Any inner product on a vector space induces a norm by the equation $${\displaystyle \|x\|={\sqrt {\langle x,x\rangle }}.}$$  The polarization identities reverse this relationship, recovering the inner product from the norm. Every inner product satisfies: $${\displaystyle \|x+y\|^{2}=\|x\|^{2}+\|y\|^{2}+2\operatorname {Re} \langle x,y\rangle \qquad {\text{ for all vectors }}x,y.}$$ 

Solving for ${\displaystyle \operatorname {Re} \langle x,y\rangle }$  gives the formula ${\displaystyle \operatorname {Re} \langle x,y\rangle ={\frac {1}{2}}\left(\|x+y\|^{2}-\|x\|^{2}-\|y\|^{2}\right).}$  If the inner product is real then ${\displaystyle \operatorname {Re} \langle x,y\rangle =\langle x,y\rangle }$  and this formula becomes a polarization identity for real inner products.

If the vector space is over the real numbers then the polarization identities are:^[4] $${\displaystyle {\begin{alignedat}{4}\langle x,y\rangle &={\frac {1}{4}}\left(\|x+y\|^{2}-\|x-y\|^{2}\right)\\[3pt]&={\frac {1}{2}}\left(\|x+y\|^{2}-\|x\|^{2}-\|y\|^{2}\right)\\[3pt]&={\frac {1}{2}}\left(\|x\|^{2}+\|y\|^{2}-\|x-y\|^{2}\right).\\[3pt]\end{alignedat}}}$$ 

These various forms are all equivalent by the parallelogram law:^{[proof 1]} $${\displaystyle 2\|x\|^{2}+2\|y\|^{2}=\|x+y\|^{2}+\|x-y\|^{2}.}$$ 

This further implies that ${\displaystyle L^{p}}$  class is not a Hilbert space whenever ⁠${\displaystyle p\neq 2}$ ⁠, as the parallelogram law is not satisfied. For the sake of counterexample, consider ${\displaystyle x=1_{A}}$  and ${\displaystyle y=1_{B}}$  for any two disjoint subsets ${\displaystyle A,B}$  of general domain ${\displaystyle \Omega \subset \mathbb {R} ^{n}}$  and compute the measure of both sets under parallelogram law.

For vector spaces over the complex numbers, the above formulas are not quite correct because they do not describe the imaginary part of the (complex) inner product. However, an analogous expression does ensure that both real and imaginary parts are retained. The complex part of the inner product depends on whether it is antilinear in the first or the second argument. The notation ${\displaystyle \langle x|y\rangle ,}$  which is commonly used in physics will be assumed to be antilinear in the first argument while ${\displaystyle \langle x,\,y\rangle ,}$  which is commonly used in mathematics, will be assumed to be antilinear in its second argument. They are related by the formula: $${\displaystyle \langle x,\,y\rangle =\langle y\,|\,x\rangle \quad {\text{ for all }}x,y\in H.}$$ 

The real part of any inner product (no matter which argument is antilinear and no matter if it is real or complex) is a symmetric bilinear map that for any ${\displaystyle x,y\in H}$  is always equal to:^{[4][proof 1]} $${\displaystyle {\begin{alignedat}{4}R(x,y):&=\operatorname {Re} \langle x\mid y\rangle =\operatorname {Re} \langle x,y\rangle \\&={\frac {1}{4}}\left(\|x+y\|^{2}-\|x-y\|^{2}\right)\\&={\frac {1}{2}}\left(\|x+y\|^{2}-\|x\|^{2}-\|y\|^{2}\right)\\[3pt]&={\frac {1}{2}}\left(\|x\|^{2}+\|y\|^{2}-\|x-y\|^{2}\right).\\[3pt]\end{alignedat}}}$$ 

It is always a symmetric map, meaning that^{[proof 1]} $${\displaystyle R(x,y)=R(y,x)\quad {\text{ for all }}x,y\in H,}$$  and it also satisfies:^{[proof 1]} $${\displaystyle R(ix,y)=-R(x,iy)\quad {\text{ for all }}x,y\in H,}$$  which in plain English says that to move a factor of ${\displaystyle i}$  to the other argument, introduce a negative sign. These properties can be proven either from the properties of inner products directly or from properties of norms by using the polarization identity.

Unlike its real part, the imaginary part of a complex inner product depends on which argument is antilinear.

