Mathematics · Glossary

What is free family?

Also known as: basis

Definition 18.14 University Mathematics — Year 1 · Chapter 18 — Vector Spaces

A family (x1,,xp)(x_1, \dots, x_p) of vectors of EE is:

  • generating (of EE) when Vect(x1,,xp)=E\operatorname{Vect}(x_1,\dots,x_p) = E;
  • free (its vectors linearly independent) when

    λ1x1++λpxp=0    λ1==λp=0;\lambda_1 x_1 + \dots + \lambda_p x_p = 0 \implies \lambda_1 = \dots = \lambda_p = 0 ;

    otherwise linked;

  • a basis when it is free and generating.

Examples

Example 18.16

The canonical basis of KnK^n: ei=(0,,1,,0)e_i = (0, \dots, 1, \dots, 0) (11 in slot ii). The monomials (1,X,X2,,Xn)(1, X, X^2, \dots, X^n): a basis of Kn[X]K_n[X] (freeness: a null combination is the zero polynomial, so all coefficients vanish, Definition 8.1). In C\C over R\R: the basis (1,i)(1, \iu).

Example 18.18 (Testing a candidate basis, start to finish)

Is F=(1+X, 1+X2, X+X2)\mathcal{F} = (1 + X,\ 1 + X^2,\ X + X^2) a basis of R2[X]\R_2[X]? Write u1,u2,u3u_1, u_2, u_3 for the three polynomials. Freeness: a null combination au1+bu2+cu3=0a\,u_1 + b\,u_2 + c\,u_3 = 0 gives, coefficient by coefficient,

a+b=0,a+c=0,b+c=0;a + b = 0, \qquad a + c = 0, \qquad b + c = 0 ;

subtracting the first two, b=cb = c, then the third gives 2b=02b = 0: a=b=c=0a = b = c = 0, free. Generating: instead of solving three systems, notice the symmetric combination

u1+u2u3=(1+X)+(1+X2)(X+X2)=2,u_1 + u_2 - u_3 = (1 + X) + (1 + X^2) - (X + X^2) = 2 ,

so 1=12(u1+u2u3)1 = \frac12(u_1 + u_2 - u_3); then

X=u11=12(u1u2+u3),X2=u21=12(u1+u2+u3).X = u_1 - 1 = \tfrac12\bigl(u_1 - u_2 + u_3\bigr), \qquad X^2 = u_2 - 1 = \tfrac12\bigl(-u_1 + u_2 + u_3\bigr).

The monomials lie in the span, so everything does: F\mathcal{F} is a basis. As a bonus, assembling the three displays gives the coordinates of any P=α+βX+γX2P = \alpha + \beta X + \gamma X^2:

P=α+βγ2u1+αβ+γ2u2+α+β+γ2u3.P = \frac{\alpha + \beta - \gamma}{2}\,u_1 + \frac{\alpha - \beta + \gamma}{2}\,u_2 + \frac{-\alpha + \beta + \gamma}{2}\,u_3 .

(Sanity check with P=XP = X: coordinates (12,12,12)\bigl(\frac12, -\frac12, \frac12\bigr), as found above.) Two lessons: symmetry in the family usually hides a shortcut combination; and once dimension is available (Chapter 19), the whole generating half of this work will come free of charge — three free vectors of a 33-dimensional space always form a basis.

Example 18.20 (The staircase principle)

Let P0,P1,,PnKn[X]P_0, P_1, \dots, P_n \in K_n[X] with degPk=k\deg P_k = k for each kk (a “staircase” of degrees). Then (P0,,Pn)(P_0, \dots, P_n) is a basis of Kn[X]K_n[X]. Freeness is Proposition 18.19 (1). For the generating property, argue by finite descent on the degree: let QKn[X]Q \in K_n[X], Q0Q \neq 0, of degree dd, with leading coefficient aa, and let b0b \neq 0 be the leading coefficient of PdP_d. Then QabPdQ - \frac ab P_d has degree <d< d (the top terms cancel); replacing QQ by this difference and iterating, after at most n+1n + 1 steps one reaches the zero polynomial, and unwinding the subtractions expresses QQ as a combination of the PkP_k. Two staircases already met: the shifted powers ((Xa)k)0kn\bigl((X-a)^k\bigr)_{0 \leq k \leq n} (Exercise 18.4), and the Newton products ((Xx0)(Xx1)(Xxk1))0kn\bigl((X - x_0)(X - x_1)\cdots(X - x_{k-1})\bigr)_{0 \leq k \leq n}, put to work in the weekend problem.

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