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arXiv:2606.01011v2 [math.ST] 19 Aug 2026

Semiparametric Efficiency of Residual Correlation Testing under Gaussian Additive Noise Models

Yin Tanga, Yanyuan Mab, Bing Lib

aDr. Bing Zhang Department of Statistics, University of Kentucky, USA
bDepartment of Statistics, Pennsylvania State University, USA

Keywords: Conditional independence test, Pearson correlation, semiparametric efficiency, additive noise model

Abstract

This paper studies conditional independence testing under the Gaussian additive noise model (GANM), where two variables are modeled as nonlinear functions of covariates with independent bivariate Gaussian regression errors. Under this framework, conditional independence can be characterized by the correlation coefficient of the regression errors, which motivates a test based on the Pearson correlation coefficient computed from the fitted residuals. Despite its simple form, the asymptotic behavior and statistical efficiency of the resulting test have not been well understood. In this paper, we develop the semiparametric efficiency theory under GANM and show, surprisingly, that the efficient estimator coincides exactly with the ordinary residual Pearson correlation estimator. We further establish the asymptotic properties of the proposed test and develop the corresponding inference procedure. Simulation studies demonstrate that the proposed method achieves near-oracle efficiency and competitive empirical power while maintaining valid Type I error control. We further apply the proposed test to conditional dependence analysis of U.S. stock returns.

1 Introduction

Consider the case where XX and YY are random variables, and 𝐙{\bf Z} is a random vector. We want to test

H0:X   Y|𝐙\displaystyle H_{0}:\quad X\;\,\rule[0.0pt]{0.29999pt}{6.69998pt}\hskip-2.5pt\rule[0.0pt]{6.49994pt}{0.29999pt}\hskip-2.5pt\rule[0.0pt]{0.29999pt}{6.69998pt}\;\,Y|{\bf Z} (1)

against the alternative that XX and YY are dependent conditioning on 𝐙{\bf Z}. See 6 for detailed explanations of conditional independence. Conditional independence test plays a central role in many statistical fields, including sufficient dimension reduction (20; 22), statistical graphical models (18; 17), and causal inference (8; 24).

In the multivariate Gaussian case, conditional independence can be characterized by partial correlations (7; 2), which can be interpreted through linear regression. Specifically, the partial correlation between XX and YY given 𝐙{\bf Z} equals the ordinary Pearson correlation between the regression errors from the linear regressions of XX on 𝐙{\bf Z} and YY on 𝐙{\bf Z}. Consequently, in Gaussian linear models, testing (1) reduces to testing whether these regression errors are uncorrelated, with the unknown errors replaced in practice by their fitted residuals. Such a characterization is often used in multivariate analysis (1) and graphical models (18).

In the partial correlation test, it is assumed that the mean functions of XX and YY given 𝐙{\bf Z} are both linear. An extension is the additive noise model (ANM), in which the conditional mean functions are allowed to be nonlinear while the regression errors remain additive. Specifically, XX and YY are some deterministic functions of 𝐙{\bf Z} plus additive regression errors, i.e.,

X=mx(𝐙)+ϵx,Y=my(𝐙)+ϵy,\displaystyle X=m_{x}({\bf Z})+\epsilon_{x},\qquad Y=m_{y}({\bf Z})+\epsilon_{y}, (2)

where ϵx\epsilon_{x} and ϵy\epsilon_{y} are zero-mean regression errors independent of 𝐙{\bf Z}. In particular, the ANM with Gaussian noise can be viewed as a nonlinear extension of the classical linear Gaussian model. In practice, ANM is often applied to causal discovery (32; 14; 25; 26).

As pointed out in Section 3.1.5 of 21, testing conditional independence under the ANM framework can be reduced to testing unconditional independence between the corresponding regression errors (41; 40). In practice, this is typically carried out in two steps: (1) regress XX on 𝐙{\bf Z} and YY on 𝐙{\bf Z} to estimate the regression functions; and (2) test for unconditional independence between the resulting fitted residuals

ϵ^x=Xm^x(𝐙),ϵ^y=Ym^y(𝐙).\displaystyle\widehat{\epsilon}_{x}=X-\widehat{m}_{x}({\bf Z}),\qquad\widehat{\epsilon}_{y}=Y-\widehat{m}_{y}({\bf Z}).

When ANM is violated, some nonparametric tests for conditional independence have been proposed, including the discretization-based conditional independence test (16), the metric-based approaches via suitable discrepancy criteria, (35; 15; 39), the permutation-based kernel conditional independence test (9), and the transformation-based mutual independence framework (4). See 21 for a review. In addition, under the reproducing kernel Hilbert space (RKHS) framework, 42 proposed the kernel conditional independence test (KCIT) based on the conditional covariance operator of 10; 11; see also 31 and 36 for further theoretical developments. Furthermore, 33 introduced two tests based on random Fourier features, the randomized conditional independence test (RCIT) and the randomized conditional correlation test (RCoT).

In this paper, we focus on the Gaussian additive noise model (GANM). That is, we assume that (X,Y,𝐙)(X,Y,{\bf Z}) satisfy the model (2), where the regression errors (ϵx,ϵy)(\epsilon_{x},\epsilon_{y}) follow a bivariate Gaussian distribution. In this setting, following the idea of 41, conditional independence between XX and YY given 𝐙{\bf Z} can be tested using Pearson’s correlation coefficient computed from the fitted residuals ϵ^x\widehat{\epsilon}_{x} and ϵ^y\widehat{\epsilon}_{y}.

However, despite this seemingly simple construction, several important theoretical questions remain largely unresolved. First, after replacing the unobserved regression errors (ϵx,ϵy)(\epsilon_{x},\epsilon_{y}) by fitted residuals (ϵ^x,ϵ^y)(\widehat{\epsilon}_{x},\widehat{\epsilon}_{y}) obtained from nonparametric regressions, the asymptotic distribution of the resulting Pearson correlation estimator is no longer immediate, especially when flexible machine learning methods are employed. Second, it remains unclear whether the resulting residual-correlation-based test retains statistical efficiency after the nuisance regression functions are estimated nonparametrically. In particular, it is important to understand whether the estimation error from the nonparametric regressions affects the first-order asymptotic behavior of the test statistic, and whether the procedure can still achieve the same asymptotic efficiency as the oracle procedure based on the true regression errors. Third, suitable convergence rate conditions on the nonparametric regression estimators are needed to guarantee the validity of the asymptotic inference. Addressing these issues is therefore essential for establishing a rigorous theoretical foundation for residual-correlation-based conditional independence testing under the GANM framework.

Surprisingly, under GANM, the semiparametrically efficient estimator induced by the efficient influence function coincides exactly with the ordinary Pearson correlation coefficient computed from the fitted residuals. Thus, despite its simple form, the residual correlation estimator remains asymptotically efficient even when the nuisance regression functions are estimated nonparametrically using flexible machine learning methods. Moreover, by combining sample splitting and cross-fitting, the resulting asymptotic theory only requires suitable convergence rate conditions on the nuisance regression estimators, without requiring explicit asymptotic expansions of the underlying machine learning procedures. To establish these results, we develop the semiparametric efficiency theory under GANM and derive the asymptotic linearity and asymptotic normality of the resulting estimator.

Although our work is also based on residuals from nonparametric regression, its scope is narrower from that of 5, which develops a general framework for high-dimensional conditional independence testing. By focusing on the more specific class of Gaussian additive noise models, we are able to recast the conditional independence test to the problem of testing zero residual correlation. This approach further allows us to establish the semiparametric efficiency theory for the residual Pearson correlation estimator, which leads to a most powerful test. In summary, using different tools, we study a more specific problem more thoroughly, whereas 5 works in a more general framework without studying optimality.

The rest of the paper is organized as follows. Section 2 illustrates the setting of GANM and the intuition of the residual correlation estimator. Section 3 introduces the semiparametric efficiency theory of the estimator and gives its asymptotic properties. Section 4 conducts some simulation studies of the proposed estimator with some comparisons with some other conditional independence tests. Section 5 applies the proposed test to a real dataset on U.S. stocks. To save space, all proofs and additional simulations tables and figures are presented in Supplementary Materials.

2 Model and Test Construction

2.1 Gaussian Additive Noise Model

Consider the Gaussian additive noise model (GANM), where X,Y,𝐙X,Y,{\bf Z} satisfy the ANM in (2), where the regression errors (ϵx,ϵy)N(𝟎,𝚺)(\epsilon_{x},\epsilon_{y})^{\top}\sim N({\bf 0},{\bm{\Sigma}}) where

𝚺=(σx2ρσxσyρσxσyσy2).\displaystyle{\bm{\Sigma}}=\left(\begin{matrix}\sigma_{x}^{2}&\rho\sigma_{x}\sigma_{y}\\ \rho\sigma_{x}\sigma_{y}&\sigma_{y}^{2}\end{matrix}\right).

Here, σx2\sigma_{x}^{2} and σy2\sigma_{y}^{2} are the variances of ϵx\epsilon_{x} and ϵy\epsilon_{y}, respectively, and ρ\rho is the correlation coefficient between ϵx\epsilon_{x} and ϵy\epsilon_{y}, i.e., ρ=corr(ϵx,ϵy)\rho=\mbox{corr}(\epsilon_{x},\epsilon_{y}).

Clearly, under GANM, since XX and YY depend on 𝐙{\bf Z} only through the conditional mean function mx(𝐙)m_{x}({\bf Z}) and my(𝐙)m_{y}({\bf Z}), we know that X   Y|𝐙X\;\,\rule[0.0pt]{0.29999pt}{6.69998pt}\hskip-2.5pt\rule[0.0pt]{6.49994pt}{0.29999pt}\hskip-2.5pt\rule[0.0pt]{0.29999pt}{6.69998pt}\;\,Y|{\bf Z} if and only if the regression errors are independent, i.e., ϵx   ϵy\epsilon_{x}\;\,\rule[0.0pt]{0.29999pt}{6.69998pt}\hskip-2.5pt\rule[0.0pt]{6.49994pt}{0.29999pt}\hskip-2.5pt\rule[0.0pt]{0.29999pt}{6.69998pt}\;\,\epsilon_{y}, which, under the joint Gaussian assumption for (ϵx,ϵy)(\epsilon_{x},\epsilon_{y}), is further equivalent to corr(ϵx,ϵy)=0\mbox{corr}(\epsilon_{x},\epsilon_{y})=0, i.e., ρ=0\rho=0. Therefore, to test whether (1) holds, we can equivalently test

H0:ρ=0vs.H1:ρ0.\displaystyle H_{0}:\rho=0\quad\text{vs.}\quad H_{1}:\rho\neq 0. (3)

In this way, under GANM, testing conditional independence of XX and YY given 𝐙{\bf Z} is equivalent to testing the uncorrelatedness of the regression errors ϵx\epsilon_{x} and ϵy\epsilon_{y}.

2.2 Residual Correlation Estimator

We first consider the oracle case when the regression functions mxm_{x} and mym_{y} are known. In this case, we could directly calculate the true regression errors

ϵxi=Ximx(𝐙i),ϵyi=Yimy(𝐙i),i=1,,n,\displaystyle\epsilon_{xi}=X_{i}-m_{x}({\bf Z}_{i}),\quad\epsilon_{yi}=Y_{i}-m_{y}({\bf Z}_{i}),\qquad i=1,\dots,n,

Based on (ϵx1,ϵy1),,(ϵxn,ϵyn)(\epsilon_{x1},\epsilon_{y1}),\dots,(\epsilon_{xn},\epsilon_{yn}), we then estimate ρ\rho by the Pearson correlation coefficient

ρ^orc=σ^xy,orcσ^x,orcσ^y,orc=i=1nϵxiϵyi(i=1nϵxi2)1/2(i=1nϵyi2)1/2.\displaystyle\widehat{\rho}_{\rm{orc}}=\frac{\widehat{\sigma}_{xy,\rm{orc}}}{\widehat{\sigma}_{x,\rm{orc}}\widehat{\sigma}_{y,\rm{orc}}}=\frac{\sum_{i=1}^{n}\epsilon_{xi}\epsilon_{yi}}{(\sum_{i=1}^{n}\epsilon_{xi}^{2})^{1/2}(\sum_{i=1}^{n}\epsilon_{yi}^{2})^{1/2}}.

Here,

σ^xy,orc=n1i=1nϵxiϵyi,σ^x,orc2=n1i=1nϵxi2,σ^y,orc2=n1i=1nϵyi2\displaystyle\widehat{\sigma}_{xy,\rm{orc}}=n^{-1}\sum_{i=1}^{n}\epsilon_{xi}\epsilon_{yi},\quad\widehat{\sigma}_{x,\rm{orc}}^{2}=n^{-1}\sum_{i=1}^{n}\epsilon_{xi}^{2},\quad\widehat{\sigma}_{y,\rm{orc}}^{2}=n^{-1}\sum_{i=1}^{n}\epsilon_{yi}^{2}

are estimators of σx2=var(ϵx)\sigma_{x}^{2}=\mbox{var}(\epsilon_{x}), σy2=var(ϵy)\sigma_{y}^{2}=\mbox{var}(\epsilon_{y}), and σxy=cov(ϵx,ϵy)\sigma_{xy}=\mbox{cov}(\epsilon_{x},\epsilon_{y}), respectively. Since (ϵxi,ϵyi)(\epsilon_{xi},\epsilon_{yi})^{\top} are i.i.d. bivariate Gaussian random vectors, by Theorem 5.1.6 of 23, the asymptotic distribution of ρ^orc\widehat{\rho}_{\rm{orc}} is

n1/2(ρ^orcρ)𝑑N{0,(1ρ2)2}.\displaystyle n^{1/2}(\widehat{\rho}_{\rm{orc}}-\rho)\overset{d}{\to}N\{0,(1-\rho^{2})^{2}\}. (4)

In particular, under the null hypothesis H0:ρ=0H_{0}:\rho=0, the asymptotic null distribution of ρ^\widehat{\rho} is

n1/2ρ^orc𝑑N(0,1).\displaystyle n^{1/2}\widehat{\rho}_{\rm{orc}}\overset{d}{\to}N(0,1).

In practice, the regression functions mxm_{x} and mym_{y} are unknown, and we define m^x\widehat{m}_{x} and m^y\widehat{m}_{y} as nonparametric estimators of mxm_{x} and mym_{y}, respectively. Based on m^x\widehat{m}_{x} and m^y\widehat{m}_{y}, We calculate the fitted residuals as

ϵ^xi=Xim^x(𝐙i),ϵ^yi=Yim^y(𝐙i),i=1,,n,\displaystyle\widehat{\epsilon}_{xi}=X_{i}-\widehat{m}_{x}({\bf Z}_{i}),\quad\widehat{\epsilon}_{yi}=Y_{i}-\widehat{m}_{y}({\bf Z}_{i}),\qquad i=1,\dots,n, (5)

and the residual correlation estimator is given by the Pearson correlation coefficient based on (ϵ^x1,ϵ^y1),,(ϵ^xn,ϵ^yn)(\widehat{\epsilon}_{x1},\widehat{\epsilon}_{y1}),\dots,(\widehat{\epsilon}_{xn},\widehat{\epsilon}_{yn}) is

ρ^=σ^xyσ^xσ^y=i=1nϵ^xiϵ^yi(i=1nϵ^xi2)1/2(i=1nϵ^yi2)1/2.\displaystyle\widehat{\rho}=\frac{\widehat{\sigma}_{xy}}{\widehat{\sigma}_{x}\widehat{\sigma}_{y}}=\frac{\sum_{i=1}^{n}\widehat{\epsilon}_{xi}\widehat{\epsilon}_{yi}}{(\sum_{i=1}^{n}\widehat{\epsilon}_{xi}^{2})^{1/2}(\sum_{i=1}^{n}\widehat{\epsilon}_{yi}^{2})^{1/2}}. (6)

Here,

σ^xy=n1i=1nϵ^xiϵ^yi,σ^x2=n1i=1nϵ^xi2,σ^y2=n1i=1nϵ^yi2\displaystyle\widehat{\sigma}_{xy}=n^{-1}\sum_{i=1}^{n}\widehat{\epsilon}_{xi}\widehat{\epsilon}_{yi},\quad\widehat{\sigma}_{x}^{2}=n^{-1}\sum_{i=1}^{n}\widehat{\epsilon}_{xi}^{2},\quad\widehat{\sigma}_{y}^{2}=n^{-1}\sum_{i=1}^{n}\widehat{\epsilon}_{yi}^{2} (7)

are corresponding estimators of σxy\sigma_{xy}, σx2\sigma_{x}^{2} and σy2\sigma_{y}^{2} when mxm_{x} and mym_{y} are estimated.

