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Estimation and testing of the factor-augmented panel regression models with missing data

  • Difa Xiao , Lu Wang and Jianhong Wu EMAIL logo
Published/Copyright: March 2, 2023

Abstract

This paper focuses on the factor-augmented panel regression models with missing data and individual-varying factors. A so-called CCEM estimator for the slope coefficient is proposed and its asymptotic properties are investigated under some regularity conditions. Furthermore, a joint test statistic is constructed for serial correlation and heteroscedasticity in the idiosyncratic errors. Under the null hypothesis, the test statistic can be shown to be asymptotically chi-square distributed. Monte Carlo simulation results show that the proposed estimator and test statistic have desired performance in finite samples.

JEL Classification: C12; C13; C33

Corresponding author: Jianhong Wu, Shanghai Normal University, Shanghai 200234, China, E-mail:

  1. Author contributions: All the authors have accepted responsibility for the entire content of this submitted manuscript and approved submission.

  2. Research funding: This paper is supported in part by the National Nature Science Foundation of China (Grant No. 72173086).

  3. Conflict of interest statement: The authors declare no conflicts of interest regarding this article.

Appendix

The appendix contains the proofs of Theorems 1–3.

A.1 Proof of Theorem 1

As a step of the proof of Theorem 1, an asymptotic expansion of N ( β ̂ CCEM β ) will be firstly derived. Moreover, since the proof of Theorem 1 is similar to that of Theorem 1 in Westerlund et al. (2019), only some important details are presented here.

A.1.1 Step1: deriving the asymptotic expansion of N ( β ̂ CCEM β )

This expansion depends on whether m < k + 1 or m = k + 1. Suppose first that m < k + 1. We introduce a full rank matrix H j = [H m,j , H m,j ] and a normalization matrix D N j = diag ( I m , N j I k + 1 m ) , where H j and D N j are both (k + 1) × (k + 1). Also, H m,j and H m,j are (k + 1) × m and (k + 1) × (k + 1 − m) matrices, respectively. H m , j = Q C ̄ j C ̄ j Q Q C ̄ j 1 and H m,j = G j B m,j where G j and B m,j are the same as G and B m in Westerlund et al. (2019). The useful properties of H j and D N j are respectively C ̄ j Q H j = I m , 0 m × ( k + 1 m ) and U ̄ j Q H j D N j = [ U ̄ j Q H m , j , N j U ̄ j Q H m , j ] = U ̄ m , j 0 , U ̄ m , j 0 = U ̄ j 0 , where U ̄ m , j 0 = O p N j 1 / 2 and U ̄ m , j 0 = O p ( 1 ) . We have

Z ̄ j 0 = Z ̄ j H j D N j = F j , 0 T j × ( k + 1 m ) + U ̄ m , j 0 , U ̄ m , j 0 = F j , U ̄ m , j 0 + O p N j 1 / 2 , Y i = X j i β + Z ̄ j H m , j γ j i ( Z ̄ j F j C ̄ j Q ) H m , j γ j i + ε j i = X j i β + Z ̄ j H m , j γ j i U ̄ m , j 0 γ j i + ε j i .

Moreover, since M Z ̄ j = M Z ̄ j 0 , we have

N ( β ̂ CCEM β ) = 1 N j = 1 n i = 1 N j X j i M Z ̄ j 0 X j i 1 1 N j = 1 n i = 1 N j X j i M Z ̄ j 0 ε j i U ̄ m , j 0 γ j i .

Consider the numerator,

1 N j = 1 n i = 1 N j X j i M Z ̄ j 0 ε j i U ̄ m , j 0 γ j i = j = 1 n N j N 1 N j i = 1 N j X j i M Z ̄ j 0 ε j i U ̄ m , j 0 γ j i .

