Density Estimation and Combination under Model Ambiguity



Now, the same expansion used for KI21 can be applied to KI22(fθ*, g):

ki 22(fθ* ,g) =


1 XX μ fθ* (xi) - g(xi) v b (x )
n M   g(x
i)     f


1 X <fθ* (xi) - g(xi)A2 b, ʌ 1     1 τ

- 2n Σ —g(χi)— f fn(xi) = Jn1- 2J2


(96)


E Jin(fθ* ,g)) = E


K(u) (fθ* (x) g(x)) g(x + hu)dxdu.

(97)


Applying the same steps used for S2n we can show that


lim sup E
n→∞


(Jin(fθ*,g)) У


(fθ* (x) — g(x)) g(x)dx = E (fθ* (x) g(x))


lim E ( Jin(fθ* ,g)) = E (fθ* (x) g(x)).                                 (98)

n→∞

It follows that J1n(fθ*, g) = Op(1). Repeating the same steps once more for J2n(fθ*, g) we obtain:

E А XX μ fθ(xi) - g(xi) ..^ A = E (t μ fθ- (xi) -g(xi) V2 fn^^d

n i=1         g(xi)                                       g(xi)

=E


(fθ* (xi) - g(xi))2


g(xi)


fn(xi)dxi I = (( K(u)    ( ) g^ g( g(x + hu)dxdu,

g(x)


lim sup E (J2n(fθ* ,g)) ( (fθ (x) g(x))2 dx

n→∞

lim E (J2n(fθ* ,g))= ( (fθ* (x) g(x))2 dx > 0.

n→∞

Then also J2n(fθ* ,g) = Op(1). This implies that KI22(fθ* ,g) = Jni 2 Jn2 = Op(1).
Then it is clear that given assumptions A1-A4, if h 0,nh→∞then


(99)

(100)

(101)


KI22(fθ* ,g) p E (fθ* (x) g(x)) 2 У (fθ* (x) g(x))2 dx = E [lnfθ* lng],


(102)


this implies that nh1/2 KTI 22 p , hence we need to rescale it by dn = n-1h-1/2 where dn 0 as
This is embodied in assumption A6:


n →∞.


Finally we can put all terms together:


KI =


(ln

x


KTI22 ` ah1/2Cn


(103)


—~~                           —~~                 —~~

fTn(x) lnfbθ(x))fTn(x)dx == KTI1


—-~.

KTI2


(nh1/2) 1ιNι (nh1/2) 12N2 2 Cn


KI21(fb, fθ* ) + KI22(fθ* , g)J ,


(104)


since we showed that

32



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