Antilinear in first argument

The polarization identities for the inner product ${\displaystyle \langle x\,|\,y\rangle ,}$  which is antilinear in the first argument, are

${\displaystyle {\begin{alignedat}{4}\langle x\,|\,y\rangle &={\frac {1}{4}}\left(\|x+y\|^{2}-\|x-y\|^{2}-i\|x+iy\|^{2}+i\|x-iy\|^{2}\right)\\&={\frac {1}{4}}\sum _{k=0}^{3}i^{k}\|x+(-i)^{k}y\|^{2}\\&=R(x,y)-iR(x,iy)\\&=R(x,y)+iR(ix,y)\\\end{alignedat}}}$ 

where ${\displaystyle x,y\in H.}$  The second to last equality is similar to the formula expressing a linear functional ${\displaystyle \varphi }$  in terms of its real part: ${\displaystyle \varphi (y)=\operatorname {Re} \varphi (y)-i(\operatorname {Re} \varphi )(iy).}$ 

Antilinear in second argument

The polarization identities for the inner product ${\displaystyle \langle x,\ y\rangle ,}$  which is antilinear in the second argument, follows from that of ${\displaystyle \langle x\,|\,y\rangle }$  by the relationship: ${\displaystyle \langle x,\ y\rangle :=\langle y\,|\,x\rangle ={\overline {\langle x\,|\,y\rangle }}\quad {\text{ for all }}x,y\in H.}$  So for any ${\displaystyle x,y\in H,}$ ^[4]

${\displaystyle {\begin{alignedat}{4}\langle x,\,y\rangle &={\frac {1}{4}}\left(\|x+y\|^{2}-\|x-y\|^{2}+i\|x+iy\|^{2}-i\|x-iy\|^{2}\right)\\&=R(x,y)+iR(x,iy)\\&=R(x,y)-iR(ix,y).\\\end{alignedat}}}$ 

This expression can be phrased symmetrically as:^[5] $${\displaystyle \langle x,y\rangle ={\frac {1}{4}}\sum _{k=0}^{3}i^{k}\left\|x+i^{k}y\right\|^{2}.}$$ 

Summary of both cases

Thus if ${\displaystyle R(x,y)+iI(x,y)}$  denotes the real and imaginary parts of some inner product's value at the point ${\displaystyle (x,y)\in H\times H}$  of its domain, then its imaginary part will be: $${\displaystyle I(x,y)~=~{\begin{cases}~R({\color {red}i}x,y)&\qquad {\text{ if antilinear in the }}{\color {red}1}{\text{st argument}}\\~R(x,{\color {blue}i}y)&\qquad {\text{ if antilinear in the }}{\color {blue}2}{\text{nd argument}}\\\end{cases}}}$$  where the scalar ${\displaystyle i}$  is always located in the same argument that the inner product is antilinear in.

Using ⁠${\displaystyle R(ix,y)=-R(x,iy)}$ ⁠, the above formula for the imaginary part becomes: $${\displaystyle I(x,y)~=~{\begin{cases}-R(x,{\color {black}i}y)&\qquad {\text{ if antilinear in the }}{\color {black}1}{\text{st argument}}\\-R({\color {black}i}x,y)&\qquad {\text{ if antilinear in the }}{\color {black}2}{\text{nd argument}}\\\end{cases}}}$$ 

In a normed space ${\displaystyle (H,\|\cdot \|),}$  if the parallelogram law $${\displaystyle \|x+y\|^{2}~+~\|x-y\|^{2}~=~2\|x\|^{2}+2\|y\|^{2}}$$  holds, then there exists a unique inner product ${\displaystyle \langle \cdot ,\ \cdot \rangle }$  on ${\displaystyle H}$  such that ${\displaystyle \|x\|^{2}=\langle x,\ x\rangle }$  for all ${\displaystyle x\in H.}$ ^[4][1]

Another necessary and sufficient condition for there to exist an inner product that induces a given norm ${\displaystyle \|\cdot \|}$  is for the norm to satisfy Ptolemy's inequality, which is:^[6] $${\displaystyle \|x-y\|\,\|z\|~+~\|y-z\|\,\|x\|~\geq ~\|x-z\|\,\|y\|\qquad {\text{ for all vectors }}x,y,z.}$$ 

If ${\displaystyle H}$  is a complex Hilbert space then ${\displaystyle \langle x\mid y\rangle }$  is real if and only if its imaginary part is ⁠${\displaystyle 0=R(x,iy)={\frac {1}{4}}\left(\Vert x+iy\Vert ^{2}-\Vert x-iy\Vert ^{2}\right)}$ ⁠, which happens if and only if ⁠${\displaystyle \Vert x+iy\Vert =\Vert x-iy\Vert }$ ⁠. Similarly, ${\displaystyle \langle x\mid y\rangle }$  is (purely) imaginary if and only if ⁠${\displaystyle \Vert x+y\Vert =\Vert x-y\Vert }$ ⁠. For example, from ${\displaystyle \|x+ix\|=|1+i|\|x\|={\sqrt {2}}\|x\|=|1-i|\|x\|=\|x-ix\|}$  it can be concluded that ${\displaystyle \langle x|x\rangle }$  is real and that ${\displaystyle \langle x|ix\rangle }$  is purely imaginary.

