Linear-Algebra-Done-Right Β· Unit 15 Β· Video 3 Β· Interactive Practice
Linear Functionals and the Riesz Representation Theorem
I Key Formulas
Key Insight: The right side of (R) seems to depend on the orthonormal basis, but uniqueness says v v v is determined by Ο \varphi Ο alone β every orthonormal basis gives the same sum.
II Visualization 1 β Formula (R) Ignores the Basis
For Ο ( x , y ) = 2 x + y \varphi(x, y) = 2x + y Ο ( x , y ) = 2 x + y on R 2 \mathbf{R}^2 R 2 , every orthonormal basis builds the same vector v = ( 2 , 1 ) v = (2, 1) v = ( 2 , 1 ) .
III Visualization 2 β Why Formula (R) Needs the Bar
On C 2 \mathbf{C}^2 C 2 , Ο ( z 1 , z 2 ) = Ξ» z 1 + 2 z 2 \varphi(z_1, z_2) = \lambda z_1 + 2z_2 Ο ( z 1 β , z 2 β ) = Ξ» z 1 β + 2 z 2 β is represented by v = ( Ξ» βΎ , 2 ) v = (\overline{\lambda}, 2) v = ( Ξ» , 2 ) , not by ( Ξ» , 2 ) (\lambda, 2) ( Ξ» , 2 ) .
π‘ Challenge: find every Ξ» \lambda Ξ» for which ( Ξ» , 2 ) (\lambda, 2) ( Ξ» , 2 ) also represents Ο \varphi Ο , so that dropping the bar does no harm.
IV Visualization 3 β Same Integral, Different Function
Against every p β P 2 ( R ) p \in \mathcal{P}_2(\mathbf{R}) p β P 2 β ( R ) , the parabola q q q and cos β‘ ( Ο t ) \cos(\pi t) cos ( Ο t ) have the same integral β beyond P 2 ( R ) \mathcal{P}_2(\mathbf{R}) P 2 β ( R ) they need not.
π‘ The representing vector depends on the space: on P 5 ( R ) \mathcal{P}_5(\mathbf{R}) P 5 β ( R ) the same Ο \varphi Ο is represented by a polynomial of degree four, not by q q q .
V Quiz Questions
Problem 1 Β· Formula (R) in a Rotated Basis
Given: Ο ( x , y ) = x + 3 y \varphi(x, y) = x + 3y Ο ( x , y ) = x + 3 y on R 2 \mathbf{R}^2 R 2 with the Euclidean inner product, and the orthonormal basis e 1 = 1 2 ( 1 , 1 ) e_1 = \tfrac{1}{\sqrt2}(1, 1) e 1 β = 2 β 1 β ( 1 , 1 ) , e 2 = 1 2 ( 1 , β 1 ) e_2 = \tfrac{1}{\sqrt2}(1, -1) e 2 β = 2 β 1 β ( 1 , β 1 ) . Find v = Ο ( e 1 ) e 1 + Ο ( e 2 ) e 2 v = \varphi(e_1)e_1 + \varphi(e_2)e_2 v = Ο ( e 1 β ) e 1 β + Ο ( e 2 β ) e 2 β .
a v = ( 2 2 , β 2 ) v = (2\sqrt2, -\sqrt2) v = ( 2 2 β , β 2 β )
b v = ( 2 , 6 ) v = (2, 6) v = ( 2 , 6 )
c v = ( 1 , 3 ) v = (1, 3) v = ( 1 , 3 )
d v = ( 3 , 1 ) v = (3, 1) v = ( 3 , 1 )
β
Correct! The rotated basis gives back
( 1 , 3 ) (1, 3) ( 1 , 3 ) , the coefficient vector of
Ο \varphi Ο β as uniqueness demands.
β Not quite. ( 2 2 , β 2 ) (2\sqrt2, -\sqrt2) ( 2 2 β , β 2 β ) lists the numbers
Ο ( e 1 ) , Ο ( e 2 ) \varphi(e_1), \varphi(e_2) Ο ( e 1 β ) , Ο ( e 2 β ) ; formula (R) still has to multiply them by
e 1 e_1 e 1 β and
e 2 e_2 e 2 β and add.
β Close, butβ¦ that is what
( 1 , 1 ) (1, 1) ( 1 , 1 ) and
( 1 , β 1 ) (1, -1) ( 1 , β 1 ) give before normalizing. Formula (R) needs an
orthonormal basis; with unnormalized vectors each term is off by the factor
β₯ e k β₯ 2 = 2 \|e_k\|^2 = 2 β₯ e k β β₯ 2 = 2 .
