Because the lefthand side of the equation is a sum of the squares of real numbers it is greater than or equal to zero, thus:

\sum_{i=1}^n x_i^2 \sum_{i=1}^n y_i^2  \left( \sum_{i=1}^n x_i y_i \right)^2 \geq 0.
Yet another approach when n ≥ 2 (n = 1 is trivial) is to consider the plane containing x and y. More precisely, recoordinatize R^{n} with any orthonormal basis whose first two vectors span a subspace containing x and y. In this basis only x_1,~x_2,~y_1 and y_2~ are nonzero, and the inequality reduces to the algebra of dot product in the plane, which is related to the angle between two vectors, from which we obtain the inequality:

x \cdot y = \x\ \y\  \cos \theta  \le \x\ \y\.
When n = 3 the Cauchy–Schwarz inequality can also be deduced from Lagrange's identity, which takes the form

\langle x,x\rangle \cdot \langle y,y\rangle = \langle x,y\rangle^2 + x \times y^2
from which readily follows the Cauchy–Schwarz inequality.
Another proof of the general case for n can be done by using the technique used to prove Inequality of arithmetic and geometric means.
L^{2}
For the inner product space of squareintegrable complexvalued functions, one has

\left\int_{\mathbb{R}^n} f(x) \overline{g(x)}\,dx\right^2\leq\int_{\mathbb{R}^n} \leftf(x)\right^2\,dx \cdot \int_{\mathbb{R}^n}\leftg(x)\right^2\,dx.
A generalization of this is the Hölder inequality.
Applications
The triangle inequality for the inner product is often shown as a consequence of the Cauchy–Schwarz inequality, as follows: given vectors x and y:

\begin{align} \x + y\^2 & = \langle x + y, x + y \rangle \\ & = \x\^2 + \langle x, y \rangle + \langle y, x \rangle + \y\^2 \\ & = \x\^2 + 2 \text{ Re} \langle x, y \rangle + \y\^2\\ & \le \x\^2 + 2\langle x, y \rangle + \y\^2 \\ & \le \x\^2 + 2\x\\y\ + \y\^2 \\ & = \left (\x\ + \y\\right)^2. \end{align}
Taking square roots gives the triangle inequality.
The Cauchy–Schwarz inequality allows one to extend the notion of "angle between two vectors" to any real inner product space, by defining:

\cos\theta_{xy}=\frac{\langle x,y\rangle}{\x\ \y\}.
The Cauchy–Schwarz inequality proves that this definition is sensible, by showing that the righthand side lies in the interval [−1, 1], and justifies the notion that (real) Hilbert spaces are simply generalizations of the Euclidean space.
It can also be used to define an angle in complex inner product spaces, by taking the absolute value of the righthand side, as is done when extracting a metric from quantum fidelity.
The Cauchy–Schwarz is used to prove that the inner product is a continuous function with respect to the topology induced by the inner product itself.
The Cauchy–Schwarz inequality is usually used to show Bessel's inequality.
Probability theory
Let X, Y be random variables, then:

\text{Var}\left(Y\right)\ge\frac{\text{Cov}\left(Y,X\right)\text{Cov}\left(Y,X\right)}{\text{Var}\left(X\right)}.
In fact we can define an inner product on the set of random variables using the expectation of their product:

\langle X, Y \rangle \triangleq \operatorname{E}(X Y),
and so, by the Cauchy–Schwarz inequality,

\operatorname{E}(XY)^2 \leq \operatorname{E}(X^2) \operatorname{E}(Y^2).
Moreover, if μ = E(X) and ν = E(Y), then

\begin{align} \operatorname{Cov}(X,Y)^2 &= \operatorname{E}( (X  \mu)(Y  \nu) )^2 \\ &=  \langle X  \mu, Y  \nu \rangle ^2\\ &\leq \langle X  \mu, X  \mu \rangle \langle Y  \nu, Y  \nu \rangle \\ & = \operatorname{E}( (X\mu)^2 ) \operatorname{E}( (Y\nu)^2 ) \\ & = \operatorname{Var}(X) \operatorname{Var}(Y), \end{align}
where Var denotes variance and Cov denotes covariance.
Generalizations
Various generalizations of the Cauchy–Schwarz inequality exist in the context of operator theory, e.g. for operatorconvex functions, and operator algebras, where the domain and/or range of φ are replaced by a C*algebra or W*algebra.
This section lists a few of such inequalities from the operator algebra setting, to give a flavor of results of this type.
Positive functionals on C* and W*algebras
One can discuss inner products as positive functionals. Given a Hilbert space L^{2}(m), m being a finite measure, the inner product < · , · > gives rise to a positive functional φ by

\phi (g) = \langle g, 1 \rangle.
Since < f, f > ≥ 0, φ(f*f) ≥ 0 for all f in L^{2}(m), where f* is pointwise conjugate of f. So φ is positive. Conversely every positive functional φ gives a corresponding inner product < f, g >_{φ} = φ(g*f). In this language, the Cauchy–Schwarz inequality becomes

 \phi(g^*f) ^2 \leq \phi(f^*f) \phi(g^*g),
which extends verbatim to positive functionals on C*algebras.
We now give an operator theoretic proof for the Cauchy–Schwarz inequality which passes to the C*algebra setting. One can see from the proof that the Cauchy–Schwarz inequality is a consequence of the positivity and antisymmetry innerproduct axioms.
Consider the positive matrix

M = \begin{bmatrix} f^*\\ g^* \end{bmatrix} \begin{bmatrix} f & g \end{bmatrix} = \begin{bmatrix} f^*f & f^* g \\ g^*f & g^*g \end{bmatrix}.
Since φ is a positive linear map whose range, the complex numbers C, is a commutative C*algebra, φ is completely positive. Therefore