To make the asymptotic theory applicable to a broad class of machine learning methods for estimating mxm_{x} and mym_{y}, without requiring explicit asymptotic expansions of the nuisance regression estimators, we employ sample splitting and cross-fitting. Specifically, one part of the data is used to estimate the regression functions, while the other part is used to construct the residual correlation estimator ρ^\widehat{\rho}. The two resulting estimators are then averaged to obtain the final estimator. More details are given in Section 3.5.

3 Semiparametric Efficiency Theory

3.1 Semiparametric Model and Likelihood

Since (ϵx,ϵy)   𝐙(\epsilon_{x},\epsilon_{y})\;\,\rule[0.0pt]{0.29999pt}{6.69998pt}\hskip-2.5pt\rule[0.0pt]{6.49994pt}{0.29999pt}\hskip-2.5pt\rule[0.0pt]{0.29999pt}{6.69998pt}\;\,{\bf Z}, the conditional density of X,Y|𝐙X,Y|{\bf Z} can be written in terms of the joint density of the regression errors (ϵx,ϵy)(\epsilon_{x},\epsilon_{y}). That is,

fX,Y|𝐙(x,y,𝐳)=fϵx,ϵy{xmx(𝐳),ymy(𝐳)}=fϵx,ϵy(ϵx,ϵy),\displaystyle f_{X,Y|{\bf Z}}(x,y,{\bf z})=f_{\epsilon_{x},\epsilon_{y}}\{x-m_{x}({\bf z}),y-m_{y}({\bf z})\}=f_{\epsilon_{x},\epsilon_{y}}(\epsilon_{x},\epsilon_{y}),

where

ϵx=xmx(𝐳),ϵy=ymy(𝐳).\displaystyle\epsilon_{x}=x-m_{x}({\bf z}),\quad\epsilon_{y}=y-m_{y}({\bf z}). (8)

Then, for a realization (x,y,𝐳)(x,y,{\bf z}), the likelihood function can be written as

f(x,y,𝐳)=fX,Y|𝐙(x,y,𝐳)f𝐙(𝐳)=fϵx,ϵy(ϵx,ϵy)f𝐙(𝐳),\displaystyle f(x,y,{\bf z})=f_{X,Y|{\bf Z}}(x,y,{\bf z})f_{\bf Z}({\bf z})=f_{\epsilon_{x},\epsilon_{y}}(\epsilon_{x},\epsilon_{y})f_{\bf Z}({\bf z}),

where f𝐙f_{\bf Z} is the marginal distribution of 𝐙{\bf Z}. Furthermore, since (ϵx,ϵy)N(𝟎,𝚺)(\epsilon_{x},\epsilon_{y})^{\top}\sim N({\bf 0},{\bm{\Sigma}}), we plug in the Gaussian density function to get

f(x,y,𝐳)=12πσxσy1ρ2exp{12(1ρ2)(ϵx2σx22ρϵxϵyσxσy+ϵy2σy2)}f𝐙(𝐳),\displaystyle f(x,y,{\bf z})=\frac{1}{2\pi\sigma_{x}\sigma_{y}\sqrt{1-\rho^{2}}}\exp\left\{-\frac{1}{2(1-\rho^{2})}\left(\frac{\epsilon_{x}^{2}}{\sigma_{x}^{2}}-2\rho\frac{\epsilon_{x}\epsilon_{y}}{\sigma_{x}\sigma_{y}}+\frac{\epsilon_{y}^{2}}{\sigma_{y}^{2}}\right)\right\}f_{\bf Z}({\bf z}), (9)

where ϵx\epsilon_{x} and ϵy\epsilon_{y} are given by (8).

Note that, in the likelihood, our parameter of interest is ρ\rho, and all other parameters, including η={σx,σy,mx(),my(),f𝐙()}\eta=\{\sigma_{x},\sigma_{y},m_{x}(\cdot),m_{y}(\cdot),f_{\bf Z}(\cdot)\}, can be viewed as nuisance parameters. As we see, in the nuisance parameters, σx\sigma_{x} and σy\sigma_{y} are parametric, and the rest ones mx()m_{x}(\cdot), my()m_{y}(\cdot) and f𝐙()f_{\bf Z}(\cdot) are nonparametric.

The log likelihood is given by

logf(x,y,𝐳)\displaystyle\mbox{log}f(x,y,{\bf z}) =\displaystyle= log(2π)log(σx)log(σy)12log(1ρ2)\displaystyle\mbox{log}(2\pi)-\mbox{log}(\sigma_{x})-\mbox{log}(\sigma_{y})-\frac{1}{2}\mbox{log}(1-\rho^{2})
12(1ρ2)(ϵx2σx22ρϵxϵyσxσy+ϵy2σy2)+log{f𝐙(𝐳)}.\displaystyle-\frac{1}{2(1-\rho^{2})}\left(\frac{\epsilon_{x}^{2}}{\sigma_{x}^{2}}-2\rho\frac{\epsilon_{x}\epsilon_{y}}{\sigma_{x}\sigma_{y}}+\frac{\epsilon_{y}^{2}}{\sigma_{y}^{2}}\right)+\mbox{log}\{f_{\bf Z}({\bf z})\}.

3.2 Nuisance Tangent Spaces

To derive the efficient score for ρ\rho, we first calculate the nuisance tangent space associated with each of the the nuisance parameter in η={σx,σy,mx(),my(),f𝐙()}\eta=\{\sigma_{x},\sigma_{y},m_{x}(\cdot),m_{y}(\cdot),f_{\bf Z}(\cdot)\}. We then derive its orthogonal decomposition and its orthogonal complement, on which we will need to project the score function with respect to ρ\rho to find the efficient score (3; 37).

Denote ={f(x,y,𝐳):E{f(X,Y,𝐙)}=0,var{f(X,Y,𝐙)}<}{\cal H}=\{f(x,y,{\bf z}):E\{f(X,Y,{\bf Z})\}=0,\mbox{var}\{f(X,Y,{\bf Z})\}<\infty\} the Hilbert space of all possible influence functions. We first give the nuisance tangent space as the next proposition.

Proposition 1.

Under model (9) with parameter of interest ρ\rho and nuisance parameters η={σx,σy,mx(),my(),f𝐙()}\eta=\{\sigma_{x},\sigma_{y},m_{x}(\cdot),m_{y}(\cdot),f_{\bf Z}(\cdot)\}, let Λj\Lambda_{j}, j=1,,5j=1,\dots,5, denote the nuisance tangent space associated with the corresponding nuisance parameter component:

Λ1:σx,Λ2:σy,Λ3:mx,Λ4:my,Λ5:fZ.\displaystyle\Lambda_{1}:\sigma_{x},\qquad\Lambda_{2}:\sigma_{y},\qquad\Lambda_{3}:m_{x},\qquad\Lambda_{4}:m_{y},\qquad\Lambda_{5}:f_{Z}.

Then the nuisance tangent space of model (9) is

Λ=Λ1+Λ2+Λ3+Λ4+Λ5,\displaystyle\Lambda=\Lambda_{1}+\Lambda_{2}+\Lambda_{3}+\Lambda_{4}+\Lambda_{5},

where

Λ1\displaystyle\Lambda_{1} =\displaystyle= {c1(1σx+11ρ2ϵx2σx3ρ1ρ2ϵxϵyσx2σy)},\displaystyle\left\{c_{1}\left(-\frac{1}{\sigma_{x}}+\frac{1}{1-\rho^{2}}\frac{\epsilon_{x}^{2}}{\sigma_{x}^{3}}-\frac{\rho}{1-\rho^{2}}\frac{\epsilon_{x}\epsilon_{y}}{\sigma_{x}^{2}\sigma_{y}}\right)\right\},
Λ2\displaystyle\Lambda_{2} =\displaystyle= {c2(1σy+11ρ2ϵy2σy3ρ1ρ2ϵxϵyσxσy2)},\displaystyle\left\{c_{2}\left(-\frac{1}{\sigma_{y}}+\frac{1}{1-\rho^{2}}\frac{\epsilon_{y}^{2}}{\sigma_{y}^{3}}-\frac{\rho}{1-\rho^{2}}\frac{\epsilon_{x}\epsilon_{y}}{\sigma_{x}\sigma_{y}^{2}}\right)\right\},
Λ3\displaystyle\Lambda_{3} =\displaystyle= {11ρ2(ϵxσx2ρϵyσxσy)B1(𝐳)},\displaystyle\left\{\frac{1}{1-\rho^{2}}\left(\frac{\epsilon_{x}}{\sigma_{x}^{2}}-\rho\frac{\epsilon_{y}}{\sigma_{x}\sigma_{y}}\right)B_{1}({\bf z})\right\},
Λ4\displaystyle\Lambda_{4} =\displaystyle= {11ρ2(ϵyσy2ρϵxσxσy)B2(𝐳)},\displaystyle\left\{\frac{1}{1-\rho^{2}}\left(\frac{\epsilon_{y}}{\sigma_{y}^{2}}-\rho\frac{\epsilon_{x}}{\sigma_{x}\sigma_{y}}\right)B_{2}({\bf z})\right\},
Λ5\displaystyle\Lambda_{5} =\displaystyle= {a(𝐳):E(a)=0}.\displaystyle\{a({\bf z}):E(a)=0\}.

Based on the nuisance tangent space in Proposition 1, we derive the orthogonal complement of the nuisance tangent space as the following proposition.

Proposition 2.

Let Λ\Lambda^{\perp} denote the orthogonal complement of the nuisance tangent space Λ\Lambda in {\cal H}, where Λ\Lambda is given in Proposition 1. Then

Λ\displaystyle\Lambda^{\perp} =\displaystyle= {b(x,y,𝐳):E{(ϵ~x2ρϵ~xϵ~y)b(X,Y,𝐙)}=0,E{(ϵ~y2ρϵ~xϵ~y)b(X,Y,𝐙)}=0,\displaystyle\left\{b(x,y,{\bf z}):E\left\{\left(\widetilde{\epsilon}_{x}^{2}-\rho\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}\right)b(X,Y,{\bf Z})\right\}=0,E\left\{\left(\widetilde{\epsilon}_{y}^{2}-\rho\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}\right)b(X,Y,{\bf Z})\right\}=0,\right.
E{ϵ~xb(X,Y,𝐙)|𝐙}=0,E{ϵ~yb(X,Y,𝐙)|𝐙}=0,E{b(X,Y,𝐙)|𝐙}=0},\displaystyle\left.E\left\{\widetilde{\epsilon}_{x}b(X,Y,{\bf Z})\Big|{\bf Z}\right\}=0,E\left\{\widetilde{\epsilon}_{y}b(X,Y,{\bf Z})\Big|{\bf Z}\right\}=0,E\left\{b(X,Y,{\bf Z})|{\bf Z}\right\}=0\right\},

where ϵ~x=ϵx/σx\widetilde{\epsilon}_{x}=\epsilon_{x}/\sigma_{x} and ϵ~y=ϵy/σy\widetilde{\epsilon}_{y}=\epsilon_{y}/\sigma_{y}.

3.3 Efficient Score and Influence Function

In the next theorem, we give the efficient score function, which is defined as the projection of the score function with respect to ρ\rho onto Λ\Lambda^{\perp}, which is given in Proposition 2. The efficient score is written as Seff=Π(Sρ|Λ)S_{\rm eff}=\Pi(S_{\rho}|\Lambda^{\perp}), where Π\Pi is the projection operator. Based on the efficient score, we can further derive the efficient Fisher information and the efficient influence function as the next theorem.

Proposition 3.

Under model (9), the efficient score for ρ\rho is

Seff=12(1ρ2)2(ρϵ~x22ϵ~xϵ~y+ρϵ~y2).\displaystyle S_{\rm eff}=-\frac{1}{2(1-\rho^{2})^{2}}\left(\rho\widetilde{\epsilon}_{x}^{2}-2\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}+\rho\widetilde{\epsilon}_{y}^{2}\right). (10)

Furthermore, the semiparametric efficiency bound for estimating ρ\rho is

E(Seff2)1=(1ρ2)2,\displaystyle E(S_{\rm eff}^{2})^{-1}=(1-\rho^{2})^{2},

and the efficient influence function for ρ\rho is

ϕeff(x,y,𝐳)=12(ρϵ~x22ϵ~xϵ~y+ρϵ~y2).\displaystyle\phi_{\rm eff}(x,y,{\bf z})=-\frac{1}{2}\left(\rho\widetilde{\epsilon}_{x}^{2}-2\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}+\rho\widetilde{\epsilon}_{y}^{2}\right). (11)

As shown in (10), the efficient score function has a simple quadratic form involving only the standardized regression errors, and the corresponding efficient estimating equation leads to a simple explicit estimator in Section 3.4.

3.4 Efficient Estimating Equation

Based on semiparametric theory, the efficient estimator can be obtained through implementing

i=1nSeff(Xi,Yi,𝐙i)=0.\displaystyle\sum_{i=1}^{n}S_{\rm eff}(X_{i},Y_{i},{\bf Z}_{i})=0.

Plugging in the efficient score function (10), we have

i=1n(ρϵxi2σx22ϵxiϵyiσxσy+ρϵyi2σy2)=0.\displaystyle\sum_{i=1}^{n}\left(\rho\frac{\epsilon_{xi}^{2}}{\sigma_{x}^{2}}-2\frac{\epsilon_{xi}\epsilon_{yi}}{\sigma_{x}\sigma_{y}}+\rho\frac{\epsilon_{yi}^{2}}{\sigma_{y}^{2}}\right)=0. (12)

The solution to the estimating equation (12) can be explicitly written as

ρ^=2σxσyi=1nϵxiϵyiσy2i=1nϵxi2+σx2i=1nϵyi2.\displaystyle\widehat{\rho}=\frac{2\sigma_{x}\sigma_{y}\sum_{i=1}^{n}\epsilon_{xi}\epsilon_{yi}}{\sigma_{y}^{2}\sum_{i=1}^{n}\epsilon_{xi}^{2}+\sigma_{x}^{2}\sum_{i=1}^{n}\epsilon_{yi}^{2}}. (13)

In practice, all nuisance parameters need to be estimated. Firstly, mxm_{x} and mym_{y} are estimated by m^x\widehat{m}_{x} and m^y\widehat{m}_{y}. Then, based on m^x\widehat{m}_{x} and m^y\widehat{m}_{y}, we need to calculate the residuals ϵ^xi\widehat{\epsilon}_{xi} and ϵ^yi\widehat{\epsilon}_{yi} in (5) as the estimated versions of regression errors ϵxi\epsilon_{xi} and ϵyi\epsilon_{yi}. Next, based on the residuals ϵ^xi\widehat{\epsilon}_{xi} and ϵ^yi\widehat{\epsilon}_{yi}, we can estimate the unknown parameters σx\sigma_{x} and σy\sigma_{y} by σ^x\widehat{\sigma}_{x} and σ^y\widehat{\sigma}_{y} as defined in (7).

Surprisingly, after replacing all nuisance parameters in (13) by their empirical estimators, we obtain

ρ^=2(n1i=1nϵ^xi2)1/2(n1i=1nϵ^yi2)1/2i=1nϵ^xiϵ^yin1i=1nϵ^yi2i=1nϵ^xi2+n1i=1nϵ^xi2i=1nϵ^yi2=i=1nϵ^xiϵ^yi(i=1nϵ^xi2)1/2(i=1nϵ^yi2)1/2,\displaystyle\widehat{\rho}=\frac{2(n^{-1}\sum_{i=1}^{n}\widehat{\epsilon}_{xi}^{2})^{1/2}(n^{-1}\sum_{i=1}^{n}\widehat{\epsilon}_{yi}^{2})^{1/2}\sum_{i=1}^{n}\widehat{\epsilon}_{xi}\widehat{\epsilon}_{yi}}{n^{-1}\sum_{i=1}^{n}\widehat{\epsilon}_{yi}^{2}\sum_{i=1}^{n}\widehat{\epsilon}_{xi}^{2}+n^{-1}\sum_{i=1}^{n}\widehat{\epsilon}_{xi}^{2}\sum_{i=1}^{n}\widehat{\epsilon}_{yi}^{2}}=\frac{\sum_{i=1}^{n}\widehat{\epsilon}_{xi}\widehat{\epsilon}_{yi}}{(\sum_{i=1}^{n}\widehat{\epsilon}_{xi}^{2})^{1/2}(\sum_{i=1}^{n}\widehat{\epsilon}_{yi}^{2})^{1/2}},

which coincides with residual correlation estimator as in (6). Therefore, the residual correlation estimator in (6) can be equivalently interpreted as the estimator induced by the efficient influence function under GANM.