If ${\displaystyle A:H\to Z}$  is a linear isometry between two Hilbert spaces (so ${\displaystyle \|Ah\|=\|h\|}$  for all ${\displaystyle h\in H}$ ) then $${\displaystyle \langle Ah,Ak\rangle _{Z}=\langle h,k\rangle _{H}\quad {\text{ for all }}h,k\in H;}$$  that is, linear isometries preserve inner products.

If ${\displaystyle A:H\to Z}$  is instead an antilinear isometry then $${\displaystyle \langle Ah,Ak\rangle _{Z}={\overline {\langle h,k\rangle _{H}}}=\langle k,h\rangle _{H}\quad {\text{ for all }}h,k\in H.}$$ 

The second form of the polarization identity can be written as $${\displaystyle \|{\textbf {u}}-{\textbf {v}}\|^{2}=\|{\textbf {u}}\|^{2}+\|{\textbf {v}}\|^{2}-2({\textbf {u}}\cdot {\textbf {v}}).}$$ 

This is essentially a vector form of the law of cosines for the triangle formed by the vectors ⁠${\displaystyle {\textbf {u}}}$ ⁠, ⁠${\displaystyle {\textbf {v}}}$ ⁠, and ⁠${\displaystyle {\textbf {u}}-{\textbf {v}}}$ ⁠. In particular, $${\displaystyle {\textbf {u}}\cdot {\textbf {v}}=\|{\textbf {u}}\|\,\|{\textbf {v}}\|\cos \theta ,}$$  where ${\displaystyle \theta }$  is the angle between the vectors ${\displaystyle {\textbf {u}}}$  and ⁠${\displaystyle {\textbf {v}}}$ ⁠.

The equation is numerically unstable if u and v are similar because of catastrophic cancellation and should be avoided for numeric computation.

The basic relation between the norm and the dot product is given by the equation $${\displaystyle \|{\textbf {v}}\|^{2}={\textbf {v}}\cdot {\textbf {v}}.}$$ 

Then $${\displaystyle {\begin{aligned}\|{\textbf {u}}+{\textbf {v}}\|^{2}&=({\textbf {u}}+{\textbf {v}})\cdot ({\textbf {u}}+{\textbf {v}})\\[3pt]&=({\textbf {u}}\cdot {\textbf {u}})+({\textbf {u}}\cdot {\textbf {v}})+({\textbf {v}}\cdot {\textbf {u}})+({\textbf {v}}\cdot {\textbf {v}})\\[3pt]&=\|{\textbf {u}}\|^{2}+\|{\textbf {v}}\|^{2}+2({\textbf {u}}\cdot {\textbf {v}}),\end{aligned}}}$$  and similarly $${\displaystyle \|{\textbf {u}}-{\textbf {v}}\|^{2}=\|{\textbf {u}}\|^{2}+\|{\textbf {v}}\|^{2}-2({\textbf {u}}\cdot {\textbf {v}}).}$$ 

Forms (1) and (2) of the polarization identity now follow by solving these equations for ⁠${\displaystyle {\textbf {u}}\cdot {\textbf {v}}}$ ⁠, while form (3) follows from subtracting these two equations. (Adding these two equations together gives the parallelogram law.)

The standard Jordan–von Neumann theorem, as stated previously, is that the if a norm satisfies the parallelogram law, then it can be induced by an inner product defined by the polarization identity. There are variants of the theorem.^[7]

Define various senses of orthogonality:

• isosceles: ${\textstyle \|x+y\|=\|x-y\|}$ 
• Roberts’: ${\textstyle \left\|x+ty\right\|=\left\|x-ty\right\|}$  for all scalar ${\textstyle t}$ .
• Pythagorean: ${\textstyle \left\|x+y\right\|^{2}=\|x\|^{2}+\left\|y\right\|^{2}}$ 
• Birkhoff–James: ${\textstyle \|x\|\leq \|x+ty\|}$  for all scalar ${\textstyle t}$ .

Let ${\textstyle V}$  be a vector space over the real or complex numbers. Let ${\textstyle \|\cdot \|}$  be a norm over ${\textstyle V}$ . We consider conditions for which the norm is induced by an inner product. In the following statements, whenever a scalar appears, the scalar may be restricted to be merely real, even when ${\textstyle V}$  is over the complex numbers.