M' = (I_2 \otimes \phi)(M) = \begin{bmatrix} \phi(f^*f) & \phi(f^* g) \\ \phi(g^*f) & \phi(g^*g) \end{bmatrix}
is a positive 2 × 2 scalar matrix, which implies it has positive determinant:

\phi \left (f^*f \right) \phi \left (g^*g \right)  \left  \phi \left (g^*f \right) \right ^2 \geq 0 \quad \text{i.e.} \quad \phi\left (f^*f \right) \left (g^*g \right) \geq \left  \phi \left (g^*f \right ) \right^2.
This is precisely the Cauchy–Schwarz inequality. If f and g are elements of a C*algebra, f* and g* denote their respective adjoints.
We can also deduce from above that every positive linear functional is bounded, corresponding to the fact that the inner product is jointly continuous.
Positive maps
Positive functionals are special cases of positive maps. A linear map Φ between C*algebras is said to be a positive map if a ≥ 0 implies Φ(a) ≥ 0. It is natural to ask whether inequalities of Schwarztype exist for positive maps. In this more general setting, usually additional assumptions are needed to obtain such results.
Kadison–Schwarz inequality
The following theorem is named after Richard Kadison.
Theorem. If \Phi is a unital positive map, then for every normal element a in its domain, we have \Phi(a^*a) \ge \Phi(a^*) \Phi(a) and \Phi(a^*a) \ge \Phi(a) \Phi(a^*).
This extends the fact \varphi(a^*a) \cdot 1 \ge \varphi(a)^* \varphi(a) = \varphi(a)^2, when \varphi is a linear functional.
The case when a is selfadjoint, i.e. a = a^*, is sometimes known as Kadison's inequality.
2positive maps
When Φ is 2positive, a stronger assumption than merely positive, one has something that looks very similar to the original Cauchy–Schwarz inequality:
Theorem (Modified Schwarz inequality for 2positive maps).^{[3]} For a 2positive map Φ between C*algebras, for all a, b in its domain,

\Phi(a)^*\Phi(a) \leq \Vert\Phi(1)\Vert\Phi(a^*a)

\Vert\Phi(a^*b)\Vert^2 \leq \Vert\Phi(a^*a)\Vert \cdot \Vert\Phi(b^*b)\Vert.
A simple argument for (2) is as follows. Consider the positive matrix

M= \begin{bmatrix} a^* & 0 \\ b^* & 0 \end{bmatrix} \begin{bmatrix} a & b \\ 0 & 0 \end{bmatrix} = \begin{bmatrix} a^*a & a^* b \\ b^*a & b^*b \end{bmatrix}.
By 2positivity of Φ,

(I_2 \otimes \Phi) M = \begin{bmatrix} \Phi(a^*a) & \Phi(a^* b) \\ \Phi(b^*a) & \Phi(b^*b) \end{bmatrix}
is positive. The desired inequality then follows from the properties of positive 2 × 2 (operator) matrices.
Part (1) is analogous. One can replace the matrix \begin{bmatrix} a & b \\ 0 & 0 \end{bmatrix} by \begin{bmatrix} 1 & a \\ 0 & 0 \end{bmatrix}.
Reforming CauchySchwarz Inequality for cross product
Theorem. Let u and v be nonzero vectors, then:

\ \mathbf{v} \times \mathbf{u} \ \leq \\mathbf{v}\ \cdot \\mathbf{u}\.
To prove this inequality we first write the outer product magnitude as

\ \mathbf{v} \times \mathbf{u} \ = \\mathbf{v}\ \cdot \ \mathbf{u} \ \cdot \sin(\mathbf{v} , \mathbf{u})
Dividing both sides by the product of the magnitudes we arrive at:

\frac{\ \mathbf{v} \times \mathbf{u} \}{\\mathbf{v}\ \cdot \ \mathbf{u} \} = \sin(\mathbf{v} , \mathbf{u}) \leq 1.
The last line follows from the fact that \sin{(\mathbf{v} , \mathbf{u})} \in [1,1].
Physics
The general formulation of the Heisenberg uncertainty principle is derived using the Cauchy–Schwarz inequality.
See also
Notes

^ ^{a} ^{b} The Cauchy–Schwarz Master Class: an Introduction to the Art of Mathematical Inequalities, Ch. 1 by J. Michael Steele.

^ Strang, Gilbert (19 July 2005). "3.2". Linear Algebra and its Applications (4th ed.). Stamford, CT: Cengage Learning. pp. 154–155.

^ Paulsen (2002), Completely Bounded Maps and Operator Algebras, page 40.
References

Bityutskov, V.I. (2001), "Bunyakovskii inequality", in Hazewinkel, Michiel,


Cauchy, A. (1821), Oeuvres 2, III, p. 373

Dragomir, S. S. (2003), "A survey on Cauchy–Bunyakovsky–Schwarz type discrete inequalities", JIPAM. J. Inequal. Pure Appl. Math. 4 (3): 142 pp

.

Lohwater, Arthur (1982), Introduction to Inequalities, Online ebook in PDF fomat

Paulsen, V. (2003), Completely Bounded Maps and Operator Algebras, Cambridge University Press .

Schwarz, H. A. (1888), "Über ein Flächen kleinsten Flächeninhalts betreffendes Problem der Variationsrechnung" (PDF), Acta Societatis scientiarum Fennicae XV: 318

Solomentsev, E.D. (2001), "Cauchy inequality", in Hazewinkel, Michiel,

Steele, J.M. (2004), The Cauchy–Schwarz Master Class, Cambridge University Press,
External links

Earliest Uses: The entry on the Cauchy–Schwarz inequality has some historical information.

Example of application of Cauchy–Schwarz inequality to determine Linearly Independent Vectors Tutorial and Interactive program.
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