3.5 Sample Splitting and Cross-Fitting

Note that the nuisance regression functions mxm_{x} and mym_{y} need to be estimated nonparametrically from the data. To facilitate the asymptotic analysis, we employ sample splitting and cross-fitting as introduced in Section 2.2. This construction separates the nuisance estimation step from the estimation step for ρ\rho, which avoids requiring explicit asymptotic expansions of the nonparametric regression estimators and allows the asymptotic theory to rely primarily on suitable convergence rate conditions.

Specifically, we use the first n1n_{1} data to estimate mxm_{x} and mym_{y}, denote the corresponding estimators by m^x1\widehat{m}_{x1} and m^y1\widehat{m}_{y1}, and use the remaining n2n_{2} data to estimate σx2\sigma_{x}^{2}, σy2\sigma_{y}^{2}, σxy\sigma_{xy} and ρ\rho. That is,

σ^xy2=n21i=n1+1nϵ^xi1ϵ^yi1,σ^x22=n21i=n1+1nϵ^xi12,σ^y22=n21i=n1+1nϵ^yi12,\displaystyle\widehat{\sigma}_{xy2}=n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\widehat{\epsilon}_{xi1}\widehat{\epsilon}_{yi1},\quad\widehat{\sigma}_{x2}^{2}=n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\widehat{\epsilon}_{xi1}^{2},\quad\widehat{\sigma}_{y2}^{2}=n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\widehat{\epsilon}_{yi1}^{2},

where

ϵ^xi1=Xim^x1(𝐙i),ϵ^yi1=Yim^y1(𝐙i),i=n1+1,,n.\displaystyle\widehat{\epsilon}_{xi1}=X_{i}-\widehat{m}_{x1}({\bf Z}_{i}),\quad\widehat{\epsilon}_{yi1}=Y_{i}-\widehat{m}_{y1}({\bf Z}_{i}),\qquad i=n_{1}+1,\dots,n.

and the final estimator of ρ\rho is

ρ^2=σ^xy2σ^x2σ^y2=i=n1+1nϵ^xi1ϵ^yi1(i=n1+1nϵ^xi12)1/2(i=n1+1nϵ^yi12)1/2.\displaystyle\widehat{\rho}_{2}=\frac{\widehat{\sigma}_{xy2}}{\widehat{\sigma}_{x2}\widehat{\sigma}_{y2}}=\frac{\sum_{i=n_{1}+1}^{n}\widehat{\epsilon}_{xi1}\widehat{\epsilon}_{yi1}}{(\sum_{i=n_{1}+1}^{n}\widehat{\epsilon}_{xi1}^{2})^{1/2}(\sum_{i=n_{1}+1}^{n}\widehat{\epsilon}_{yi1}^{2})^{1/2}}. (14)

We can also switch the roles of the two parts of data, using the later n2n_{2} data to estimate mxm_{x} and mym_{y}, which are denoted similarly by m^x2\widehat{m}_{x2} and m^y2\widehat{m}_{y2}. We then use the first n1n_{1} data to estimate σx2\sigma_{x}^{2}, σy2\sigma_{y}^{2} and σxy\sigma_{xy}, which are denoted similarly by σ^x12\widehat{\sigma}_{x1}^{2}, σ^y12\widehat{\sigma}_{y1}^{2} and σ^xy1\widehat{\sigma}_{xy1}. Then we construct the estimator ρ^1\widehat{\rho}_{1} as

ρ^1=σ^xy1σ^x1σ^y1=i=1n1ϵ^xi2ϵ^yi2(i=1n1ϵ^xi22)1/2(i=1n1ϵ^yi22)1/2,\displaystyle\widehat{\rho}_{1}=\frac{\widehat{\sigma}_{xy1}}{\widehat{\sigma}_{x1}\widehat{\sigma}_{y1}}=\frac{\sum_{i=1}^{n_{1}}\widehat{\epsilon}_{xi2}\widehat{\epsilon}_{yi2}}{(\sum_{i=1}^{n_{1}}\widehat{\epsilon}_{xi2}^{2})^{1/2}(\sum_{i=1}^{n_{1}}\widehat{\epsilon}_{yi2}^{2})^{1/2}},

where

σ^xy1=n11i=1n1ϵ^xi2ϵ^yi2,σ^x12=n11i=1n1ϵ^xi22,σ^y12=n11i=1n1ϵ^yi22,\displaystyle\widehat{\sigma}_{xy1}=n_{1}^{-1}\sum_{i=1}^{n_{1}}\widehat{\epsilon}_{xi2}\widehat{\epsilon}_{yi2},\quad\widehat{\sigma}_{x1}^{2}=n_{1}^{-1}\sum_{i=1}^{n_{1}}\widehat{\epsilon}_{xi2}^{2},\quad\widehat{\sigma}_{y1}^{2}=n_{1}^{-1}\sum_{i=1}^{n_{1}}\widehat{\epsilon}_{yi2}^{2},

with

ϵ^xi2=Xim^x2(𝐙i),ϵ^yi2=Yim^y2(𝐙i),i=1,,n1.\displaystyle\widehat{\epsilon}_{xi2}=X_{i}-\widehat{m}_{x2}({\bf Z}_{i}),\quad\widehat{\epsilon}_{yi2}=Y_{i}-\widehat{m}_{y2}({\bf Z}_{i}),\qquad i=1,\dots,n_{1}.

Taking n1=n2=n/2n_{1}=n_{2}=n/2 for simplicity, we can average the two estimators ρ^1\widehat{\rho}_{1} and ρ^2\widehat{\rho}_{2} to construct the final estimator

ρ^=(ρ^1+ρ^2)/2.\displaystyle\widehat{\rho}=(\widehat{\rho}_{1}+\widehat{\rho}_{2})/2. (15)

3.6 Asymptotic Expansion and Efficiency

In the next theorem, we give the asymptotic properties of ρ^2\widehat{\rho}_{2}. The analogous properties for ρ^1\widehat{\rho}_{1} can be similarly derived.

Theorem 1.

Under model (9), suppose that the nonparametric regression estimators m^xk\widehat{m}_{xk} and m^yk\widehat{m}_{yk} satisfy the convergence rate assumption:

m^xkmx2=op(n11/4),m^ykmy2=op(n11/4),k=1,2,\displaystyle\|\widehat{m}_{xk}-m_{x}\|_{2}=o_{p}(n_{1}^{-1/4}),\qquad\|\widehat{m}_{yk}-m_{y}\|_{2}=o_{p}(n_{1}^{-1/4}),\qquad k=1,2, (16)

where 2\|\cdot\|_{2} denotes the L2(P𝐙)L_{2}(P_{\bf Z})-norm, where P𝐙P_{\bf Z} denotes the marginal distribution of 𝐙{\bf Z}. If n1=n2=n/2n_{1}=n_{2}=n/2, we have

n1/2(ρ^ρ)=n1/2i=1nϕeff(Xi,Yi,𝐙i)+Op(n1/2),\displaystyle n^{1/2}(\widehat{\rho}-\rho)=n^{-1/2}\sum_{i=1}^{n}\phi_{\rm eff}(X_{i},Y_{i},{\bf Z}_{i})+O_{p}(n^{-1/2}), (17)

where ϕeff\phi_{\rm eff} is given by (11).

Note that (17) indicates that the estimator ρ^\widehat{\rho} is indeed efficient under the convergence rate assumptions in (16).

Remark 1 (Effect of regression bias).

In the case where two nonparametric regression estimators have nonvanishing asymptotic bias, the corresponding estimator of residual correlation coefficient will also have some bias. Take ρ^2\widehat{\rho}_{2} as an example. Suppose that the regression estimators m^x1\widehat{m}_{x1} and m^y1\widehat{m}_{y1} converge to the functions mxm_{x}^{*} and mym_{y}^{*}, which may be different from mxm_{x} and mym_{y}. Under similar or weaker convergence assumptions like (16) where mxm_{x} and mym_{y} are replaced by mxm_{x}^{*} and mym_{y}^{*}, we can similarly show that

σ^x22𝑃σx2+var{δx(𝐙)},σ^y22𝑃σy2+var{δy(𝐙)},σ^xy2𝑃σxy+cov{δx(𝐙),δy(𝐙)},\displaystyle\widehat{\sigma}_{x2}^{2}\xrightarrow{P}\sigma_{x}^{2}+\mbox{var}\{\delta_{x}({\bf Z})\},\quad\widehat{\sigma}_{y2}^{2}\xrightarrow{P}\sigma_{y}^{2}+\mbox{var}\{\delta_{y}({\bf Z})\},\quad\widehat{\sigma}_{xy2}\xrightarrow{P}\sigma_{xy}+\mbox{cov}\{\delta_{x}({\bf Z}),\delta_{y}({\bf Z})\},

where δx=mxmx\delta_{x}=m_{x}^{*}-m_{x} and δy=mymy\delta_{y}=m_{y}^{*}-m_{y} are corresponding biases. Thus, by Slutsky’s theorem, we know that

ρ^2=σ^xy2σ^x2σ^y2𝑃σxy+cov{δx(𝐙),δy(𝐙)}[σx2+var{δx(𝐙)}]1/2[σy2+var{δy(𝐙)}]1/2.\displaystyle\widehat{\rho}_{2}=\frac{\widehat{\sigma}_{xy2}}{\widehat{\sigma}_{x2}\widehat{\sigma}_{y2}}\xrightarrow{P}\frac{\sigma_{xy}+\mbox{cov}\{\delta_{x}({\bf Z}),\delta_{y}({\bf Z})\}}{[\sigma_{x}^{2}+\mbox{var}\{\delta_{x}({\bf Z})\}]^{1/2}[\sigma_{y}^{2}+\mbox{var}\{\delta_{y}({\bf Z})\}]^{1/2}}.

Note that the variance terms in the denominator are always inflated by the regression bias, while the numerator can either increase or decrease according to the sign of the covariance term. Therefore, if the true correlation ρ\rho is nonzero, the regression bias is more likely to shrink the residual correlation estimator toward zero, especially when the covariance between the two regression bias terms is relatively small. On the other hand, if ρ=0\rho=0, the regression bias may as well induce some bias due to the cov{δx(𝐙),δy(𝐙)}\mbox{cov}\{\delta_{x}({\bf Z}),\delta_{y}({\bf Z})\} term. The same phenomenon also holds for ρ^1\widehat{\rho}_{1} and ρ^\widehat{\rho}.

3.7 Asymptotic Distribution and Statistical inference

Note that the variance of ϕeff(X,Y,𝐙)\phi_{\rm eff}(X,Y,{\bf Z}) is

E{ϕeff2(X,Y,𝐙)}=E(Seff2)1=(1ρ2)2.\displaystyle E\left\{\phi_{\rm eff}^{2}(X,Y,{\bf Z})\right\}=E(S_{\rm eff}^{2})^{-1}=(1-\rho^{2})^{2}.

The next theorem gives the the asymptotic distribution of ρ^\widehat{\rho}.

Theorem 2.

Under model (9), suppose that the nonparametric regression estimators m^xk\widehat{m}_{xk} and m^yk\widehat{m}_{yk} satisfy (16), for k=1,2k=1,2. Let ρ^\widehat{\rho} be defined by (15). If n1=n2=n/2n_{1}=n_{2}=n/2, then we have

n1/2(ρ^ρ)𝑑N{0,(1ρ2)2}.\displaystyle n^{1/2}(\widehat{\rho}-\rho)\xrightarrow{d}N\left\{0,(1-\rho^{2})^{2}\right\}. (18)

The asymptotic variance in (18) coincides with that in the oracle result (4), indicating that the convergence rate conditions in (16) are sufficient to make the nonparametric regression estimation errors negligible in terms of first-order asymptotics.

Under the null hypothesis ρ=0\rho=0, the asymptotic distribution of ρ^\widehat{\rho} becomes

n1/2ρ^𝑑N(0,1).\displaystyle n^{1/2}\widehat{\rho}\xrightarrow{d}N(0,1).

Therefore, we can construct a Wald test for (3) (19). At significance level α\alpha, our decision rule is to reject H0H_{0} if n1/2|ρ^|>z1α/2n^{1/2}|\widehat{\rho}|>z_{1-\alpha/2}, where z1α/2z_{1-\alpha/2} denotes the (1α/2)(1-\alpha/2)-quantile of the standard normal distribution. Equivalently, the corresponding p-value is given by 2Φ(n1/2|ρ^|)2\Phi(-n^{1/2}|\widehat{\rho}|), where Φ\Phi is the cumulative distribution function of the standard normal distribution.

In general, to construct a confidence interval for ρ\rho, since the asymptotic variance (1ρ2)2(1-\rho^{2})^{2} in (18) involves the unknown parameter ρ\rho, we use the plug-in estimator as (1ρ^2)2(1-\widehat{\rho}^{2})^{2}. Therefore, by Slutsky’s theorem, an asymptotic 100(1α)%100(1-\alpha)\% confidence interval for ρ\rho is given by

ρ^±n1/2z1α/2(1ρ^2).\displaystyle\widehat{\rho}\pm n^{-1/2}z_{1-\alpha/2}(1-\widehat{\rho}^{2}).

4 Simulations

4.1 Simulation Settings

In the simulation studies, we consider two models:

Model 1: 𝐙=(Z1,,Z6),whereZ1,,Z6iidUniform(0,1),\displaystyle{\bf Z}=(Z_{1},\dots,Z_{6})^{\top},\quad\text{where}\ Z_{1},\dots,Z_{6}\overset{\mathrm{iid}}{\sim}\mathrm{Uniform}(0,1),
X=0.4Z1+0.6Z3+ϵx,Y=0.6Z4+0.4Z5+ϵy,\displaystyle X=0.4Z_{1}+0.6\sqrt{Z_{3}}+\epsilon_{x},\quad Y=0.6Z_{4}+0.4\sqrt{Z_{5}}+\epsilon_{y},
Model 2: 𝐙=(Z1,,Z10),whereZ1,,Z10iidUniform(0,1),\displaystyle{\bf Z}=(Z_{1},\dots,Z_{10})^{\top},\quad\text{where}\ Z_{1},\dots,Z_{10}\overset{\mathrm{iid}}{\sim}\mathrm{Uniform}(0,1),
X=(Z1++Z10)/10+ϵx,Y=log(1+Z3+Z6)+ϵy,\displaystyle X=(Z_{1}+\dots+Z_{10})/10+\epsilon_{x},\quad Y=\mbox{log}(1+Z_{3}+Z_{6})+\epsilon_{y},

where in both models, the regression errors (ϵx,ϵy)   𝐙(\epsilon_{x},\epsilon_{y})^{\top}\;\,\rule[0.0pt]{0.29999pt}{6.69998pt}\hskip-2.5pt\rule[0.0pt]{6.49994pt}{0.29999pt}\hskip-2.5pt\rule[0.0pt]{0.29999pt}{6.69998pt}\;\,{\bf Z} and (ϵx,ϵy)N(𝟎,𝚺)(\epsilon_{x},\epsilon_{y})^{\top}\sim N({\bf 0},{\bm{\Sigma}}) with

𝚺=(σ2ρσ2ρσ2σ2).\displaystyle{\bm{\Sigma}}=\left(\begin{matrix}\sigma^{2}&\rho\sigma^{2}\\ \rho\sigma^{2}&\sigma^{2}\end{matrix}\right).

We set σ2=0.2\sigma^{2}=0.2. We take sample sizes to be n=100,200,500,1000,2000,5000n=100,200,500,1000,2000,5000. Under the null hypothesis, we simply set ρ=0\rho=0. Under the alternative hypothesis, we consider two sets of ρ\rho: (1) ρ=±0.25,±0.5,±0.75,±1\rho=\pm 0.25,\pm 0.5,\pm 0.75,\pm 1; (2) ρ=±0.025,±0.05,±0.075,±0.1\rho=\pm 0.025,\pm 0.05,\pm 0.075,\pm 0.1. The former set of ρ\rho indicates a strong dependence signal, which represents deviation from the null hypothesis; the later indicates a weak dependence signal which is hard to detect. For each model, we conduct 500 independent experiments, and the significance level is set as α=0.05\alpha=0.05.

