The parallelogram identity is one of the equalities in vector algebra and vector analysis .
Content
In Euclidean geometry
The sum of the squared lengths of the sides of the parallelogram is the sum of the squared lengths of its diagonals .
In spaces with scalar product
In vector spaces with a scalar product, this identity looks like this [1] :
Where
In normed spaces (polarization identity)
In the normed space ( V , ), for which the parallelogram identity holds, we can introduce the scalar product generating this norm, that is, such that all vectors of space . This theorem is attributed to Frechet , von Neumann and Jordan [2] [3] . This can be done in the following way:
- for real space
- or or
- for complex space
The above formulas expressing the scalar product of two vectors in terms of the norm are called the polarization identity .
Obviously, the norm expressed in terms of any scalar product as follows will satisfy this identity.
Polarization identity is often used to turn Banach spaces into Hilbert spaces .
Summary
If B is a symmetric bilinear form in a vector space, and the quadratic form Q is expressed as
- ,
then
Notes
- ↑ Shilov, 1961 , p. 185.
- ↑ Philippe Blanchard, Erwin Brüning. Proposition 14.1.2 (Fréchet – von Neumann – Jordan) // Mathematical methods in physics: distributions, Hilbert space operators, and variational methods . - Birkhäuser, 2003 .-- P. 192. - ISBN 0817642285 .
- ↑ Gerald Teschl. Theorem 0.19 (Jordan – von Neumann) // Mathematical methods in quantum mechanics: with applications to Schrödinger operators . - American Mathematical Society Bookstore, 2009. - P. 19. - ISBN 0-8218-4660-4 .
Links
Literature
- Shilov G.E. Mathematical analysis. Special course. - M .: Nauka, 1961 .-- 436 p.