An Orthonormal basis is defined as a basis of a finite-dimensional vector space that’s orthonormal. Additional Information orthonormal list of the right length is a basis An orthonormal list is linearly independent, and linearly independent list of length dim V are a basis of V. \blacksquare Writing a vector as a linear combination of orthonormal basis According to Axler, this result is why there’s so much hoopla about orthonormal basis. Result and Motivation For any basis of V, and a vector v \in V, we by basis spanning have:
Yet, for orthonormal basis, we can actually very easily know what the a_{j} are (and not just that some a_{j} exist). Specifically:
That is, for orthonormal basis e_{j} of V, we have that:
for all v \in V. Furthermore:
Proof Given e_{j} are basis (nevermind orthonormal quite yet), we have that:
WLOG let’s take \langle v, e_{j} \rangle:
Given additivity and homogenity in the first slot, we now have:
Of course, each e_{i} and e_{j} are orthogonal, so for the most part a_{i}\langle e_{i}, e_{j} \rangle = 0 for i \neq j. Except where a_{j} \langle e_{j}, e_{j} \rangle = a_{j} 1 = a_{j} because the e vectors are also norm 1. Therefore:
We now have \langle v,e_{j} \rangle = a_{j} WLOG for all j, as desired. Plugging this in for each a_{j} and applying Norm of an Orthogonal Linear Combination yields the \|v\|^{2} equation above. \blacksquare