β Not quite. Compute
Ο ( e 1 ) = 4 2 \varphi(e_1) = \tfrac{4}{\sqrt2} Ο ( e 1 β ) = 2 β 4 β and
Ο ( e 2 ) = β 2 2 \varphi(e_2) = -\tfrac{2}{\sqrt2} Ο ( e 2 β ) = β 2 β 2 β , then form
Ο ( e 1 ) e 1 + Ο ( e 2 ) e 2 \varphi(e_1)e_1 + \varphi(e_2)e_2 Ο ( e 1 β ) e 1 β + Ο ( e 2 β ) e 2 β .
Show solution
Everything is real, so the conjugates in (R) do nothing.
Ο ( e 1 ) = 1 2 ( 1 + 3 ) = 2 2 , Ο ( e 2 ) = 1 2 ( 1 β 3 ) = β 2 . \varphi(e_1) = \tfrac{1}{\sqrt2}(1 + 3) = 2\sqrt2, \qquad \varphi(e_2) = \tfrac{1}{\sqrt2}(1 - 3) = -\sqrt2. Ο ( e 1 β ) = 2 β 1 β ( 1 + 3 ) = 2 2 β , Ο ( e 2 β ) = 2 β 1 β ( 1 β 3 ) = β 2 β .
v = 2 2 β
1 2 ( 1 , 1 ) β 2 β
1 2 ( 1 , β 1 ) = ( 2 , 2 ) β ( 1 , β 1 ) = ( 1 , 3 ) . v = 2\sqrt2 \cdot \tfrac{1}{\sqrt2}(1, 1) - \sqrt2 \cdot \tfrac{1}{\sqrt2}(1, -1) = (2, 2) - (1, -1) = (1, 3). v = 2 2 β β
2 β 1 β ( 1 , 1 ) β 2 β β
2 β 1 β ( 1 , β 1 ) = ( 2 , 2 ) β ( 1 , β 1 ) = ( 1 , 3 ) .
Check: β¨ ( x , y ) , ( 1 , 3 ) β© = x + 3 y = Ο ( x , y ) \langle (x, y), (1, 3) \rangle = x + 3y = \varphi(x, y) β¨( x , y ) , ( 1 , 3 )β© = x + 3 y = Ο ( x , y ) . The standard basis gives the same v v v immediately: Ο ( 1 , 0 ) = 1 \varphi(1, 0) = 1 Ο ( 1 , 0 ) = 1 , Ο ( 0 , 1 ) = 3 \varphi(0, 1) = 3 Ο ( 0 , 1 ) = 3 .
Problem 2 Β· The Conjugate Trap
Given: Ο ( z 1 , z 2 ) = ( 2 + i ) z 1 β 3 i β z 2 \varphi(z_1, z_2) = (2 + i)z_1 - 3i\,z_2 Ο ( z 1 β , z 2 β ) = ( 2 + i ) z 1 β β 3 i z 2 β on C 2 \mathbf{C}^2 C 2 with the Euclidean inner product β¨ z , w β© = z 1 w 1 βΎ + z 2 w 2 βΎ \langle z, w \rangle = z_1\overline{w_1} + z_2\overline{w_2} β¨ z , w β© = z 1 β w 1 β β + z 2 β w 2 β β . Find the unique v β C 2 v \in \mathbf{C}^2 v β C 2 with Ο ( z ) = β¨ z , v β© \varphi(z) = \langle z, v \rangle Ο ( z ) = β¨ z , v β© for every z z z .
a v = ( 2 + i , Β β 3 i ) v = (2 + i,\ -3i) v = ( 2 + i , Β β 3 i )
b v = ( 2 β i , Β β 3 i ) v = (2 - i,\ -3i) v = ( 2 β i , Β β 3 i )
c v = ( β 2 β i , Β 3 i ) v = (-2 - i,\ 3i) v = ( β 2 β i , Β 3 i )
d v = ( 2 β i , Β 3 i ) v = (2 - i,\ 3i) v = ( 2 β i , Β 3 i )
β
Correct! β¨ z , ( 2 β i , 3 i ) β© = z 1 ( 2 β i ) βΎ + z 2 3 i βΎ = ( 2 + i ) z 1 β 3 i β z 2 \langle z, (2 - i, 3i) \rangle = z_1\overline{(2 - i)} + z_2\overline{3i} = (2 + i)z_1 - 3i\,z_2 β¨ z , ( 2 β i , 3 i )β© = z 1 β ( 2 β i ) β + z 2 β 3 i = ( 2 + i ) z 1 β β 3 i z 2 β .