In the simulation studies, we implement our method using residual correlation estimator with sample splitting (RPCS). As is mentioned in Section 3.5, the nonparametric regression estimators m^x\widehat{m}_{x} and m^y\widehat{m}_{y} are fitted on the first part of samples, while the residual correlation estimator ρ^\widehat{\rho} is computed on the second part. We further switch the roles of two parts and construct another estimate, and finally average over the two estimates to get the final result. We also consider a full-data version, referred to as residual correlation estimator with full data (RPCF), in which both the estimation of m^x,m^y\widehat{m}_{x},\widehat{m}_{y} and the computation of ρ^\widehat{\rho} are performed using the entire dataset without sample splitting. As an oracle benchmark, we further include a test based on the Pearson correlation of the true regression errors ϵx\epsilon_{x} and ϵy\epsilon_{y}, which we refer to as residual correlation estimator in the oracle setting (RPCO).

On performing the nonparametric regression for mxm_{x} and mym_{y}, we use Super Learner (38; 28; 29), which combines a collection of candidate regression algorithms including both parametric and nonparametric methods. In our implementation, we include the mean estimator (SL.mean), generalized linear models (SL.glm), penalized linear regression (SL.glmnet), random forests (SL.ranger), gradient boosting trees (SL.xgboost), and neural networks (SL.nnet). The Super Learner is implemented under the Gaussian loss using nonnegative least squares based on the Lawson–Hanson algorithm (method.NNLS) to estimate the ensemble weights for combining the candidate learners. In addition, 5-fold cross-validation is used to evaluate and combine the individual learners.

We compare our method with several existing approaches. The first is the partial correlation test (PaCo), which can be viewed as a special case of our framework in which the regression functions mx(𝐳)m_{x}({\bf z}) and my(𝐳)m_{y}({\bf z}) are restricted to be linear in 𝐳{\bf z}. Partial correlation plays a fundamental role in multivariate analysis (1) and graphical models (18). Moreover, its asymptotic distribution coincides with (18); see Section 5.3 of 23. The second method is based on residual Hilbert–Schmidt independence criterion (RHSIC), which measures the dependence between the residuals ϵ^x\widehat{\epsilon}_{x} and ϵ^y\widehat{\epsilon}_{y} using a kernel-based independence criterion; see, for example, 12; 13. The implementation of RHSIC utilizes the R package dHSIC (27). The next three methods are the residual Randomized Independence Test (RRIT), the Randomized Conditional Independence Test (RCIT), and the Randomized conditional Correlation Test (RCoT). Here, RCIT and RCoT were proposed by 33, while RRIT denotes the unconditional version of RCIT (or RCoT) applied to the residuals ϵ^x\widehat{\epsilon}_{x} and ϵ^y\widehat{\epsilon}_{y}. As shown by 33, RCIT and RCoT achieve comparable or better empirical performance than the Kernel Conditional Independence Test (KCIT) of 42, including similar power and Type I error control, while being substantially more computationally efficient. Therefore, in our simulation studies, we include only RCIT and RCoT as representatives of nonparametric conditional independence tests. We implement RRIT, RCIT and RCoT by the R package RCIT (34).

4.2 Type I Error Control

Under the null hypothesis (ρ=0\rho=0), the empirical levels for Model 1 are reported in Table 1, while the corresponding boxplots of p-values are shown in Figure 1. The analogous results for Model 2 are provided in Table S.1 and Figure S.1 in the supplement. Overall, most methods achieve empirical levels close to the nominal level of 0.05 when the sample size is sufficiently large. For smaller sample sizes, the residual-based tests still maintain levels reasonably close to 0.05. In contrast, the two nonparametric methods, RCIT and RCoT, appear unable to well control the Type I error rate, particularly when n=100n=100 or 200200. A possible explanation is that these methods do not explicitly consider the additive noise structure and may therefore be more sensitive to spurious dependence in small-sample settings.

nn RPCO RPCS RPCF PaCo RHSIC RRIT RCIT RCoT
100 0.074 0.090 0.070 0.080 0.070 0.058 1.000 1.000
200 0.062 0.080 0.066 0.064 0.062 0.054 0.224 0.180
500 0.050 0.058 0.050 0.052 0.048 0.052 0.076 0.088
1000 0.034 0.050 0.036 0.038 0.050 0.046 0.068 0.084
2000 0.046 0.044 0.042 0.042 0.036 0.050 0.054 0.050
5000 0.044 0.034 0.044 0.038 0.044 0.050 0.050 0.030
Table 1: Empirical levels of eight tests under Model 1 based on 500 experiments.
Figure 1: Boxplots of p-values of eight tests for Model 1 under the null hypothesis, with sample sizes n=100,200,500,1000,2000,5000n=100,200,500,1000,2000,5000. The red line represents 0.05.

4.3 Power

Under the alternative hypothesis, we report in Table 2 the empirical powers in Model 1 when ρ\rho is positive, and the results when ρ\rho is negative are symmetric and are reported in Table S.2 of the supplement. We also present the boxplots of p-values for Model 1 in Figures S.2S.5 in the supplement. Analogous results for Model 2 are reported in Tables S.3S.4 and Figures S.6S.9 in the supplement.

ρ\rho nn RPCO RPCS RPCF PaCo RHSIC RRIT RCIT RCoT
0.25 100 0.730 0.644 0.692 0.726 0.328 0.466 1.000 1.000
0.25 200 0.954 0.912 0.940 0.946 0.610 0.804 0.746 0.784
0.25 500 1.000 1.000 1.000 1.000 0.986 0.982 0.944 0.994
0.25 1000 1.000 1.000 1.000 1.000 1.000 0.996 0.990 0.996
0.25 2000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
0.25 5000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
0.50 100 1.000 0.992 1.000 1.000 0.954 0.974 1.000 1.000
0.50 200 1.000 1.000 1.000 1.000 0.998 1.000 0.982 0.994
0.50 500 1.000 1.000 1.000 1.000 1.000 1.000 1.000 0.998
0.50 1000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
0.50 2000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
0.50 5000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
0.75 100 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
0.75 200 1.000 1.000 1.000 1.000 1.000 1.000 0.998 1.000
0.75 500 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
0.75 1000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
0.75 2000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
0.75 5000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
1.00 100 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
1.00 200 1.000 1.000 1.000 1.000 1.000 1.000 0.998 1.000
1.00 500 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
1.00 1000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
1.00 2000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
1.00 5000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
0.025 100 0.064 0.080 0.054 0.066 0.054 0.050 1.000 1.000
0.025 200 0.052 0.064 0.050 0.050 0.052 0.064 0.230 0.250
0.025 500 0.078 0.092 0.076 0.078 0.064 0.074 0.092 0.080
0.025 1000 0.084 0.086 0.086 0.092 0.074 0.078 0.088 0.084
0.025 2000 0.174 0.170 0.172 0.176 0.094 0.128 0.152 0.160
0.025 5000 0.432 0.416 0.418 0.420 0.196 0.286 0.226 0.260
0.050 100 0.068 0.102 0.070 0.074 0.080 0.058 1.000 1.000
0.050 200 0.120 0.144 0.120 0.118 0.064 0.082 0.206 0.222
0.050 500 0.172 0.180 0.176 0.178 0.074 0.118 0.144 0.152
0.050 1000 0.364 0.356 0.358 0.358 0.144 0.250 0.256 0.258
0.050 2000 0.614 0.616 0.614 0.618 0.282 0.448 0.366 0.432
0.050 5000 0.944 0.938 0.942 0.944 0.578 0.820 0.704 0.782
0.075 100 0.120 0.132 0.128 0.130 0.074 0.090 1.000 1.000
0.075 200 0.202 0.198 0.200 0.196 0.108 0.120 0.278 0.282
0.075 500 0.372 0.354 0.358 0.364 0.168 0.232 0.236 0.282
0.075 1000 0.654 0.644 0.660 0.646 0.278 0.468 0.412 0.460
0.075 2000 0.930 0.924 0.926 0.926 0.564 0.772 0.680 0.724
0.075 5000 1.000 1.000 1.000 1.000 0.936 0.970 0.934 0.970
0.100 100 0.168 0.158 0.164 0.172 0.080 0.120 1.000 1.000
0.100 200 0.292 0.288 0.294 0.304 0.132 0.196 0.364 0.336
0.100 500 0.640 0.634 0.654 0.654 0.272 0.452 0.412 0.464
0.100 1000 0.866 0.864 0.864 0.868 0.472 0.692 0.630 0.686
0.100 2000 0.996 0.996 0.996 0.996 0.838 0.928 0.884 0.902
0.100 5000 1.000 1.000 1.000 1.000 1.000 0.996 0.978 0.998
Table 2: Empirical powers of eight tests under Model 1 based on 500 experiments, where the alternative distributions include (1) ρ=0.25,0.5,0.75,1\rho=0.25,0.5,0.75,1 and (2) ρ=0.025,0.05,0.075,0.1\rho=0.025,0.05,0.075,0.1.

Overall, the proposed methods RPCS and RPCF achieve strong empirical power in most settings, especially when the dependence signal or the sample size is not too small. In most cases, RPCS and RPCF perform similarly to the oracle procedure RPCO, showing that the proposed residual-correlation-based approach performs nearly as well as the ideal procedure using the true regression errors.

For relatively strong dependence signals, i.e., ρ\rho in set (1), all residual-correlation-based methods achieve power close to 1 when the sample size is sufficiently large. In particular, RPCS and RPCF remain very close to the oracle benchmark RPCO in most settings, suggesting that estimating the regression functions causes only a small loss of efficiency. As the sample size increases, the differences among the three procedures quickly become negligible. In contrast, although RHSIC and RRIT also achieve high power for large sample sizes, their performance is noticeably worse when the sample size is small.

For relatively weak dependence signals, i.e., ρ\rho in set (2), RPCS and RPCF still show increasing power as either the signal strength or the sample size increases, and they continue to perform similarly to RPCO in most settings. For example, under Model 1 with ρ=0.05\rho=0.05 and moderate or large sample sizes, the powers of RPCS and RPCF are already very close to those of RPCO. These results suggest that the proposed methods remain effective even when the conditional dependence is weak. Compared with RHSIC and RRIT, the proposed methods generally achieve higher power under weak dependence signals, particularly when the sample size is small or moderate. This suggests that directly using the residual correlation structure under GANM improves the ability to detect weak dependence.

In addition, in both settings with weak and strong signals, RPCS and RPCF perform very similarly across all settings, indicating that sample splitting causes only a small loss of efficiency in finite samples.

4.4 Estimation Efficiency

Table and Tables S.5S.7 in the supplement further compare the estimation efficiency of the proposed residual correlation estimators, including RPCS, RPCF, RPCO and PaCo. We consider the cases where ρ\rho is in set (1) without the setting ρ=±1\rho=\pm 1, because in this case, the true asymptotic variance is (1ρ2)2=0(1-\rho^{2})^{2}=0. In all the tables, SD^\widehat{\rm SD} is computed based on the average of the estimated asymptotic standard deviations, which is n1/2(1ρ^2)n^{-1/2}(1-\widehat{\rho}^{2}), and 95% cvg is the empirical coverage of the 95% asymptotic confidence intervals given by ρ^±n1/2z1α/2(1ρ^2)\widehat{\rho}\pm n^{-1/2}z_{1-\alpha/2}(1-\widehat{\rho}^{2}).

4.5 Strong Nonlinear Effects

In the previous simulation settings, the nonlinear regression structures are relatively smooth and can still be reasonably approximated by linear relationships. As a result, the partial-correlation-based method PaCo remains competitive in many settings. To further investigate the effect of nonlinear nuisance regression, we additionally consider a more challenging null setting in which the conditional mean functions are strongly nonlinear while the true correlation of the regression errors remains ρ=0\rho=0.

Specifically, we consider

Model 3: 𝐙=(Z1,Z2),whereZ1,Z2iidUniform(0,1),\displaystyle{\bf Z}=(Z_{1},Z_{2})^{\top},\quad\text{where}\ Z_{1},Z_{2}\overset{\mathrm{iid}}{\sim}\mathrm{Uniform}(0,1),
X=sin(2πZ1)+4(Z20.5)2+ϵx,Y=cos(4πZ1)+4(Z20.5)2+ϵy,\displaystyle X=\sin(2\pi Z_{1})+4(Z_{2}-0.5)^{2}+\epsilon_{x},\quad Y=\cos(4\pi Z_{1})+4(Z_{2}-0.5)^{2}+\epsilon_{y},

where the distribution of (ϵx,ϵy)(\epsilon_{x},\epsilon_{y})^{\top} is same as in Section 4.1, and ρ=0\rho=0. We report the empirical levels and boxplots of p-values for the eight estimators under this setting as Table 3 and Figure 2, as well as the estimation results in Table S.8 in the supplement.

ρ\rho nn RPCO RPCS RPCF PaCo RHSIC RRIT RCIT RCoT
0 100 0.046 0.112 0.054 0.318 0.056 0.032 0.126 0.110
0 200 0.040 0.092 0.072 0.452 0.048 0.052 0.108 0.080
0 500 0.044 0.056 0.054 0.902 0.060 0.054 0.072 0.072
0 1000 0.048 0.110 0.076 1.000 0.088 0.072 0.076 0.064
0 2000 0.060 0.108 0.082 1.000 0.054 0.064 0.078 0.076
0 5000 0.044 0.106 0.060 1.000 0.060 0.064 0.170 0.174
Table 3: Empirical levels of eight tests under Model 3 based on 500 experiments.
Figure 2: Boxplots of p-values of eight tests for Model 3 under the null hypothesis, with sample sizes n=100,200,500,1000,2000,5000n=100,200,500,1000,2000,5000. The red line represents 0.05.

As shown in Table 3 and Figure 2, all tests except PaCo continue to maintain reasonably accurate empirical levels under the strong nonlinear setting. In contrast, PaCo has substantially inflated Type I error rates, and most of its p-values are concentrated near 0, especially when the sample size is large. Furthermore, Table S.8 shows that PaCo also produces large biases in the estimation of ρ^\widehat{\rho}. These results indicate that flexible nonparametric regression is essential in this setting. In particular, linear regression fails to adequately capture the nonlinear effects of 𝐙{\bf Z} on XX and YY, thereby leaving substantial residual dependence and causing PaCo to reject the null hypothesis much more frequently than the nominal level. The observed estimation bias is also consistent with Remark 1, where regression bias may induce additional residual correlation even under the null hypothesis ρ=0\rho=0.

5 Data Application

We collected daily adjusted closing prices for 12 representative U.S. stocks, including Apple (AAPL), Microsoft (MSFT), NVIDIA (NVDA), Alphabet (GOOGL), Amazon (AMZN), JPMorgan Chase (JPM), Bank of America (BAC), Goldman Sachs (GS), ExxonMobil (XOM), Chevron (CVX), Walmart (WMT), and Costco (COST), together with several observed market factors, including the S&P 500 ETF (SPY), the volatility index (VIX), long-term treasury bonds (TLT), oil prices (USO), and the U.S. dollar index (UUP), from Yahoo Finance using the R package quantmod (30) over the period from January 1, 2018 to January 1, 2024. Adjusted prices were used to account for stock splits and dividends. Daily log returns were computed as differences of the logarithms of consecutive adjusted prices. Observations containing missing values were removed to ensure complete alignment across all variables and factors. The resulting cleaned dataset was then separated into the stock return variables of interest 𝐗{\bf X} and the observed market factor variables 𝐙{\bf Z}. Here, 𝐗{\bf X} represents the daily log returns of the 12 individual stocks, while 𝐙{\bf Z} contains 5 market-wide factors intended to capture common variation shared across stock returns and serves as the conditioning variables in the subsequent conditional dependence analysis. After the cleaning process, the sample size is n=1453n=1453.

We further conduct pairwise conditional independence tests among the 12 stocks based on the proposed residual correlation test under the additive noise model (ANM). Specifically, for each pair of stocks (Xi,Xj)(X_{i},X_{j}), for 1i<j121\leq i<j\leq 12, we test whether

Xi   Xj|𝐙,\displaystyle X_{i}\;\,\rule[0.0pt]{0.29999pt}{6.69998pt}\hskip-2.5pt\rule[0.0pt]{6.49994pt}{0.29999pt}\hskip-2.5pt\rule[0.0pt]{0.29999pt}{6.69998pt}\;\,X_{j}|{\bf Z},

where 𝐙{\bf Z} consists of the observed market factors represented by SPY, VIX, TLT, USO, and UUP. Under the ANM framework, each stock return is modeled as a nonparametric function of 𝐙{\bf Z} plus an independent additive noise term, and the proposed test is then applied to the residuals to determine whether any remaining conditional dependence exists after conditioning on these observed market factors. This analysis allows us to investigate the dependence structure among stocks beyond the effects explained by the common market factors.

