Large-N and Large-T Properties of Panel Data Estimators and the Hausman Test



Notice that by Lemmas 2 and 4, under the fixed effect assumption (Assumption
10), the first term of (92) is

θ2NTGχ,τN Xxi(zzi + vi)
i

θ2NTGx,τD-τNN X Dχ,τzi(zi + Vi)

θ2NTGx,TD-,T {Ξχλ + op (1)} ,

where we partition


xx

zx


xz

zz


conformably to the sizes of xit and zi , and set


)

Ξx = (Ξxx , Ξxz) . Similarly, by


Lemmas 2 and 4, under the fixed effect assumption, the second term of (92) is


θT √NTGχ,τ D-T


N x Dχ,τxiz! f-N X ziz!  (N χ z (u+vi)

ii

θT√NTGχ,τD-,1T {


xzΞz-z1Ξzλ+op(1) .

Therefore, the limit of (92) is

θ ' G D    [ ( Ξχχ

Ξ-1 Ξ    .. 0 λ + op

xz zz zx .               p

Recall that it is assumed that NN c < . Also, recall that under the restric-
tions given in the theorem,
Gx,T = diag (Ik22, Ik3) and Dχ,τ = diag TTlk22, D3τ) .
Then, letting λmax (A) denote the maximum eigenvalue of matrix A, we can have


λmax (θTNTGχ,TD-Т)

O (1) ∕T λmax μ TIk22 , D3T1^ 0.


So, under the assumptions of Part (b), the probability limit of the numerator
of (88) is


1

NT


∑∑G∙,t ⅛⅛ + op (1).


(93)


Combining (91) and (93), we can obtain Part (b). ¥


Proof of Theorem 8

Using the notation in (87) , we can express the GLS estimator γg by


^

Yg - Y


57




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