β Close, butβ¦ this drops the bars of (R). Then
β¨ z , v β© = ( 2 β i ) z 1 + 3 i β z 2 \langle z, v \rangle = (2 - i)z_1 + 3i\,z_2 β¨ z , v β© = ( 2 β i ) z 1 β + 3 i z 2 β β the second slot conjugates the coefficients, giving a different functional.
β Not quite. Every coordinate gets conjugated, including the purely imaginary one:
β 3 i βΎ = 3 i \overline{-3i} = 3i β 3 i β = 3 i .
β Not quite. Conjugation flips the sign of the imaginary part only:
2 + i βΎ = 2 β i \overline{2 + i} = 2 - i 2 + i β = 2 β i , not
β 2 β i -2 - i β 2 β i .
Show solution
Use (R) with the standard basis: Ο ( e 1 ) = 2 + i \varphi(e_1) = 2 + i Ο ( e 1 β ) = 2 + i and Ο ( e 2 ) = β 3 i \varphi(e_2) = -3i Ο ( e 2 β ) = β 3 i , so
v = ( 2 + i ) βΎ β e 1 + ( β 3 i ) βΎ β e 2 = ( 2 β i , Β 3 i ) . v = \overline{(2 + i)}\,e_1 + \overline{(-3i)}\,e_2 = (2 - i,\ 3i). v = ( 2 + i ) β e 1 β + ( β 3 i ) β e 2 β = ( 2 β i , Β 3 i ) .
Check:
β¨ z , v β© = z 1 ( 2 β i ) βΎ + z 2 ( 3 i ) βΎ = ( 2 + i ) z 1 β 3 i β z 2 = Ο ( z ) . \langle z, v \rangle = z_1\overline{(2 - i)} + z_2\overline{(3i)} = (2 + i)z_1 - 3i\,z_2 = \varphi(z). β¨ z , v β© = z 1 β ( 2 β i ) β + z 2 β ( 3 i ) β = ( 2 + i ) z 1 β β 3 i z 2 β = Ο ( z ) .
The bar in (R) undoes the bar that the second slot applies.
Problem 3 Β· Representing Evaluation at Zero
Given: P 2 ( R ) \mathcal{P}_2(\mathbf{R}) P 2 β ( R ) with β¨ p , q β© = β« β 1 1 p β q \langle p, q \rangle = \int_{-1}^{1} p\,q β¨ p , q β© = β« β 1 1 β p q and orthonormal basis e 1 = 1 2 e_1 = \sqrt{\tfrac12} e 1 β = 2 1 β β , e 2 = 3 2 β x e_2 = \sqrt{\tfrac32}\,x e 2 β = 2 3 β β x , e 3 = 45 8 ( x 2 β 1 3 ) e_3 = \sqrt{\tfrac{45}{8}}\left(x^2 - \tfrac13\right) e 3 β = 8 45 β β ( x 2 β 3 1 β ) . Find the q β P 2 ( R ) q \in \mathcal{P}_2(\mathbf{R}) q β P 2 β ( R ) with p ( 0 ) = β« β 1 1 p β q p(0) = \int_{-1}^{1} p\,q p ( 0 ) = β« β 1 1 β p q for every p β P 2 ( R ) p \in \mathcal{P}_2(\mathbf{R}) p β P 2 β ( R ) .
a q ( x ) = 9 8 β 15 8 x 2 q(x) = \tfrac{9}{8} - \tfrac{15}{8}x^2 q ( x ) = 8 9 β β 8 15 β x 2
b q ( x ) = 1 2 β 15 8 x 2 q(x) = \tfrac{1}{2} - \tfrac{15}{8}x^2 q ( x ) = 2 1 β β 8 15 β x 2
c q ( x ) = 1 2 q(x) = \tfrac{1}{2} q ( x ) = 2 1 β
d q ( x ) = 1 q(x) = 1 q ( x ) = 1
β
Correct! β« β 1 1 q = 1 \int_{-1}^1 q = 1 β« β 1 1 β q = 1 ,
β« β 1 1 x q = 0 \int_{-1}^1 xq = 0 β« β 1 1 β x q = 0 ,
β« β 1 1 x 2 q = 0 \int_{-1}^1 x^2 q = 0 β« β 1 1 β x 2 q = 0 β exactly
p ( 0 ) p(0) p ( 0 ) for
p = 1 , x , x 2 p = 1, x, x^2 p = 1 , x , x 2 .