Figure 3: Heatmap of pairwise estimated Pearson correlations of residuals.
Figure 4: Estimated graph based on the conditional independence test.

Figure 4 presents the heatmap of the absolute values of estimated pairwise residual correlations after conditioning on the observed market factors 𝐙{\bf Z}. The residual correlations are estimated by RPCS, while the nonparametric regressions are fitted using Super Learner (38; 28; 29), under the same settings as in Section 4.1. Larger absolute values in the heatmap indicate stronger remaining conditional dependence between the corresponding pairs of stocks after removing the common effects explained by SPY, VIX, TLT, USO, and UUP. Several sector-related dependence patterns can still be observed after conditioning on the market factors. In particular, relatively strong residual dependence appears among the financial stocks JPM, BAC, and GS, as well as between the energy stocks XOM and CVX. Although some cross-sector pairs exhibit weaker dependence after conditioning on the market factors, many stock pairs still retain noticeable residual dependence.

Figure 4 further visualizes the estimated conditional dependence structure through a graph constructed from the pairwise conditional independence tests based on RPCS. In the graph, each node represents a stock, and an edge is included when the null hypothesis of conditional independence is rejected for the corresponding pair of stocks. The resulting network exhibits many connections across the stocks, indicating that substantial residual dependence remains even after conditioning on the observed market factors. These findings suggest that, although the observed market factors explain part of the common market variation, important residual relationships among individual stocks still persist.

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Supplementary Materials

S.1 Proofs

Proof of Proposition 1.

Note that

Sσx(x,y,𝐳)=1σx+11ρ2ϵx2σx3ρ1ρ2ϵxϵyσx2σy.\displaystyle S_{\sigma_{x}}(x,y,{\bf z})=-\frac{1}{\sigma_{x}}+\frac{1}{1-\rho^{2}}\frac{\epsilon_{x}^{2}}{\sigma_{x}^{3}}-\frac{\rho}{1-\rho^{2}}\frac{\epsilon_{x}\epsilon_{y}}{\sigma_{x}^{2}\sigma_{y}}.

Thus, the nuisance tangent space for σx\sigma_{x} is

Λ1={c1Sσx(x,y,𝐳)}={c1(1σx+11ρ2ϵx2σx3ρ1ρ2ϵxϵyσx2σy)}.\displaystyle\Lambda_{1}=\{c_{1}S_{\sigma_{x}}(x,y,{\bf z})\}=\left\{c_{1}\left(-\frac{1}{\sigma_{x}}+\frac{1}{1-\rho^{2}}\frac{\epsilon_{x}^{2}}{\sigma_{x}^{3}}-\frac{\rho}{1-\rho^{2}}\frac{\epsilon_{x}\epsilon_{y}}{\sigma_{x}^{2}\sigma_{y}}\right)\right\}.

Similarly, the nuisance tangent space for σy\sigma_{y} is

Sσy(x,y,𝐳)=1σy+11ρ2ϵy2σy3ρ1ρ2ϵxϵyσxσy2.\displaystyle S_{\sigma_{y}}(x,y,{\bf z})=-\frac{1}{\sigma_{y}}+\frac{1}{1-\rho^{2}}\frac{\epsilon_{y}^{2}}{\sigma_{y}^{3}}-\frac{\rho}{1-\rho^{2}}\frac{\epsilon_{x}\epsilon_{y}}{\sigma_{x}\sigma_{y}^{2}}.

And

Λ2={c2Sσy(x,y,𝐳)}={c2(1σy+11ρ2ϵy2σy3ρ1ρ2ϵxϵyσxσy2)}.\displaystyle\Lambda_{2}=\{c_{2}S_{\sigma_{y}}(x,y,{\bf z})\}=\left\{c_{2}\left(-\frac{1}{\sigma_{y}}+\frac{1}{1-\rho^{2}}\frac{\epsilon_{y}^{2}}{\sigma_{y}^{3}}-\frac{\rho}{1-\rho^{2}}\frac{\epsilon_{x}\epsilon_{y}}{\sigma_{x}\sigma_{y}^{2}}\right)\right\}.

Then, let Λ3\Lambda_{3} be the nuisance tangent space for mxm_{x}. Take mx(𝐳)=m0(𝐳)+γxB1(𝐳)m_{x}({\bf z})=m_{0}({\bf z})+\gamma_{x}B_{1}({\bf z}) as a parametric submodel of mx(𝐳)m_{x}({\bf z}). Thus,

Sγx|γx=0\displaystyle S_{\gamma_{x}}|_{\gamma_{x}=0} =\displaystyle= 12(1ρ2)[2ϵx{B1(𝐳)}σx22ρϵy{B1(𝐳)}σxσy]\displaystyle-\frac{1}{2(1-\rho^{2})}\left[\frac{2\epsilon_{x}\{-B_{1}({\bf z})\}}{\sigma_{x}^{2}}-2\rho\frac{\epsilon_{y}\{-B_{1}({\bf z})\}}{\sigma_{x}\sigma_{y}}\right]
=\displaystyle= 11ρ2(ϵxσx2ρϵyσxσy)B1(𝐳).\displaystyle\frac{1}{1-\rho^{2}}\left(\frac{\epsilon_{x}}{\sigma_{x}^{2}}-\rho\frac{\epsilon_{y}}{\sigma_{x}\sigma_{y}}\right)B_{1}({\bf z}).

Denote

A={11ρ2(ϵxσx2ρϵyσxσy)B1(𝐳)}.\displaystyle A=\left\{\frac{1}{1-\rho^{2}}\left(\frac{\epsilon_{x}}{\sigma_{x}^{2}}-\rho\frac{\epsilon_{y}}{\sigma_{x}\sigma_{y}}\right)B_{1}({\bf z})\right\}.

Note that mx(𝐳)=m0(𝐳)+γxB1(𝐳)m_{x}({\bf z})=m_{0}({\bf z})+\gamma_{x}B_{1}({\bf z}) is a parametric submodel of mx(𝐳)m_{x}({\bf z}), so AΛ3A\subset\Lambda_{3}. On the other hand, for any parametric submodel mx(𝐳,γ)m_{x}({\bf z},\gamma) with γ=γ0\gamma=\gamma_{0} leading to the truth, we have

logfγ|γ=γ0\displaystyle\frac{\partial\mbox{log}f}{\partial\gamma}\Big|_{\gamma=\gamma_{0}} =\displaystyle= 12(1ρ2)[2ϵxσx2{mx(𝐳,γ)γ|γ=γ0}2ρϵyσxσy{mx(𝐳,γ)γ|γ=γ0}]\displaystyle-\frac{1}{2(1-\rho^{2})}\left[\frac{2\epsilon_{x}}{\sigma_{x}^{2}}\left\{-\frac{\partial m_{x}({\bf z},\gamma)}{\partial\gamma}\Big|_{\gamma=\gamma_{0}}\right\}-2\rho\frac{\epsilon_{y}}{\sigma_{x}\sigma_{y}}\left\{-\frac{\partial m_{x}({\bf z},\gamma)}{\partial\gamma}\Big|_{\gamma=\gamma_{0}}\right\}\right]
=\displaystyle= 11ρ2(ϵxσx2ρϵyσxσy){mx(𝐳,γ)γ|γ=γ0}A,\displaystyle\frac{1}{1-\rho^{2}}\left(\frac{\epsilon_{x}}{\sigma_{x}^{2}}-\rho\frac{\epsilon_{y}}{\sigma_{x}\sigma_{y}}\right)\left\{\frac{\partial m_{x}({\bf z},\gamma)}{\partial\gamma}\Big|_{\gamma=\gamma_{0}}\right\}\in A,

so Λ3A\Lambda_{3}\subset A. Since both Λ3\Lambda_{3} and AA are closed, we have Λ3=A\Lambda_{3}=A, i.e.,

Λ3={11ρ2(ϵxσx2ρϵyσxσy)B1(𝐳)}.\displaystyle\Lambda_{3}=\left\{\frac{1}{1-\rho^{2}}\left(\frac{\epsilon_{x}}{\sigma_{x}^{2}}-\rho\frac{\epsilon_{y}}{\sigma_{x}\sigma_{y}}\right)B_{1}({\bf z})\right\}.

Similarly, the nuisance tangent space for mym_{y} is

Λ4={11ρ2(ϵyσy2ρϵxσxσy)B2(𝐳)}.\displaystyle\Lambda_{4}=\left\{\frac{1}{1-\rho^{2}}\left(\frac{\epsilon_{y}}{\sigma_{y}^{2}}-\rho\frac{\epsilon_{x}}{\sigma_{x}\sigma_{y}}\right)B_{2}({\bf z})\right\}.

Obviously, the nuisance tangent space for f𝐙f_{\bf Z} is

Λ5={a(𝐳):E(a)=0}.\displaystyle\Lambda_{5}=\{a({\bf z}):E(a)=0\}.

Summarizing the above results gives

Λ=Λ1+Λ2+Λ3+Λ4+Λ5.\displaystyle\Lambda=\Lambda_{1}+\Lambda_{2}+\Lambda_{3}+\Lambda_{4}+\Lambda_{5}.

Proof of Proposition 2.

We then check the orthogonality of the five spaces above. For any B1(𝐳)B_{1}({\bf z}), we have

E{(1σx+11ρ2ϵx2σx3ρ1ρ2ϵxϵyσx2σy)11ρ2(ϵxσx2ϵyσxσy)B1(𝐙)}\displaystyle E\left\{\left(-\frac{1}{\sigma_{x}}+\frac{1}{1-\rho^{2}}\frac{\epsilon_{x}^{2}}{\sigma_{x}^{3}}-\frac{\rho}{1-\rho^{2}}\frac{\epsilon_{x}\epsilon_{y}}{\sigma_{x}^{2}\sigma_{y}}\right)\frac{1}{1-\rho^{2}}\left(\frac{\epsilon_{x}}{\sigma_{x}^{2}}-\frac{\epsilon_{y}}{\sigma_{x}\sigma_{y}}\right)B_{1}({\bf Z})\right\}
=\displaystyle= E{(1σx+11ρ2ϵx2σx3ρ1ρ2ϵxϵyσx2σy)11ρ2(ϵxσx2ϵyσxσy)}E{B1(𝐙)}\displaystyle E\left\{\left(-\frac{1}{\sigma_{x}}+\frac{1}{1-\rho^{2}}\frac{\epsilon_{x}^{2}}{\sigma_{x}^{3}}-\frac{\rho}{1-\rho^{2}}\frac{\epsilon_{x}\epsilon_{y}}{\sigma_{x}^{2}\sigma_{y}}\right)\frac{1}{1-\rho^{2}}\left(\frac{\epsilon_{x}}{\sigma_{x}^{2}}-\frac{\epsilon_{y}}{\sigma_{x}\sigma_{y}}\right)\right\}E\left\{B_{1}({\bf Z})\right\}
=\displaystyle= 0,\displaystyle 0,

since this only includes the first and third moments of a multivariate normal distribution. Thus, Λ1Λ3\Lambda_{1}\perp\Lambda_{3}. Similarly, Λ1Λ4\Lambda_{1}\perp\Lambda_{4}, Λ2Λ3\Lambda_{2}\perp\Lambda_{3}, Λ2Λ4\Lambda_{2}\perp\Lambda_{4}.

For a(𝐳)Λ5a({\bf z})\in\Lambda_{5}, we have

E{(1σx+11ρ2ϵx2σx3ρ1ρ2ϵxϵyσx2σy)a(𝐙)}\displaystyle E\left\{\left(-\frac{1}{\sigma_{x}}+\frac{1}{1-\rho^{2}}\frac{\epsilon_{x}^{2}}{\sigma_{x}^{3}}-\frac{\rho}{1-\rho^{2}}\frac{\epsilon_{x}\epsilon_{y}}{\sigma_{x}^{2}\sigma_{y}}\right)a({\bf Z})\right\}
=\displaystyle= E(1σx+11ρ2ϵx2σx3ρ1ρ2ϵxϵyσx2σy)E{a(𝐙)}\displaystyle E\left(-\frac{1}{\sigma_{x}}+\frac{1}{1-\rho^{2}}\frac{\epsilon_{x}^{2}}{\sigma_{x}^{3}}-\frac{\rho}{1-\rho^{2}}\frac{\epsilon_{x}\epsilon_{y}}{\sigma_{x}^{2}\sigma_{y}}\right)E\left\{a({\bf Z})\right\}
=\displaystyle= 0.\displaystyle 0.

Thus, Λ1Λ5\Lambda_{1}\perp\Lambda_{5}. Similarly, Λ2Λ5\Lambda_{2}\perp\Lambda_{5}.

For a(𝐳)Λ5a({\bf z})\in\Lambda_{5} and any B1(𝐳)B_{1}({\bf z}),

E[11ρ2{ϵxσx2ρϵyσxσy}B1(𝐙)a(𝐙)]=11ρ2E{ϵxσx2ρϵyσxσy}E[B1(𝐙)a(𝐙)]=0.\displaystyle E\left[\frac{1}{1-\rho^{2}}\left\{\frac{\epsilon_{x}}{\sigma_{x}^{2}}-\rho\frac{\epsilon_{y}}{\sigma_{x}\sigma_{y}}\right\}B_{1}({\bf Z})a({\bf Z})\right]=\frac{1}{1-\rho^{2}}E\left\{\frac{\epsilon_{x}}{\sigma_{x}^{2}}-\rho\frac{\epsilon_{y}}{\sigma_{x}\sigma_{y}}\right\}E\left[B_{1}({\bf Z})a({\bf Z})\right]=0.

Thus, Λ3Λ5\Lambda_{3}\perp\Lambda_{5}. Similarly, Λ4Λ5\Lambda_{4}\perp\Lambda_{5}.