• (von Neumann–Jordan condition) The norm satisfies the parallelogram identity.
• (weakened von Neumann–Jordan condition) ${\textstyle \|x+y\|^{2}+\|x-y\|^{2}=4}$  for all unit vectors ${\textstyle x,y}$ . That is, the norm satisfies the parallelogram identity for unit vectors.
• For any ${\textstyle x,y\in V}$ , the set of points equidistant to ${\textstyle x,y}$  is flat, that is, an affine subspace.
• Orthogonality in either isosceles or Roberts’ sense is either additive or homogeneous on one variable.
• For every two-dimensional subspace ${\textstyle W\subset V}$ , for every ${\textstyle x\in W}$ , there exists ${\textstyle y\in W}$  that is Roberts’ orthogonal to ${\textstyle x}$ .
• Isosceles orthogonality implies Pythagorean orthogonality.
• Pythagorean orthogonality implies isosceles orthogonality.
• If ${\textstyle x,y}$  are Pythagorean orthogonal, then so are ${\textstyle x,-y}$ .
• Birkhoff–James orthogonality is symmetric.
• If ${\textstyle \|x\|=\|y\|}$  and ${\textstyle t,s}$  are real, then ${\textstyle \|tx+sy\|=\|sx+ty\|}$ .

For the real vector space, there is also the condition:

• Any two-dimensional slice of the unit sphere is an ellipse, that is, parameterizable as ${\textstyle \{x\cos \theta +y\sin \theta :\theta \in [0,2\pi ]\}}$ , for some unit vectors ${\textstyle x,y}$ .

The Banach-Mazur rotation problem: Given a separable Banach space ${\textstyle V}$  such that for any two unit vectors ${\textstyle x,y,}$  there exists a linear surjective isometry ${\textstyle T}$  such that ${\textstyle T(x)=y}$  or ${\textstyle T(y)=x}$ , is ${\textstyle V}$  isometrically isomorphic to a Hilbert space?

The general case of the problem is open. When the space is parable finite-dimensional, the answer is yes. In other words, given a finite-dimensional normed vector space over the real or complex numbers, if any point on the unit sphere can be mapped (rotated) to any other point by a linear isometry, then the norm is induced by an inner product.^[8]

The polarization identities are not restricted to inner products. If ${\displaystyle B}$  is any symmetric bilinear form on a vector space, and ${\displaystyle Q}$  is the quadratic form defined by $${\displaystyle Q(v)=B(v,v),}$$  then $${\displaystyle {\begin{aligned}2B(u,v)&=Q(u+v)-Q(u)-Q(v),\\2B(u,v)&=Q(u)+Q(v)-Q(u-v),\\4B(u,v)&=Q(u+v)-Q(u-v).\end{aligned}}}$$ 

The so-called symmetrization map generalizes the latter formula, replacing ${\displaystyle Q}$  by a homogeneous polynomial of degree ${\displaystyle k}$  defined by ${\displaystyle Q(v)=B(v,\ldots ,v),}$  where ${\displaystyle B}$  is a symmetric ${\displaystyle k}$ -linear map.^[9]

The formulas above even apply in the case where the field of scalars has characteristic two, though the left-hand sides are all zero in this case. Consequently, in characteristic two there is no formula for a symmetric bilinear form in terms of a quadratic form, and they are in fact distinct notions, a fact which has important consequences in L-theory; for brevity, in this context "symmetric bilinear forms" are often referred to as "symmetric forms".

These formulas also apply to bilinear forms on modules over a commutative ring, though again one can only solve for ${\displaystyle B(u,v)}$  if 2 is invertible in the ring, and otherwise these are distinct notions. For example, over the integers, one distinguishes integral quadratic forms from integral symmetric forms, which are a narrower notion.

More generally, in the presence of a ring involution or where 2 is not invertible, one distinguishes ${\displaystyle \varepsilon }$ -quadratic forms and ${\displaystyle \varepsilon }$ -symmetric forms; a symmetric form defines a quadratic form, and the polarization identity (without a factor of 2) from a quadratic form to a symmetric form is called the "symmetrization map", and is not in general an isomorphism. This has historically been a subtle distinction: over the integers it was not until the 1950s that relation between "twos out" (integral quadratic form) and "twos in" (integral symmetric form) was understood – see discussion at integral quadratic form; and in the algebraization of surgery theory, Mishchenko originally used symmetric L-groups, rather than the correct quadratic L-groups (as in Wall and Ranicki) – see discussion at L-theory.

Finally, in any of these contexts these identities may be extended to homogeneous polynomials (that is, algebraic forms) of arbitrary degree, where it is known as the polarization formula, and is reviewed in greater detail in the article on the polarization of an algebraic form.

• Inner product space – Vector space with generalized dot product
• Law of cosines – Generalization of Pythagorean theorem
• Mazur–Ulam theorem – Surjective isometries are affine mappings
• Minkowski distance – Vector distance using pth powers
• Parallelogram law – Sides and diagonals have equal sums of squares
• Ptolemy's inequality – Relation between distances of four points

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• Schechter, Eric (1996). Handbook of Analysis and Its Foundations. San Diego, CA: Academic Press. ISBN 978-0-12-622760-4. OCLC 175294365.