β Close, butβ¦ you used
Ο ( e 3 ) \varphi(e_3) Ο ( e 3 β ) correctly but multiplied it by
x 2 x^2 x 2 alone. Formula (R) multiplies by all of
e 3 e_3 e 3 β , whose
β 1 3 -\tfrac13 β 3 1 β contributes the constant
5 8 \tfrac58 8 5 β .
β Not quite. e 3 ( 0 ) = 45 8 β
( β 1 3 ) β 0 e_3(0) = \sqrt{\tfrac{45}{8}}\cdot\left(-\tfrac13\right) \neq 0 e 3 β ( 0 ) = 8 45 β β β
( β 3 1 β ) ξ = 0 : the third basis element is not zero at the origin, so its term survives.
β Not quite. β« β 1 1 p β
1 \int_{-1}^{1} p \cdot 1 β« β 1 1 β p β
1 is the integral of
p p p , not
p ( 0 ) p(0) p ( 0 ) : for
p = x 2 p = x^2 p = x 2 it gives
2 3 \tfrac23 3 2 β instead of
0 0 0 .
Show solution
Let Ο ( p ) = p ( 0 ) \varphi(p) = p(0) Ο ( p ) = p ( 0 ) , a linear functional. Over R \mathbf{R} R , formula (R) reads q = Ο ( e 1 ) e 1 + Ο ( e 2 ) e 2 + Ο ( e 3 ) e 3 q = \varphi(e_1)e_1 + \varphi(e_2)e_2 + \varphi(e_3)e_3 q = Ο ( e 1 β ) e 1 β + Ο ( e 2 β ) e 2 β + Ο ( e 3 β ) e 3 β .
Ο ( e 1 ) = 1 2 , Ο ( e 2 ) = 0 , Ο ( e 3 ) = 45 8 ( β 1 3 ) . \varphi(e_1) = \sqrt{\tfrac12}, \qquad \varphi(e_2) = 0, \qquad \varphi(e_3) = \sqrt{\tfrac{45}{8}}\left(-\tfrac13\right). Ο ( e 1 β ) = 2 1 β β , Ο ( e 2 β ) = 0 , Ο ( e 3 β ) = 8 45 β β ( β 3 1 β ) .
q = 1 2 + 45 8 ( β 1 3 ) ( x 2 β 1 3 ) = 1 2 β 15 8 x 2 + 5 8 = 9 8 β 15 8 x 2 . q = \tfrac12 + \tfrac{45}{8}\left(-\tfrac13\right)\left(x^2 - \tfrac13\right) = \tfrac12 - \tfrac{15}{8}x^2 + \tfrac{5}{8} = \tfrac98 - \tfrac{15}{8}x^2. q = 2 1 β + 8 45 β ( β 3 1 β ) ( x 2 β 3 1 β ) = 2 1 β β 8 15 β x 2 + 8 5 β = 8 9 β β 8 15 β x 2 .
Check on 1 , x , x 2 1, x, x^2 1 , x , x 2 : β« β 1 1 q = 9 4 β 5 4 = 1 = p ( 0 ) \int_{-1}^1 q = \tfrac94 - \tfrac54 = 1 = p(0) β« β 1 1 β q = 4 9 β β 4 5 β = 1 = p ( 0 ) for p = 1 p = 1 p = 1 ; β« β 1 1 x q = 0 \int_{-1}^1 xq = 0 β« β 1 1 β x q = 0 (odd integrand); β« β 1 1 x 2 q = 3 4 β 3 4 = 0 \int_{-1}^1 x^2 q = \tfrac34 - \tfrac34 = 0 β« β 1 1 β x 2 q = 4 3 β β 4 3 β = 0 . By linearity it holds for every p p p .