However,

E(SσySσx)\displaystyle E(S_{\sigma_{y}}S_{\sigma_{x}})
=\displaystyle= E{(1σx+11ρ2ϵx2σx3ρ1ρ2ϵxϵyσx2σy)(1σy+11ρ2ϵy2σy3ρ1ρ2ϵxϵyσxσy2)}\displaystyle E\left\{\left(-\frac{1}{\sigma_{x}}+\frac{1}{1-\rho^{2}}\frac{\epsilon_{x}^{2}}{\sigma_{x}^{3}}-\frac{\rho}{1-\rho^{2}}\frac{\epsilon_{x}\epsilon_{y}}{\sigma_{x}^{2}\sigma_{y}}\right)\left(-\frac{1}{\sigma_{y}}+\frac{1}{1-\rho^{2}}\frac{\epsilon_{y}^{2}}{\sigma_{y}^{3}}-\frac{\rho}{1-\rho^{2}}\frac{\epsilon_{x}\epsilon_{y}}{\sigma_{x}\sigma_{y}^{2}}\right)\right\}
=\displaystyle= 1σxσy{111ρ2+ρ21ρ211ρ2+1+2ρ2(1ρ2)23ρ2(1ρ2)2+ρ21ρ2\displaystyle\frac{1}{\sigma_{x}\sigma_{y}}\left\{1-\frac{1}{1-\rho^{2}}+\frac{\rho^{2}}{1-\rho^{2}}-\frac{1}{1-\rho^{2}}+\frac{1+2\rho^{2}}{(1-\rho^{2})^{2}}-\frac{3\rho^{2}}{(1-\rho^{2})^{2}}+\frac{\rho^{2}}{1-\rho^{2}}\right.
3ρ2(1ρ2)2+ρ2(1+2ρ2)(1ρ2)2}\displaystyle\left.\qquad\quad-\frac{3\rho^{2}}{(1-\rho^{2})^{2}}+\frac{\rho^{2}(1+2\rho^{2})}{(1-\rho^{2})^{2}}\right\}
=\displaystyle= 1σxσyρ21ρ2\displaystyle-\frac{1}{\sigma_{x}\sigma_{y}}\frac{\rho^{2}}{1-\rho^{2}}
\displaystyle\neq 0,\displaystyle 0,

so Λ1⟂̸Λ2\Lambda_{1}\not\perp\Lambda_{2}. Also,

E{11ρ2(ϵxσx2ρϵyσxσy)B1(𝐙)11ρ2(ϵyσy2ρϵxσxσy)B2(𝐙)}\displaystyle E\left\{\frac{1}{1-\rho^{2}}\left(\frac{\epsilon_{x}}{\sigma_{x}^{2}}-\rho\frac{\epsilon_{y}}{\sigma_{x}\sigma_{y}}\right)B_{1}({\bf Z})\frac{1}{1-\rho^{2}}\left(\frac{\epsilon_{y}}{\sigma_{y}^{2}}-\rho\frac{\epsilon_{x}}{\sigma_{x}\sigma_{y}}\right)B_{2}({\bf Z})\right\}
=\displaystyle= 1(1ρ2)2E{(ϵxσx2ρϵyσxσy)(ϵyσy2ρϵxσxσy)}E{B1(𝐙)B2(𝐙)}\displaystyle\frac{1}{(1-\rho^{2})^{2}}E\left\{\left(\frac{\epsilon_{x}}{\sigma_{x}^{2}}-\rho\frac{\epsilon_{y}}{\sigma_{x}\sigma_{y}}\right)\left(\frac{\epsilon_{y}}{\sigma_{y}^{2}}-\rho\frac{\epsilon_{x}}{\sigma_{x}\sigma_{y}}\right)\right\}E\left\{B_{1}({\bf Z})B_{2}({\bf Z})\right\}
=\displaystyle= 1(1ρ2)21σxσy(ρρρ+ρ3)E{B1(𝐙)B2(𝐙)}\displaystyle\frac{1}{(1-\rho^{2})^{2}}\frac{1}{\sigma_{x}\sigma_{y}}\left(\rho-\rho-\rho+\rho^{3}\right)E\left\{B_{1}({\bf Z})B_{2}({\bf Z})\right\}
=\displaystyle= ρ1ρ21σxσyE{B1(𝐙)B2(𝐙)}\displaystyle-\frac{\rho}{1-\rho^{2}}\frac{1}{\sigma_{x}\sigma_{y}}E\left\{B_{1}({\bf Z})B_{2}({\bf Z})\right\}
\displaystyle\neq 0,\displaystyle 0,

so Λ3⟂̸Λ4\Lambda_{3}\not\perp\Lambda_{4}.

We now do orthogonalization on the above two pairs. First, we find cc such that

E{(SσycSσx)Sσx}=0.\displaystyle E\left\{(S_{\sigma_{y}}-cS_{\sigma_{x}})S_{\sigma_{x}}\right\}=0.

Notice that

E(Sσx2)\displaystyle E\left(S_{\sigma_{x}}^{2}\right) =\displaystyle= E{(1σx+11ρ2ϵx2σx3ρ1ρ2ϵxϵyσx2σy)2}\displaystyle E\left\{\left(-\frac{1}{\sigma_{x}}+\frac{1}{1-\rho^{2}}\frac{\epsilon_{x}^{2}}{\sigma_{x}^{3}}-\frac{\rho}{1-\rho^{2}}\frac{\epsilon_{x}\epsilon_{y}}{\sigma_{x}^{2}\sigma_{y}}\right)^{2}\right\}
=\displaystyle= 1σx2{1+3(1ρ2)2+ρ2(1+2ρ2)(1ρ2)221ρ2+2ρ21ρ26ρ2(1ρ2)2}\displaystyle\frac{1}{\sigma_{x}^{2}}\left\{1+\frac{3}{(1-\rho^{2})^{2}}+\frac{\rho^{2}(1+2\rho^{2})}{(1-\rho^{2})^{2}}-\frac{2}{1-\rho^{2}}+\frac{2\rho^{2}}{1-\rho^{2}}-\frac{6\rho^{2}}{(1-\rho^{2})^{2}}\right\}
=\displaystyle= 1σx22ρ21ρ2.\displaystyle\frac{1}{\sigma_{x}^{2}}\frac{2-\rho^{2}}{1-\rho^{2}}.

Therefore,

c=E(SσySσx)E(Sσx2)=1σxσyρ21ρ21σx22ρ21ρ2=σxσyρ22ρ2.\displaystyle c=\frac{E(S_{\sigma_{y}}S_{\sigma_{x}})}{E(S_{\sigma_{x}}^{2})}=\frac{-\frac{1}{\sigma_{x}\sigma_{y}}\frac{\rho^{2}}{1-\rho^{2}}}{\frac{1}{\sigma_{x}^{2}}\frac{2-\rho^{2}}{1-\rho^{2}}}=-\frac{\sigma_{x}}{\sigma_{y}}\frac{\rho^{2}}{2-\rho^{2}}.

We set

Λ~2\displaystyle\widetilde{\Lambda}_{2} =\displaystyle= {c2(1σy+11ρ2ϵy2σy3ρ1ρ2ϵxϵyσxσy2)\displaystyle\left\{c_{2}\left(-\frac{1}{\sigma_{y}}+\frac{1}{1-\rho^{2}}\frac{\epsilon_{y}^{2}}{\sigma_{y}^{3}}-\frac{\rho}{1-\rho^{2}}\frac{\epsilon_{x}\epsilon_{y}}{\sigma_{x}\sigma_{y}^{2}}\right)\right.
+c2σxσyρ22ρ2(1σx+11ρ2ϵx2σx3ρ1ρ2ϵxϵyσx2σy)}\displaystyle\left.\quad+c_{2}\frac{\sigma_{x}}{\sigma_{y}}\frac{\rho^{2}}{2-\rho^{2}}\left(-\frac{1}{\sigma_{x}}+\frac{1}{1-\rho^{2}}\frac{\epsilon_{x}^{2}}{\sigma_{x}^{3}}-\frac{\rho}{1-\rho^{2}}\frac{\epsilon_{x}\epsilon_{y}}{\sigma_{x}^{2}\sigma_{y}}\right)\right\}
=\displaystyle= {c2{22ρ21σy+11ρ2ϵy2σy3+ρ2(1ρ2)(2ρ2)ϵx2σx2σy2ρ(1ρ2)(2ρ2)ϵxϵyσxσy2}}.\displaystyle\left\{c_{2}\left\{-\frac{2}{2-\rho^{2}}\frac{1}{\sigma_{y}}+\frac{1}{1-\rho^{2}}\frac{\epsilon_{y}^{2}}{\sigma_{y}^{3}}+\frac{\rho^{2}}{(1-\rho^{2})(2-\rho^{2})}\frac{\epsilon_{x}^{2}}{\sigma_{x}^{2}\sigma_{y}}-\frac{2\rho}{(1-\rho^{2})(2-\rho^{2})}\frac{\epsilon_{x}\epsilon_{y}}{\sigma_{x}\sigma_{y}^{2}}\right\}\right\}.

Then, for an arbitrary B2(𝐳)B_{2}({\bf z}), we want to find B(𝐳)B({\bf z}) such that

E[{(ϵyσy2ρϵxσxσy)B2(𝐙)(ϵxσx2ρϵyσxσy)B(𝐙)}{(ϵxσx2ρϵyσxσy)B1(𝐙)}]=0\displaystyle E\left[\left\{\left(\frac{\epsilon_{y}}{\sigma_{y}^{2}}-\rho\frac{\epsilon_{x}}{\sigma_{x}\sigma_{y}}\right)B_{2}({\bf Z})-\left(\frac{\epsilon_{x}}{\sigma_{x}^{2}}-\rho\frac{\epsilon_{y}}{\sigma_{x}\sigma_{y}}\right)B({\bf Z})\right\}\left\{\left(\frac{\epsilon_{x}}{\sigma_{x}^{2}}-\rho\frac{\epsilon_{y}}{\sigma_{x}\sigma_{y}}\right)B_{1}({\bf Z})\right\}\right]=0

for all B1(𝐳)B_{1}({\bf z}). Since

E[{(ϵyσy2ρϵxσxσy)B2(𝐙)(ϵxσx2ρϵyσxσy)B(𝐙)}{(ϵxσx2ρϵyσxσy)B1(𝐙)}]\displaystyle E\left[\left\{\left(\frac{\epsilon_{y}}{\sigma_{y}^{2}}-\rho\frac{\epsilon_{x}}{\sigma_{x}\sigma_{y}}\right)B_{2}({\bf Z})-\left(\frac{\epsilon_{x}}{\sigma_{x}^{2}}-\rho\frac{\epsilon_{y}}{\sigma_{x}\sigma_{y}}\right)B({\bf Z})\right\}\left\{\left(\frac{\epsilon_{x}}{\sigma_{x}^{2}}-\rho\frac{\epsilon_{y}}{\sigma_{x}\sigma_{y}}\right)B_{1}({\bf Z})\right\}\right]
=\displaystyle= E[{(ϵyσy2ρϵxσxσy)(ϵxσx2ρϵyσxσy)}B2(𝐙)B1(𝐙)(ϵxσx2ρϵyσxσy)2B(𝐙)B1(𝐙)]\displaystyle E\left[\left\{\left(\frac{\epsilon_{y}}{\sigma_{y}^{2}}-\rho\frac{\epsilon_{x}}{\sigma_{x}\sigma_{y}}\right)\left(\frac{\epsilon_{x}}{\sigma_{x}^{2}}-\rho\frac{\epsilon_{y}}{\sigma_{x}\sigma_{y}}\right)\right\}B_{2}({\bf Z})B_{1}({\bf Z})-\left(\frac{\epsilon_{x}}{\sigma_{x}^{2}}-\rho\frac{\epsilon_{y}}{\sigma_{x}\sigma_{y}}\right)^{2}B({\bf Z})B_{1}({\bf Z})\right]
=\displaystyle= E{1σxσy(ρρρ+ρ3)B2(𝐙)B1(𝐙)1σx2(1+ρ22ρ2)B(𝐙)B1(𝐙)}\displaystyle E\left\{\frac{1}{\sigma_{x}\sigma_{y}}(\rho-\rho-\rho+\rho^{3})B_{2}({\bf Z})B_{1}({\bf Z})-\frac{1}{\sigma_{x}^{2}}(1+\rho^{2}-2\rho^{2})B({\bf Z})B_{1}({\bf Z})\right\}
=\displaystyle= E[{1σxσy(ρ3ρ)B2(𝐙)1σx2(1ρ2)B(𝐙)}B1(𝐙)],\displaystyle E\left[\left\{\frac{1}{\sigma_{x}\sigma_{y}}(\rho^{3}-\rho)B_{2}({\bf Z})-\frac{1}{\sigma_{x}^{2}}(1-\rho^{2})B({\bf Z})\right\}B_{1}({\bf Z})\right],

then we take

B(𝐳)=σxσyρB2(𝐳).\displaystyle B({\bf z})=-\frac{\sigma_{x}}{\sigma_{y}}\rho B_{2}({\bf z}).

We set

Λ~4\displaystyle\widetilde{\Lambda}_{4} =\displaystyle= {11ρ2(ϵyσy2ρϵxσxσy)B2(𝐳)+11ρ2(ϵxσx2ρϵyσxσy)σxσyρB2(𝐳)}\displaystyle\left\{\frac{1}{1-\rho^{2}}\left(\frac{\epsilon_{y}}{\sigma_{y}^{2}}-\rho\frac{\epsilon_{x}}{\sigma_{x}\sigma_{y}}\right)B_{2}({\bf z})+\frac{1}{1-\rho^{2}}\left(\frac{\epsilon_{x}}{\sigma_{x}^{2}}-\rho\frac{\epsilon_{y}}{\sigma_{x}\sigma_{y}}\right)\frac{\sigma_{x}}{\sigma_{y}}\rho B_{2}({\bf z})\right\}
=\displaystyle= {ϵyσy2B2(𝐳)}.\displaystyle\left\{\frac{\epsilon_{y}}{\sigma_{y}^{2}}B_{2}({\bf z})\right\}.

Therefore,

Λ=Λ1Λ~2Λ3Λ~4Λ5,\displaystyle\Lambda=\Lambda_{1}\oplus\widetilde{\Lambda}_{2}\oplus\Lambda_{3}\oplus\widetilde{\Lambda}_{4}\oplus\Lambda_{5}, (S.1)

where

Λ1\displaystyle\Lambda_{1} =\displaystyle= {c1(1σx+11ρ2ϵx2σx3ρ1ρ2ϵxϵyσx2σy)},\displaystyle\left\{c_{1}\left(-\frac{1}{\sigma_{x}}+\frac{1}{1-\rho^{2}}\frac{\epsilon_{x}^{2}}{\sigma_{x}^{3}}-\frac{\rho}{1-\rho^{2}}\frac{\epsilon_{x}\epsilon_{y}}{\sigma_{x}^{2}\sigma_{y}}\right)\right\},
Λ~2\displaystyle\widetilde{\Lambda}_{2} =\displaystyle= {c2{22ρ21σy+11ρ2ϵy2σy3+ρ2(1ρ2)(2ρ2)ϵx2σx2σy2ρ(1ρ2)(2ρ2)ϵxϵyσxσy2}},\displaystyle\left\{c_{2}\left\{-\frac{2}{2-\rho^{2}}\frac{1}{\sigma_{y}}+\frac{1}{1-\rho^{2}}\frac{\epsilon_{y}^{2}}{\sigma_{y}^{3}}+\frac{\rho^{2}}{(1-\rho^{2})(2-\rho^{2})}\frac{\epsilon_{x}^{2}}{\sigma_{x}^{2}\sigma_{y}}-\frac{2\rho}{(1-\rho^{2})(2-\rho^{2})}\frac{\epsilon_{x}\epsilon_{y}}{\sigma_{x}\sigma_{y}^{2}}\right\}\right\},
Λ3\displaystyle\Lambda_{3} =\displaystyle= {11ρ2(ϵxσx2ρϵyσxσy)B1(𝐳)},\displaystyle\left\{\frac{1}{1-\rho^{2}}\left(\frac{\epsilon_{x}}{\sigma_{x}^{2}}-\rho\frac{\epsilon_{y}}{\sigma_{x}\sigma_{y}}\right)B_{1}({\bf z})\right\},
Λ~4\displaystyle\widetilde{\Lambda}_{4} =\displaystyle= {ϵyσy2B2(𝐳)},\displaystyle\left\{\frac{\epsilon_{y}}{\sigma_{y}^{2}}B_{2}({\bf z})\right\},
Λ5\displaystyle\Lambda_{5} =\displaystyle= {a(𝐳):E(a)=0}.\displaystyle\{a({\bf z}):E(a)=0\}.

By (S.1), we know that

Λ=Λ1Λ~2Λ3Λ~4Λ5.\displaystyle\Lambda^{\perp}=\Lambda_{1}^{\perp}\cap\widetilde{\Lambda}_{2}^{\perp}\cap\Lambda_{3}^{\perp}\cap\widetilde{\Lambda}_{4}^{\perp}\cap\Lambda_{5}^{\perp}.