In analogy to (A.46) in Westerlund et al. (2019), we have

1 N j i = 1 N j X j i M Z ̄ j 0 ε j i U ̄ m , j 0 γ j i = 1 N j i = 1 N j V j i ( M F j P m , j ) ε j i + O p N j 1 / 2 ,

where P m , j = P M F j U ̄ m , j 0 as m < k + 1, and P m , j = 0 T j × T j as m = k + 1 (see also, Westerlund et al. 2019). Hence, the numerator of N ( β ̂ CCEM β ) can be written as

(A.1) 1 N j = 1 n i = 1 N j X j i M Z ̄ j 0 ε j i U ̄ m , j 0 γ j i = j = 1 n N j N 1 N j i = 1 N j V j i ( M F j P m , j ) ε j i + O p N j 1 / 2 = 1 N j = 1 n i = 1 N j V j i ( M F j P m , j ) ε j i + O p ( N 1 / 2 ) .

Next, consider the denominator of N ( β ̂ CCEM β ) . By analogy to Lemma A.2 in Westerlund et al. (2019), we can write

(A.2) 1 N j = 1 n i = 1 N j X j i M Z ̄ j 0 X j i = j = 1 n N j N 1 N j i = 1 N j V j i ( M F j P m , j ) V j i + O p N j 1 / 2 = 1 N j = 1 n i = 1 N j V j i ( M F j P m , j ) V j i + O p ( N 1 / 2 ) = Σ N + O p ( N 1 / 2 ) .

According to (A.1 A.2), we can obtain the asymptotic expansion of N ( β ̂ CCEM β ) as follows,

(A.3) N ( β ̂ CCEM β ) = Σ N 1 1 N j = 1 n i = 1 N j V j i ( M F j P m , j ) ε j i + O p ( N 1 / 2 ) .

A.1.2 Step 2: proof of Theorem 1

Now, we try to derive the asymptotic distribution of N ( β ̂ CCEM β ) , and first consider the case with m = k + 1. In analogy to Westerlund et al. (2019), we let ξ j i = V j i ( M F j P m , j ) ε j i = V j i M F j ε j i , ζ F j being the σ-field generated by F j , and F j i being the corresponding σ-field generated by ζ F j and ( ξ j 1 , , ξ j i ) . Then { ( ξ j i , F j i ) : i 1 } is a martingale difference sequence, and ξ j i is independent across j i and E ( ξ j i | F j i 1 ) = E ( ξ j i | ζ F j ) = 0 k × 1 . Hence, the outer sum has a mixed normal distribution (see also, Westerlund et al. 2019), which is given by

(A.4) 1 N j = 1 n i = 1 N j ξ j i d M N ( 0 k × 1 , S ) ,

where

S = lim N 1 N j = 1 n i = 1 N j E ξ j i ξ j i | F j i 1 = lim N 1 N j = 1 n i = 1 N j E V j i M F j Σ ε , j i M F j V j i | ζ F j = j = 1 n w j lim N j 1 N j i = 1 N j E V j i M F j Σ ε , j i M F j V j i | ζ F j = j = 1 n w j S j ,

with Σ ε , j i = E ε j i ε j i . By the law of large numbers of Hall and Heyde (1980), we can obtain

Σ N = 1 N j = 1 n i = 1 N j V j i M F j V j i p j = 1 n w j lim N j 1 N j i = 1 N j E V j i M F j V j i | ζ F j = j = 1 n w j Σ j = Σ .

Hence, as N → ∞, we can also show that

(A.5) N ( β ̂ CCEM β ) = Σ N 1 1 N j = 1 n i = 1 N j V j i M F j ε j i + O p ( N 1 / 2 ) d M N 0 k × 1 , Σ 1 S Σ 1 .