Problem 4 Β· A Sine Functional on P 3 ( R ) \mathcal{P}_3(\mathbf{R}) P 3 β ( R )
Given: Ο ( p ) = β« β 1 1 p ( t ) sin β‘ ( Ο t ) β d t \varphi(p) = \int_{-1}^{1} p(t)\sin(\pi t)\,dt Ο ( p ) = β« β 1 1 β p ( t ) sin ( Ο t ) d t on P 3 ( R ) \mathcal{P}_3(\mathbf{R}) P 3 β ( R ) , with β¨ p , q β© = β« β 1 1 p β q \langle p, q \rangle = \int_{-1}^{1} p\,q β¨ p , q β© = β« β 1 1 β p q and the orthonormal basis e 1 = 1 2 e_1 = \sqrt{\tfrac12} e 1 β = 2 1 β β , e 2 = 3 2 β x e_2 = \sqrt{\tfrac32}\,x e 2 β = 2 3 β β x , e 3 = 45 8 ( x 2 β 1 3 ) e_3 = \sqrt{\tfrac{45}{8}}\left(x^2 - \tfrac13\right) e 3 β = 8 45 β β ( x 2 β 3 1 β ) , e 4 = 14 4 ( 5 x 3 β 3 x ) e_4 = \tfrac{\sqrt{14}}{4}(5x^3 - 3x) e 4 β = 4 14 β β ( 5 x 3 β 3 x ) . You may use β« β 1 1 t sin β‘ ( Ο t ) β d t = 2 Ο \int_{-1}^{1} t\sin(\pi t)\,dt = \tfrac{2}{\pi} β« β 1 1 β t sin ( Ο t ) d t = Ο 2 β and β« β 1 1 t 3 sin β‘ ( Ο t ) β d t = 2 Ο β 12 Ο 3 \int_{-1}^{1} t^3\sin(\pi t)\,dt = \tfrac{2}{\pi} - \tfrac{12}{\pi^3} β« β 1 1 β t 3 sin ( Ο t ) d t = Ο 2 β β Ο 3 12 β . Which q β P 3 ( R ) q \in \mathcal{P}_3(\mathbf{R}) q β P 3 β ( R ) represents Ο \varphi Ο ?
a q ( x ) = 3 Ο x q(x) = \frac{3}{\pi}x q ( x ) = Ο 3 β x
b q ( x ) = 3 Ο x + 7 ( Ο 2 β 15 ) 2 Ο 3 ( 5 x 3 β 3 x ) q(x) = \frac{3}{\pi}x + \frac{7(\pi^2 - 15)}{2\pi^3}(5x^3 - 3x) q ( x ) = Ο 3 β x + 2 Ο 3 7 ( Ο 2 β 15 ) β ( 5 x 3 β 3 x )
c q ( x ) = sin β‘ ( Ο x ) q(x) = \sin(\pi x) q ( x ) = sin ( Ο x )
d q ( x ) = 3 Ο x + 14 ( Ο 2 β 15 ) Ο 3 ( 5 x 3 β 3 x ) q(x) = \frac{3}{\pi}x + \frac{\sqrt{14}(\pi^2 - 15)}{\pi^3}(5x^3 - 3x) q ( x ) = Ο 3 β x + Ο 3 14 β ( Ο 2 β 15 ) β ( 5 x 3 β 3 x )
β
Correct! Only the odd basis elements
e 2 e_2 e 2 β and
e 4 e_4 e 4 β contribute, and
Ο ( e 4 ) = 14 ( Ο 2 β 15 ) Ο 3 β 0 \varphi(e_4) = \tfrac{\sqrt{14}(\pi^2 - 15)}{\pi^3} \neq 0 Ο ( e 4 β ) = Ο 3 14 β ( Ο 2 β 15 ) β ξ = 0 .
β Close, butβ¦ that is the representer on
P 2 ( R ) \mathcal{P}_2(\mathbf{R}) P 2 β ( R ) . On
P 3 ( R ) \mathcal{P}_3(\mathbf{R}) P 3 β ( R ) formula (R) has a fourth term, and
Ο ( e 4 ) β 0 \varphi(e_4) \neq 0 Ο ( e 4 β ) ξ = 0 :
( 5 t 3 β 3 t ) sin β‘ ( Ο t ) (5t^3 - 3t)\sin(\pi t) ( 5 t 3 β 3 t ) sin ( Ο t ) is even, not odd. Indeed
β¨ x 3 , 3 Ο x β© = 6 5 Ο \langle x^3, \tfrac{3}{\pi}x \rangle = \tfrac{6}{5\pi} β¨ x 3 , Ο 3 β x β© = 5 Ο 6 β , while
Ο ( x 3 ) = 2 Ο β 12 Ο 3 \varphi(x^3) = \tfrac{2}{\pi} - \tfrac{12}{\pi^3} Ο ( x 3 ) = Ο 2 β β Ο 3 12 β .
β Not quite. sin β‘ ( Ο x ) \sin(\pi x) sin ( Ο x ) is not a polynomial, so it is not an element of
P 3 ( R ) \mathcal{P}_3(\mathbf{R}) P 3 β ( R ) β the theorem promises a representer
inside the space.
