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CHAPTER II DIMENSION In the present chapter we investigate ...

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So, for each v, <strong>the</strong>re is a vector u in V such that T u = v. Here u is uniquely<br />

determined by v. To see this, assume <strong>the</strong>re is ano<strong>the</strong>r vector w such that T w = v.<br />

Then T (u − w) = T u − T w = v − v = 0. This shows that u − w is in ker T . The<br />

assumption, ker T = {0} tells us that u − w = 0 and hence u = w. Now <strong>we</strong> can define<br />

<strong>the</strong> inverse T −1 of T by putting T −1 v = u if T u = v holds. We have proved<br />

Corollary 2.4.2. If T is a linear operator on a finite dimensional space V with<br />

ker T = {0}, <strong>the</strong>n T is invertible.<br />

The argument for proving <strong>the</strong> above corollary also shows<br />

Corollary 2.4.3. If T is a linear mapping on a finite dimensional space V into<br />

itself and if <strong>the</strong> homogeneous equation T x = 0 has no nontrivial solution, <strong>the</strong>n, for any<br />

vector b in V , <strong>the</strong> equation T x = b has a unique solution.<br />

Corollary 2.4.4. If M is an m × n matrix with m < n, <strong>the</strong>n <strong>the</strong> homogeneous<br />

equation Ax = 0 has nontrivial solutions. (Notice that m is <strong>the</strong> number of equations and<br />

n is <strong>the</strong> number of unknowns in <strong>the</strong> system of equations in vector form Ax = 0.)<br />

Proof. Define <strong>the</strong> linear map T : C n → C m by putting T x = Ax (in o<strong>the</strong>r<br />

words, T = MA). Then dim ker T + dim T (C n ) = dim C n = n. On <strong>the</strong> o<strong>the</strong>r hand,<br />

since T (C n ) is a subspace of C m and dim C m = m, <strong>we</strong> have dim T (C n ) ≤ m. Thus<br />

dim ker T = dim C n − dim T (C n ) ≥ n − m > 0. Hence ker T = {0}. Any nonzero vector<br />

in ker T gives a nontrivial solution to Ax = 0.<br />

Let A = [A1 A2 · · · An] be an m × n matrix. As usual, <strong>we</strong> study <strong>the</strong> homogeneous<br />

equation Ax = 0 by introducing <strong>the</strong> linear map T : C n → C m . A solution of this equation<br />

is just a vector in <strong>the</strong> kernel of T . So <strong>the</strong> dimension of <strong>the</strong> solution space is <strong>the</strong> nullity of<br />

T , which is also <strong>the</strong> number of parameters needed in writing down <strong>the</strong> general solution.<br />

The rank of A is defined to be <strong>the</strong> rank of T , which is <strong>the</strong> dimension of <strong>the</strong> range T (V )<br />

of V . From <strong>the</strong>n identity<br />

⎢<br />

T x = Ax = [A1 A2 · · · An] ⎢<br />

⎣<br />

⎡<br />

x1<br />

x2<br />

.<br />

xn<br />

⎤<br />

⎥<br />

⎦ = A1x1 + A2x2 + · · · + Anxn<br />

<strong>we</strong> see that <strong>the</strong> range of T is just <strong>the</strong> column space of A, that is, <strong>the</strong> linear span of<br />

<strong>the</strong> column vectors A1, A2, . . . , An of <strong>the</strong> matrix A. The leading vectors of this list of<br />

column vectors is a basis of <strong>the</strong> column space of A. The number of <strong>the</strong> leading vectors is<br />

<strong>the</strong> rank of A. Recall that leading vectors can be identified by <strong>the</strong> echelon form of A.<br />

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