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Section III. Basis and Dimension 135<br />

and vice versa.<br />

For (1) =⇒ (2), assume that all decompositions are unique. We will show<br />

⌢ ⌢<br />

that B1 ··· Bk spans the space and is linearly independent. It spans the<br />

space because the assumption that V = W1 + ··· + Wk means that every �v<br />

canbeexpressedas�v = �w1 + ···+ �wk, which translates by equation (∗) toan<br />

expression of �v as a linear combination of the � β’s from the concatenation. For<br />

linear independence, consider this linear relationship.<br />

�0 =c1,1 � �βk,nk<br />

β1,1 + ···+ ck,nk<br />

Regroup as in (∗) (that is, take d1, ... , dk to be 1 and move from bottom to<br />

top) to get the decomposition �0 = �w1 + ···+ �wk. Because of the assumption<br />

that decompositions are unique, and because the zero vector obviously has the<br />

decomposition �0 =�0+···+�0, we now have that each �wi is the zero vector. This<br />

means that ci,1 � �βi,ni βi,1 + ···+ ci,ni = �0. Thus, since each Bi is a basis, we have<br />

the desired conclusion that all of the c’s are zero.<br />

⌢ ⌢<br />

For (2) =⇒ (3), assume that B1 ··· Bk is a basis for the space. Consider<br />

a linear relationship among nonzero vectors from different Wi’s,<br />

�0 = ···+ di �wi + ···<br />

in order to show that it is trivial. (The relationship is written in this way<br />

because we are considering a combination of nonzero vectors from only some of<br />

the Wi’s; for instance, there might not be a �w1 in this combination.) As in (∗),<br />

�0 = ···+di(ci,1 � �βi,ni βi,1+···+ci,ni )+··· = ···+dici,1· � βi,1+···+dici,ni ·� βi,ni +···<br />

⌢ ⌢<br />

and the linear independence of B1 ··· Bk gives that each coefficient dici,j is<br />

zero. Now, �wi is a nonzero vector, so at least one of the ci,j’s is zero, and thus<br />

di is zero. This holds for each di, and therefore the linear relationship is trivial.<br />

Finally, for (3) =⇒ (1), assume that, among nonzero vectors from different<br />

Wi’s, any linear relationship is trivial. Consider two decompositions of a vector<br />

�v = �w1 + ···+ �wk and �v = �u1 + ···+ �uk in order to show that the two are the<br />

same. We have<br />

�0 =(�w1 + ···+ �wk) − (�u1 + ···+ �uk) =(�w1 − �u1)+···+(�wk − �uk)<br />

which violates the assumption unless each �wi − �ui is the zero vector. Hence,<br />

decompositions are unique. QED<br />

4.9 Definition A collection of subspaces {W1,... ,Wk} is independent if no<br />

nonzero vector from any Wi is a linear combination of vectors from the other<br />

subspaces W1,...,Wi−1,Wi+1,...,Wk.<br />

4.10 Definition A vector space V is the direct sum (or internal direct sum)<br />

of its subspaces W1,...,Wk if V = W1 + W2 + ··· + Wk and the collection<br />

{W1,...,Wk} is independent. We write V = W1 ⊕ W2 ⊕ ...⊕ Wk.<br />

4.11 Example The benchmark model fits: R 3 = x-axis ⊕ y-axis ⊕ z-axis.

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