Denote ϵ~x=ϵx/σx\widetilde{\epsilon}_{x}=\epsilon_{x}/\sigma_{x} and ϵ~y=ϵy/σy\widetilde{\epsilon}_{y}=\epsilon_{y}/\sigma_{y}. Then,

Λ1\displaystyle\Lambda_{1}^{\perp} =\displaystyle= {b(x,y,𝐳):E{(1σx+11ρ2ϵx2σx3ρ1ρ2ϵxϵyσx2σy)b(X,Y,𝐙)}=0}\displaystyle\left\{b(x,y,{\bf z}):E\left\{\left(-\frac{1}{\sigma_{x}}+\frac{1}{1-\rho^{2}}\frac{\epsilon_{x}^{2}}{\sigma_{x}^{3}}-\frac{\rho}{1-\rho^{2}}\frac{\epsilon_{x}\epsilon_{y}}{\sigma_{x}^{2}\sigma_{y}}\right)b(X,Y,{\bf Z})\right\}=0\right\}
=\displaystyle= {b(x,y,𝐳):E[{(1ρ2)+ϵ~x2ρϵ~xϵ~y}b(X,Y,𝐙)]=0},\displaystyle\left\{b(x,y,{\bf z}):E\left[\left\{-(1-\rho^{2})+\widetilde{\epsilon}_{x}^{2}-\rho\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}\right\}b(X,Y,{\bf Z})\right]=0\right\},

and

Λ~2\displaystyle\widetilde{\Lambda}_{2}^{\perp} =\displaystyle= {b(x,y,𝐳):E[{22ρ21σy+11ρ2ϵy2σy3+ρ2(1ρ2)(2ρ2)ϵx2σx2σy\displaystyle\left\{b(x,y,{\bf z}):E\left[\left\{-\frac{2}{2-\rho^{2}}\frac{1}{\sigma_{y}}+\frac{1}{1-\rho^{2}}\frac{\epsilon_{y}^{2}}{\sigma_{y}^{3}}+\frac{\rho^{2}}{(1-\rho^{2})(2-\rho^{2})}\frac{\epsilon_{x}^{2}}{\sigma_{x}^{2}\sigma_{y}}\right.\right.\right.
2ρ(1ρ2)(2ρ2)ϵxϵyσxσy2}b(X,Y,𝐙)]=0}\displaystyle\qquad\qquad\qquad\qquad\left.\left.\left.-\frac{2\rho}{(1-\rho^{2})(2-\rho^{2})}\frac{\epsilon_{x}\epsilon_{y}}{\sigma_{x}\sigma_{y}^{2}}\right\}b(X,Y,{\bf Z})\right]=0\right\}
=\displaystyle= {b(x,y,𝐳):E[{2(1ρ2)+(2ρ2)ϵ~y2+ρ2ϵ~x22ρϵ~xϵ~y}b(X,Y,𝐙)]=0}.\displaystyle\left\{b(x,y,{\bf z}):E\left[\left\{-2(1-\rho^{2})+(2-\rho^{2})\widetilde{\epsilon}_{y}^{2}+\rho^{2}\widetilde{\epsilon}_{x}^{2}-2\rho\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}\right\}b(X,Y,{\bf Z})\right]=0\right\}.

Also,

Λ3\displaystyle\Lambda_{3}^{\perp} =\displaystyle= {b(x,y,𝐳):E{11ρ2(ϵxσx2ρϵyσxσy)B1(𝐙)b(X,Y,𝐙)}=0,B1(𝐳)}\displaystyle\left\{b(x,y,{\bf z}):E\left\{\frac{1}{1-\rho^{2}}\left(\frac{\epsilon_{x}}{\sigma_{x}^{2}}-\rho\frac{\epsilon_{y}}{\sigma_{x}\sigma_{y}}\right)B_{1}({\bf Z})b(X,Y,{\bf Z})\right\}=0,\ \forall B_{1}({\bf z})\right\}
=\displaystyle= {b(x,y,𝐳):E{11ρ2(ϵxσx2ρϵyσxσy)b(X,Y,𝐙)|𝐙}=0}\displaystyle\left\{b(x,y,{\bf z}):E\left\{\frac{1}{1-\rho^{2}}\left(\frac{\epsilon_{x}}{\sigma_{x}^{2}}-\rho\frac{\epsilon_{y}}{\sigma_{x}\sigma_{y}}\right)b(X,Y,{\bf Z})\Big|{\bf Z}\right\}=0\right\}
=\displaystyle= {b(x,y,𝐳):E{(ϵ~xρϵ~y)b(X,Y,𝐙)|𝐙}=0}\displaystyle\left\{b(x,y,{\bf z}):E\left\{\left(\widetilde{\epsilon}_{x}-\rho\widetilde{\epsilon}_{y}\right)b(X,Y,{\bf Z})\Big|{\bf Z}\right\}=0\right\}

and

Λ~4\displaystyle\widetilde{\Lambda}_{4}^{\perp} =\displaystyle= {b(x,y,𝐳):E{ϵyσy2B2(Z)b(X,Y,𝐙)}=0,B2(𝐳)}\displaystyle\left\{b(x,y,{\bf z}):E\left\{\frac{\epsilon_{y}}{\sigma_{y}^{2}}B_{2}(Z)b(X,Y,{\bf Z})\right\}=0,\ \forall B_{2}({\bf z})\right\}
=\displaystyle= {b(x,y,𝐳):E{ϵ~yb(X,Y,𝐙)|𝐙}=0}.\displaystyle\left\{b(x,y,{\bf z}):E\left\{\widetilde{\epsilon}_{y}b(X,Y,{\bf Z})\Big|{\bf Z}\right\}=0\right\}.

Also obviously,

Λ5={b(x,y,𝐳):E{b(X,Y,𝐙)|𝐙}=0}.\displaystyle\Lambda_{5}^{\perp}=\left\{b(x,y,{\bf z}):E\left\{b(X,Y,{\bf Z})|{\bf Z}\right\}=0\right\}.

Therefore,

Λ\displaystyle\Lambda^{\perp} =\displaystyle= {b(x,y,𝐳):E[{(1ρ2)+ϵ~x2ρϵ~xϵ~y}b(X,Y,𝐙)]=0,\displaystyle\left\{b(x,y,{\bf z}):E\left[\left\{-(1-\rho^{2})+\widetilde{\epsilon}_{x}^{2}-\rho\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}\right\}b(X,Y,{\bf Z})\right]=0,\right.
E[{2(1ρ2)+(2ρ2)ϵ~y2+ρ2ϵ~x22ρϵ~xϵ~y}b(X,Y,𝐙)]=0,\displaystyle\left.E\left[\left\{-2(1-\rho^{2})+(2-\rho^{2})\widetilde{\epsilon}_{y}^{2}+\rho^{2}\widetilde{\epsilon}_{x}^{2}-2\rho\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}\right\}b(X,Y,{\bf Z})\right]=0,\right.
E{(ϵ~xρϵ~y)b(X,Y,𝐙)|Z}=0,E{ϵ~yb(X,Y,𝐙)|𝐙}=0,E{b(X,Y,𝐙)|𝐙}=0}\displaystyle\left.E\left\{\left(\widetilde{\epsilon}_{x}-\rho\widetilde{\epsilon}_{y}\right)b(X,Y,{\bf Z})\Big|Z\right\}=0,E\left\{\widetilde{\epsilon}_{y}b(X,Y,{\bf Z})\Big|{\bf Z}\right\}=0,E\left\{b(X,Y,{\bf Z})|{\bf Z}\right\}=0\right\}
=\displaystyle= {b(x,y,𝐳):E{(ϵ~x2ρϵ~xϵ~y)b(X,Y,𝐙)}=0,E{(ϵ~y2ρϵ~xϵ~y)b(X,Y,𝐙)}=0,\displaystyle\left\{b(x,y,{\bf z}):E\left\{\left(\widetilde{\epsilon}_{x}^{2}-\rho\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}\right)b(X,Y,{\bf Z})\right\}=0,E\left\{\left(\widetilde{\epsilon}_{y}^{2}-\rho\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}\right)b(X,Y,{\bf Z})\right\}=0,\right.
E{ϵ~xb(X,Y,𝐙)|𝐙}=0,E{ϵ~yb(X,Y,𝐙)|𝐙}=0,E{b(X,Y,𝐙)|𝐙}=0}.\displaystyle\left.E\left\{\widetilde{\epsilon}_{x}b(X,Y,{\bf Z})\Big|{\bf Z}\right\}=0,E\left\{\widetilde{\epsilon}_{y}b(X,Y,{\bf Z})\Big|{\bf Z}\right\}=0,E\left\{b(X,Y,{\bf Z})|{\bf Z}\right\}=0\right\}.

Proof of Proposition 3.

Note that

Sρ\displaystyle S_{\rho} =\displaystyle= 122ρ1ρ2+2ρ2(1ρ2)2(ϵx2σx22ρϵxϵyσxσy+ϵy2σy2)12(1ρ2)(2ϵxϵyσxσy)\displaystyle-\frac{1}{2}\frac{-2\rho}{1-\rho^{2}}+\frac{-2\rho}{2(1-\rho^{2})^{2}}\left(\frac{\epsilon_{x}^{2}}{\sigma_{x}^{2}}-2\rho\frac{\epsilon_{x}\epsilon_{y}}{\sigma_{x}\sigma_{y}}+\frac{\epsilon_{y}^{2}}{\sigma_{y}^{2}}\right)-\frac{1}{2(1-\rho^{2})}\left(-2\frac{\epsilon_{x}\epsilon_{y}}{\sigma_{x}\sigma_{y}}\right)
=\displaystyle= ρ1ρ2ρ(1ρ2)2(ϵ~x22ρϵ~xϵ~y+ϵ~y2)+11ρ2ϵ~xϵ~y.\displaystyle\frac{\rho}{1-\rho^{2}}-\frac{\rho}{(1-\rho^{2})^{2}}\left(\widetilde{\epsilon}_{x}^{2}-2\rho\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}+\widetilde{\epsilon}_{y}^{2}\right)+\frac{1}{1-\rho^{2}}\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}.

Thus,

E(Sρ|𝐙)\displaystyle E\left(S_{\rho}|{\bf Z}\right) =\displaystyle= E{ρ1ρ2ρ(1ρ2)2(ϵ~x22ρϵ~xϵ~y+ϵ~y2)+11ρ2ϵ~xϵ~y}\displaystyle E\left\{\frac{\rho}{1-\rho^{2}}-\frac{\rho}{(1-\rho^{2})^{2}}\left(\widetilde{\epsilon}_{x}^{2}-2\rho\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}+\widetilde{\epsilon}_{y}^{2}\right)+\frac{1}{1-\rho^{2}}\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}\right\}
=\displaystyle= ρ1ρ2ρ(1ρ2)2(12ρ2+1)+11ρ2ρ\displaystyle\frac{\rho}{1-\rho^{2}}-\frac{\rho}{(1-\rho^{2})^{2}}\left(1-2\rho^{2}+1\right)+\frac{1}{1-\rho^{2}}\rho
=\displaystyle= ρ1ρ22ρ1ρ2+11ρ2ρ\displaystyle\frac{\rho}{1-\rho^{2}}-\frac{2\rho}{1-\rho^{2}}+\frac{1}{1-\rho^{2}}\rho
=\displaystyle= 0.\displaystyle 0.

Also,

E(ϵ~xSρ|𝐙)=E{ρ1ρ2ϵ~xρ(1ρ2)2(ϵ~x32ρϵ~x2ϵ~y+ϵ~xϵ~y2)+11ρ2ϵ~x2ϵ~y}=0\displaystyle E\left(\widetilde{\epsilon}_{x}S_{\rho}|{\bf Z}\right)=E\left\{\frac{\rho}{1-\rho^{2}}\widetilde{\epsilon}_{x}-\frac{\rho}{(1-\rho^{2})^{2}}\left(\widetilde{\epsilon}_{x}^{3}-2\rho\widetilde{\epsilon}_{x}^{2}\widetilde{\epsilon}_{y}+\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}^{2}\right)+\frac{1}{1-\rho^{2}}\widetilde{\epsilon}_{x}^{2}\widetilde{\epsilon}_{y}\right\}=0

since it only uses the first and third moments of ϵx\epsilon_{x} and ϵy\epsilon_{y}. Similarly,

E(ϵ~ySρ|𝐙)=E{ρ1ρ2ϵ~yρ(1ρ2)2(ϵ~x2ϵ~y2ρϵ~xϵ~y2+ϵ~y3)+11ρ2ϵ~xϵ~y2}=0.\displaystyle E\left(\widetilde{\epsilon}_{y}S_{\rho}|{\bf Z}\right)=E\left\{\frac{\rho}{1-\rho^{2}}\widetilde{\epsilon}_{y}-\frac{\rho}{(1-\rho^{2})^{2}}\left(\widetilde{\epsilon}_{x}^{2}\widetilde{\epsilon}_{y}-2\rho\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}^{2}+\widetilde{\epsilon}_{y}^{3}\right)+\frac{1}{1-\rho^{2}}\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}^{2}\right\}=0.

Then,

E{(ϵ~x2ρϵ~xϵ~y)Sρ}\displaystyle E\left\{\left(\widetilde{\epsilon}_{x}^{2}-\rho\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}\right)S_{\rho}\right\}
=\displaystyle= E[(ϵ~x2ρϵ~xϵ~y){ρ1ρ2ρ(1ρ2)2(ϵ~x22ρϵ~xϵ~y+ϵ~y2)+11ρ2ϵ~xϵ~y}]\displaystyle E\left[\left(\widetilde{\epsilon}_{x}^{2}-\rho\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}\right)\left\{\frac{\rho}{1-\rho^{2}}-\frac{\rho}{(1-\rho^{2})^{2}}\left(\widetilde{\epsilon}_{x}^{2}-2\rho\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}+\widetilde{\epsilon}_{y}^{2}\right)+\frac{1}{1-\rho^{2}}\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}\right\}\right]
=\displaystyle= ρ1ρ2(1ρ2)ρ(1ρ2)2{36ρ2+1+2ρ23ρ2+2ρ2(1+2ρ2)3ρ2}\displaystyle\frac{\rho}{1-\rho^{2}}\left(1-\rho^{2}\right)-\frac{\rho}{(1-\rho^{2})^{2}}\left\{3-6\rho^{2}+1+2\rho^{2}-3\rho^{2}+2\rho^{2}(1+2\rho^{2})-3\rho^{2}\right\}
+11ρ2{3ρρ(1+2ρ2)}\displaystyle+\frac{1}{1-\rho^{2}}\left\{3\rho-\rho(1+2\rho^{2})\right\}
=\displaystyle= ρρ(1ρ2)2(48ρ2+4ρ4)+2ρ\displaystyle\rho-\frac{\rho}{(1-\rho^{2})^{2}}\left(4-8\rho^{2}+4\rho^{4}\right)+2\rho
=\displaystyle= ρ,\displaystyle-\rho,

and by symmetry,

E{(ϵ~y2ρϵ~xϵ~y)Sρ}=ρ.\displaystyle E\left\{\left(\widetilde{\epsilon}_{y}^{2}-\rho\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}\right)S_{\rho}\right\}=-\rho.

Let

S~ρ=Sρ+ρϵ~x22ρϵ~xϵ~y+ϵ~y22(1ρ2)2(1ρ2)2\displaystyle\widetilde{S}_{\rho}=S_{\rho}+\rho\frac{\widetilde{\epsilon}_{x}^{2}-2\rho\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}+\widetilde{\epsilon}_{y}^{2}-2(1-\rho^{2})}{2(1-\rho^{2})^{2}}

Note that

E{ϵ~x22ρϵ~xϵ~y+ϵ~y22(1ρ2)2(1ρ2)2|𝐙}=12ρ2+12(1ρ2)2(1ρ2)2=0,\displaystyle E\left\{\frac{\widetilde{\epsilon}_{x}^{2}-2\rho\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}+\widetilde{\epsilon}_{y}^{2}-2(1-\rho^{2})}{2(1-\rho^{2})^{2}}\Big|{\bf Z}\right\}=\frac{1-2\rho^{2}+1-2(1-\rho^{2})}{2(1-\rho^{2})^{2}}=0,

and

E{ϵ~xϵ~x22ρϵ~xϵ~y+ϵ~y22(1ρ2)2(1ρ2)2|𝐙}=E{ϵ~yϵ~x22ρϵ~xϵ~y+ϵ~y22(1ρ2)2(1ρ2)2|𝐙}=0\displaystyle E\left\{\widetilde{\epsilon}_{x}\frac{\widetilde{\epsilon}_{x}^{2}-2\rho\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}+\widetilde{\epsilon}_{y}^{2}-2(1-\rho^{2})}{2(1-\rho^{2})^{2}}\Big|{\bf Z}\right\}=E\left\{\widetilde{\epsilon}_{y}\frac{\widetilde{\epsilon}_{x}^{2}-2\rho\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}+\widetilde{\epsilon}_{y}^{2}-2(1-\rho^{2})}{2(1-\rho^{2})^{2}}\Big|{\bf Z}\right\}=0

since they both only use the first and third moments of a multivariate normal distribution. Thus, we have

E(S~ρ|𝐙)=E(ϵ~xS~ρ|𝐙)=E(ϵ~yS~ρ|𝐙)=0.\displaystyle E(\widetilde{S}_{\rho}|{\bf Z})=E(\widetilde{\epsilon}_{x}\widetilde{S}_{\rho}|{\bf Z})=E(\widetilde{\epsilon}_{y}\widetilde{S}_{\rho}|{\bf Z})=0.