Next, consider the case with m < k + 1. It follows that

1 N j = 1 n i = 1 N j V j i ( M F j P m , j ) ε j i = 1 N j = 1 n i = 1 N j t = 1 T j s = 1 T j v j i , t ( M F j , t , s P m , j , t , s ) ε j i , s = j = 1 n t = 1 T j s = 1 T j N j N ( M F j , t , s P m , j , t , s ) N j z ̄ j , t , s ,

where z ̄ j , t , s = N j 1 i = 1 N j ε j i , s v j i , t , M F j , t , s and pm,j,t,s are the (t, s)-th element of M F j and pm,j respectively. In analogy to (A.56 & A.61) in Westerlund et al. (2019), we have

N j u ̄ j , t d n u j , t = d N ( 0 ( k + 1 ) × 1 , Σ u , j , t ) , N j z ̄ j , t , s d n z j , t , s = d N ( 0 k × 1 , Σ z , j , t , s ) .

Hereafter, “ = d ” means equality in distribution, Σ u , j , t = lim N j N j 1 i = 1 N j ( Σ u , j i , t ) and Σ z , j , t , s = lim N j N j 1 i = 1 N j σ ε , j i , s 2 Σ v , j i , t . By using u ̄ m , j , t 0 to signify the tth row of U ̄ m , j 0 , we have

u ̄ m , j , t 0 = H m , j Q N j u ̄ j , t d H m , j Q n u j , t .

Then, we obtain

P m , j , t , s = l = 1 T j M F j , t , l u ̄ m , j , l 0 U ̄ m , j 0 M F j U ̄ m , j 0 1 r = 1 T j u ̄ m , j , r 0 M F j , s , r d l = 1 T j M F j , t , l n u j , l Q H m , j H m , j Q l = 1 T j r = 1 T j M F j , l , r n u j , l n u j , r Q H m , j 1 × r = 1 T j M F j , s , r H m , j Q n u j , r = p m , j , t , s ,

as N j → ∞, which implies

1 N j = 1 n i = 1 N j V j i ( M F j P m , j ) ε j i = j = 1 n t = 1 T j s = 1 T j N j N ( M F j , t , s p m , j , t , s ) N j z ̄ j , t , s d j = 1 n t = 1 T j s = 1 T j w j ( M F j , t , s p m , j , t , s ) n z j , t , s .

According to (A.64) in Westerlund et al. (2019), we have E u j i , t z l r , n , s = 0 ( k + 1 ) × k for all i, j, l, r, t, n and s. It means that n z j , n , s and M F j , t , s p m , j , t , s are independent of each other. Hence,

j = 1 n t = 1 T j s = 1 T j w j ( M F j , t , s p m , j , t , s ) n z j , t , s = d M N 0 k × 1 , S ,

where S = j = 1 n w j S j , and

S j = t = 1 T j s = 1 T j l = 1 T j r = 1 T j ( M F j , t , s p m , j , t , s ) ( M F j , l , r p m , j , l , r ) Σ z j , t , l , s , r ,

with Σ z j , t , l , s , r = lim N j N j 1 i = 1 N j ( σ ε , j i , s , r Σ v , j i , t , l ) , σ ε , j i , s , r = E ( ε j i , s ε j i , r ) and Σ v , j i , t , l = E v j i , t v j i , l . For the denominator, we have

Σ N = j = 1 n t = 1 T j s = 1 T j N j N ( M F j , t , s P m , j , t , s ) 1 N j i = 1 N j v j i , t v j i , s p j = 1 n t = 1 T j s = 1 T j w j ( M F j , t , s p m , j , t , s ) Σ v , j i , t , s = j = 1 n w j Σ j = Σ .

Hence, as N → ∞, we can show that

N ( β ̂ CCEM β ) d M N 0 k × 1 , Σ 1 S Σ 1 .

The proof of Theorem 1 is then complete. □

A.2 Proof of Theorems 2 and 3

The proofs of Theorems 2–3 are respectively similar to those of Westerlund et al. (2019) and Wu (2020), and then omitted to save the space.

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Received: 2022-04-27
Accepted: 2023-02-07
Published Online: 2023-03-02

© 2023 Walter de Gruyter GmbH, Berlin/Boston

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