β Not quite. This multiplies
Ο ( e 4 ) \varphi(e_4) Ο ( e 4 β ) by
5 x 3 β 3 x 5x^3 - 3x 5 x 3 β 3 x instead of by
e 4 = 14 4 ( 5 x 3 β 3 x ) e_4 = \tfrac{\sqrt{14}}{4}(5x^3 - 3x) e 4 β = 4 14 β β ( 5 x 3 β 3 x ) . Formula (R) uses the whole basis element, so the two factors
14 4 \tfrac{\sqrt{14}}{4} 4 14 β β combine into
14 16 \tfrac{14}{16} 16 14 β .
Show solution
By (R) over R \mathbf{R} R , q = Ο ( e 1 ) e 1 + Ο ( e 2 ) e 2 + Ο ( e 3 ) e 3 + Ο ( e 4 ) e 4 q = \varphi(e_1)e_1 + \varphi(e_2)e_2 + \varphi(e_3)e_3 + \varphi(e_4)e_4 q = Ο ( e 1 β ) e 1 β + Ο ( e 2 β ) e 2 β + Ο ( e 3 β ) e 3 β + Ο ( e 4 β ) e 4 β .
sin β‘ ( Ο t ) \sin(\pi t) sin ( Ο t ) is odd, so e 1 ( t ) sin β‘ ( Ο t ) e_1(t)\sin(\pi t) e 1 β ( t ) sin ( Ο t ) and e 3 ( t ) sin β‘ ( Ο t ) e_3(t)\sin(\pi t) e 3 β ( t ) sin ( Ο t ) are odd and integrate to zero over [ β 1 , 1 ] [-1, 1] [ β 1 , 1 ] : Ο ( e 1 ) = Ο ( e 3 ) = 0 \varphi(e_1) = \varphi(e_3) = 0 Ο ( e 1 β ) = Ο ( e 3 β ) = 0 . The other two use the given integrals:
Ο ( e 2 ) = 3 2 β
2 Ο , Ο ( e 4 ) = 14 4 ( 5 ( 2 Ο β 12 Ο 3 ) β 3 β
2 Ο ) = 14 4 ( 4 Ο β 60 Ο 3 ) . \varphi(e_2) = \sqrt{\tfrac32}\cdot\tfrac{2}{\pi}, \qquad \varphi(e_4) = \tfrac{\sqrt{14}}{4}\left(5\left(\tfrac{2}{\pi} - \tfrac{12}{\pi^3}\right) - 3\cdot\tfrac{2}{\pi}\right) = \tfrac{\sqrt{14}}{4}\left(\tfrac{4}{\pi} - \tfrac{60}{\pi^3}\right). Ο ( e 2 β ) = 2 3 β β β
Ο 2 β , Ο ( e 4 β ) = 4 14 β β ( 5 ( Ο 2 β β Ο 3 12 β ) β 3 β
Ο 2 β ) = 4 14 β β ( Ο 4 β β Ο 3 60 β ) .
Multiplying each by its basis element, the square roots combine: 3 2 β
2 Ο = 3 Ο \tfrac32 \cdot \tfrac{2}{\pi} = \tfrac{3}{\pi} 2 3 β β
Ο 2 β = Ο 3 β and 14 16 ( 4 Ο β 60 Ο 3 ) = 7 ( Ο 2 β 15 ) 2 Ο 3 \tfrac{14}{16}\left(\tfrac{4}{\pi} - \tfrac{60}{\pi^3}\right) = \tfrac{7(\pi^2 - 15)}{2\pi^3} 16 14 β ( Ο 4 β β Ο 3 60 β ) = 2 Ο 3 7 ( Ο 2 β 15 ) β . Hence
q ( x ) = 3 Ο x + 7 ( Ο 2 β 15 ) 2 Ο 3 ( 5 x 3 β 3 x ) . q(x) = \frac{3}{\pi}x + \frac{7(\pi^2 - 15)}{2\pi^3}(5x^3 - 3x). q ( x ) = Ο 3 β x + 2 Ο 3 7 ( Ο 2 β 15 ) β ( 5 x 3 β 3 x ) .
Since Ο 2 β 15 \pi^2 \neq 15 Ο 2 ξ = 15 , the cubic term is really there: the representer on P 3 ( R ) \mathcal{P}_3(\mathbf{R}) P 3 β ( R ) differs from the one on P 2 ( R ) \mathcal{P}_2(\mathbf{R}) P 2 β ( R ) , which is 3 Ο x \tfrac{3}{\pi}x Ο 3 β x .
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