Furthermore,

E[(ϵ~x2ρϵ~xϵ~y){ϵ~x22ρϵ~xϵ~y+ϵ~y22(1ρ2)2(1ρ2)2}]\displaystyle E\left[\left(\widetilde{\epsilon}_{x}^{2}-\rho\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}\right)\left\{\frac{\widetilde{\epsilon}_{x}^{2}-2\rho\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}+\widetilde{\epsilon}_{y}^{2}-2(1-\rho^{2})}{2(1-\rho^{2})^{2}}\right\}\right]
=\displaystyle= E[12(1ρ2)2{36ρ2+1+2ρ23ρ2+2ρ2(1+2ρ2)3ρ22(1ρ2)2}]\displaystyle E\left[\frac{1}{2(1-\rho^{2})^{2}}\left\{3-6\rho^{2}+1+2\rho^{2}-3\rho^{2}+2\rho^{2}(1+2\rho^{2})-3\rho^{2}-2(1-\rho^{2})^{2}\right\}\right]
=\displaystyle= E[12(1ρ2)2{48ρ2+4ρ42(1ρ2)2}]\displaystyle E\left[\frac{1}{2(1-\rho^{2})^{2}}\left\{4-8\rho^{2}+4\rho^{4}-2(1-\rho^{2})^{2}\right\}\right]
=\displaystyle= E[12(1ρ2)2{4(1ρ2)22(1ρ2)2}]\displaystyle E\left[\frac{1}{2(1-\rho^{2})^{2}}\left\{4(1-\rho^{2})^{2}-2(1-\rho^{2})^{2}\right\}\right]
=\displaystyle= 1.\displaystyle 1.

Thus, we have

E{(ϵ~x2ρϵ~xϵ~y)S~ρ}=ρ+ρ=0.\displaystyle E\left\{\left(\widetilde{\epsilon}_{x}^{2}-\rho\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}\right)\widetilde{S}_{\rho}\right\}=-\rho+\rho=0.

By symmetry,

E{(ϵ~x2ρϵ~xϵ~y)S~ρ}=ρ+ρ=0.\displaystyle E\left\{\left(\widetilde{\epsilon}_{x}^{2}-\rho\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}\right)\widetilde{S}_{\rho}\right\}=-\rho+\rho=0.

Therefore, S~ρΛ\widetilde{S}_{\rho}\in\Lambda^{\perp}. Also, notice that

E{ϵ~x22ρϵ~xϵ~y+ϵ~y22(1ρ2)2(1ρ2)2}=12ρ2+12(1ρ2)2(1ρ2)2=0,\displaystyle E\left\{\frac{\widetilde{\epsilon}_{x}^{2}-2\rho\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}+\widetilde{\epsilon}_{y}^{2}-2(1-\rho^{2})}{2(1-\rho^{2})^{2}}\right\}=\frac{1-2\rho^{2}+1-2(1-\rho^{2})}{2(1-\rho^{2})^{2}}=0,

so

ϵ~x22ρϵ~xϵ~y+ϵ~y22(1ρ2)2(1ρ2)2Λ5Λ.\displaystyle\frac{\widetilde{\epsilon}_{x}^{2}-2\rho\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}+\widetilde{\epsilon}_{y}^{2}-2(1-\rho^{2})}{2(1-\rho^{2})^{2}}\in\Lambda_{5}\subset\Lambda.

Therefore, S~ρ=Π(Sρ|Λ)\widetilde{S}_{\rho}=\Pi(S_{\rho}|\Lambda^{\perp}). Thus,

Seff=S~ρ\displaystyle S_{\rm eff}=\widetilde{S}_{\rho} =\displaystyle= ρ1ρ2ρ(1ρ2)2(ϵ~x22ρϵ~xϵ~y+ϵ~y2)+11ρ2ϵ~xϵ~y\displaystyle\frac{\rho}{1-\rho^{2}}-\frac{\rho}{(1-\rho^{2})^{2}}\left(\widetilde{\epsilon}_{x}^{2}-2\rho\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}+\widetilde{\epsilon}_{y}^{2}\right)+\frac{1}{1-\rho^{2}}\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}
+ρϵ~x22ρϵ~xϵ~y+ϵ~y22(1ρ2)2(1ρ2)2\displaystyle+\rho\frac{\widetilde{\epsilon}_{x}^{2}-2\rho\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}+\widetilde{\epsilon}_{y}^{2}-2(1-\rho^{2})}{2(1-\rho^{2})^{2}}
=\displaystyle= ρ2(1ρ2)2(ϵ~x22ρϵ~xϵ~y+ϵ~y2)+11ρ2ϵ~xϵ~y\displaystyle-\frac{\rho}{2(1-\rho^{2})^{2}}\left(\widetilde{\epsilon}_{x}^{2}-2\rho\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}+\widetilde{\epsilon}_{y}^{2}\right)+\frac{1}{1-\rho^{2}}\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}
=\displaystyle= 12(1ρ2)2(ρϵ~x22ϵ~xϵ~y+ρϵ~y2).\displaystyle-\frac{1}{2(1-\rho^{2})^{2}}\left(\rho\widetilde{\epsilon}_{x}^{2}-2\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}+\rho\widetilde{\epsilon}_{y}^{2}\right).

Based on the form of SeffS_{\rm eff}, we have

E(Seff2)\displaystyle E(S_{\rm eff}^{2}) =\displaystyle= 14(1ρ2)4E{(ρϵ~x22ϵ~xϵ~y+ρϵ~y2)2}\displaystyle\frac{1}{4(1-\rho^{2})^{4}}E\left\{\left(\rho\widetilde{\epsilon}_{x}^{2}-2\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}+\rho\widetilde{\epsilon}_{y}^{2}\right)^{2}\right\}
=\displaystyle= 14(1ρ2)4{3ρ2+2ρ2(1+2ρ2)+3ρ212ρ2+2ρ2(1+2ρ2)12ρ2}\displaystyle\frac{1}{4(1-\rho^{2})^{4}}\left\{3\rho^{2}+2\rho^{2}(1+2\rho^{2})+3\rho^{2}-12\rho^{2}+2\rho^{2}(1+2\rho^{2})-12\rho^{2}\right\}
=\displaystyle= 14(1ρ2)4{48ρ2+4ρ4}\displaystyle\frac{1}{4(1-\rho^{2})^{4}}\left\{4-8\rho^{2}+4\rho^{4}\right\}
=\displaystyle= 14(1ρ2)4{4(1ρ2)2}\displaystyle\frac{1}{4(1-\rho^{2})^{4}}\left\{4(1-\rho^{2})^{2}\right\}
=\displaystyle= 1(1ρ2)2.\displaystyle\frac{1}{(1-\rho^{2})^{2}}.

Thus, the semiparametric efficiency bound is

E(Seff2)1=(1ρ2)2.\displaystyle E(S_{\rm eff}^{2})^{-1}=(1-\rho^{2})^{2}.

The efficient influence function is

ϕeff(x,y,𝐳)=[E(Seff2)]1Seff=12(ρϵ~x22ϵ~xϵ~y+ρϵ~y2).\displaystyle\phi_{\rm eff}(x,y,{\bf z})=[E(S_{\rm eff}^{2})]^{-1}S_{\rm eff}=-\frac{1}{2}\left(\rho\widetilde{\epsilon}_{x}^{2}-2\widetilde{\epsilon}_{x}\widetilde{\epsilon}_{y}+\rho\widetilde{\epsilon}_{y}^{2}\right).

Proof of Theorem 1.

By Taylor’s mean value theorem, we have

n21/2(ρ^2ρ)\displaystyle n_{2}^{1/2}(\widehat{\rho}_{2}-\rho) =\displaystyle= n21/21σxσy(σ^xy2σxy)n21/2σxy2σx3σy(σ^x22σx2)\displaystyle n_{2}^{1/2}\frac{1}{\sigma_{x}\sigma_{y}}(\widehat{\sigma}_{xy2}-\sigma_{xy})-n_{2}^{1/2}\frac{\sigma_{xy}}{2\sigma_{x}^{3}\sigma_{y}}(\widehat{\sigma}_{x2}^{2}-\sigma_{x}^{2}) (S.2)
n21/2σxy2σxσy3(σ^y22σy2)+R,\displaystyle-n_{2}^{1/2}\frac{\sigma_{xy}}{2\sigma_{x}\sigma_{y}^{3}}(\widehat{\sigma}_{y2}^{2}-\sigma_{y}^{2})+R,

where

R\displaystyle R =\displaystyle= n21/212σx3σy(σ^xy2σxy)(σ^x22σx2)n21/212σxσy3(σ^xy2σxy)(σ^y22σy2)\displaystyle-n_{2}^{1/2}\frac{1}{2\sigma_{x*}^{3}\sigma_{y*}}(\widehat{\sigma}_{xy2}-\sigma_{xy})(\widehat{\sigma}_{x2}^{2}-\sigma_{x}^{2})-n_{2}^{1/2}\frac{1}{2\sigma_{x*}\sigma_{y*}^{3}}(\widehat{\sigma}_{xy2}-\sigma_{xy})(\widehat{\sigma}_{y2}^{2}-\sigma_{y}^{2}) (S.3)
+n21/2σxy4σx3σy3(σ^x22σx2)(σ^y22σy2)\displaystyle+n_{2}^{1/2}\frac{\sigma_{xy*}}{4\sigma_{x*}^{3}\sigma_{y*}^{3}}(\widehat{\sigma}_{x2}^{2}-\sigma_{x}^{2})(\widehat{\sigma}_{y2}^{2}-\sigma_{y}^{2})
n21/23σxy8σx5σy(σ^x22σx2)2n21/23σxy8σxσy5(σ^y22σy2)2,\displaystyle-n_{2}^{1/2}\frac{3\sigma_{xy*}}{8\sigma_{x*}^{5}\sigma_{y*}}(\widehat{\sigma}_{x2}^{2}-\sigma_{x}^{2})^{2}-n_{2}^{1/2}\frac{3\sigma_{xy*}}{8\sigma_{x*}\sigma_{y*}^{5}}(\widehat{\sigma}_{y2}^{2}-\sigma_{y}^{2})^{2},

for some σx2\sigma_{x*}^{2} between σx2\sigma_{x}^{2} and σ^x22\widehat{\sigma}_{x2}^{2}, σy2\sigma_{y*}^{2} between σy2\sigma_{y}^{2} and σ^y22\widehat{\sigma}_{y2}^{2}, and σxy\sigma_{xy*} between σxy\sigma_{xy} and σ^xy2\widehat{\sigma}_{xy2}.

We decompose σ^x22\widehat{\sigma}_{x2}^{2} into three parts as follows:

σ^x22σx2\displaystyle\widehat{\sigma}_{x2}^{2}-\sigma_{x}^{2} =\displaystyle= n21i=n1+1n{Xim^x1(𝐙i)}2σx2\displaystyle n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\{X_{i}-\widehat{m}_{x1}({\bf Z}_{i})\}^{2}-\sigma_{x}^{2} (S.4)
=\displaystyle= n21i=n1+1n{Ximx(𝐙i)}2+n21i=n1+1n{mx(𝐙i)m^x1(𝐙i)}2\displaystyle n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\{X_{i}-m_{x}({\bf Z}_{i})\}^{2}+n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\{m_{x}({\bf Z}_{i})-\widehat{m}_{x1}({\bf Z}_{i})\}^{2}
+2n21i=n1+1n{mx(𝐙i)m^x1(𝐙i)}{Ximx(𝐙i)}σx2\displaystyle+2n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\{m_{x}({\bf Z}_{i})-\widehat{m}_{x1}({\bf Z}_{i})\}\{X_{i}-m_{x}({\bf Z}_{i})\}-\sigma_{x}^{2}
=\displaystyle= n21i=n1+1nϵxi2+n21i=n1+1n{mx(𝐙i)m^x1(𝐙i)}2\displaystyle n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\epsilon_{xi}^{2}+n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\{m_{x}({\bf Z}_{i})-\widehat{m}_{x1}({\bf Z}_{i})\}^{2}
+2n21i=n1+1n{mx(𝐙i)m^x1(𝐙i)}ϵxiσx2.\displaystyle+2n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\{m_{x}({\bf Z}_{i})-\widehat{m}_{x1}({\bf Z}_{i})\}\epsilon_{xi}-\sigma_{x}^{2}.

Under m^x1mx2=op(n11/4)\|\widehat{m}_{x1}-m_{x}\|_{2}=o_{p}(n_{1}^{-1/4}), we have

E[n21i=n1+1n{mx(𝐙i)m^x1(𝐙i)}2|m^x1]\displaystyle E\left[n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\{m_{x}({\bf Z}_{i})-\widehat{m}_{x1}({\bf Z}_{i})\}^{2}|\widehat{m}_{x1}\right] =\displaystyle= E[{mx(𝐙)m^x1(𝐙)}2|m^x1]\displaystyle E\left[\{m_{x}({\bf Z})-\widehat{m}_{x1}({\bf Z})\}^{2}|\widehat{m}_{x1}\right]
=\displaystyle= m^x1mx22\displaystyle\|\widehat{m}_{x1}-m_{x}\|_{2}^{2}
=\displaystyle= op(n11/2),\displaystyle o_{p}(n_{1}^{-1/2}),

and since the sum is nonnegative, by Markov’s inequality, we have

n21i=n1+1n{mx(𝐙i)m^x1(𝐙i)}2=op(n11/2).\displaystyle n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\{m_{x}({\bf Z}_{i})-\widehat{m}_{x1}({\bf Z}_{i})\}^{2}=o_{p}(n_{1}^{-1/2}).

Also, note that

n21i=n1+1nϵxi2=σx2+op(1).\displaystyle n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\epsilon_{xi}^{2}=\sigma_{x}^{2}+o_{p}(1).

Furthermore,

E[{mx(𝐙)m^x1(𝐙)}ϵx|m^x1]=E[{mx(𝐙)m^x1(𝐙)}|m^x1]E(ϵx)=0,\displaystyle E\left[\{m_{x}({\bf Z})-\widehat{m}_{x1}({\bf Z})\}\epsilon_{x}|\widehat{m}_{x1}\right]=E\left[\{m_{x}({\bf Z})-\widehat{m}_{x1}({\bf Z})\}|\widehat{m}_{x1}\right]E(\epsilon_{x})=0,

and under m^x1mx2=op(n11/4)\|\widehat{m}_{x1}-m_{x}\|_{2}=o_{p}(n_{1}^{-1/4}),

var[n21i=n1+1n{mx(𝐙i)m^x1(𝐙i)}ϵxi|m^x1]\displaystyle\mbox{var}\left[n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\{m_{x}({\bf Z}_{i})-\widehat{m}_{x1}({\bf Z}_{i})\}\epsilon_{xi}|\widehat{m}_{x1}\right]
=\displaystyle= n21var[{mx(𝐙)m^x1(𝐙)}ϵx|m^x1]\displaystyle n_{2}^{-1}\mbox{var}\left[\{m_{x}({\bf Z})-\widehat{m}_{x1}({\bf Z})\}\epsilon_{x}|\widehat{m}_{x1}\right]
=\displaystyle= n21E[{mx(𝐙)m^x1(𝐙)}2ϵx2|m^x1]\displaystyle n_{2}^{-1}E\left[\{m_{x}({\bf Z})-\widehat{m}_{x1}({\bf Z})\}^{2}\epsilon_{x}^{2}|\widehat{m}_{x1}\right]
=\displaystyle= n21E[{mx(𝐙)m^x1(𝐙)}2|m^x1]E(ϵx2)\displaystyle n_{2}^{-1}E\left[\{m_{x}({\bf Z})-\widehat{m}_{x1}({\bf Z})\}^{2}|\widehat{m}_{x1}\right]E(\epsilon_{x}^{2})
=\displaystyle= n21m^x1mx22σx2\displaystyle n_{2}^{-1}\|\widehat{m}_{x1}-m_{x}\|_{2}^{2}\sigma_{x}^{2}
=\displaystyle= op(n21n11/2),\displaystyle o_{p}(n_{2}^{-1}n_{1}^{-1/2}),

so by Chebyshev’s inequality, we have

n21i=n1+1n{mx(𝐙i)m^x1(𝐙i)}ϵxi=op(n21/2n11/4).\displaystyle n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\{m_{x}({\bf Z}_{i})-\widehat{m}_{x1}({\bf Z}_{i})\}\epsilon_{xi}=o_{p}(n_{2}^{-1/2}n_{1}^{-1/4}).

Plugging back to (S.4), we have

σ^x22σx2=n21i=n1+1nϵxi2σx2+op(n11/2+n21/2n11/4).\displaystyle\widehat{\sigma}_{x2}^{2}-\sigma_{x}^{2}=n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\epsilon_{xi}^{2}-\sigma_{x}^{2}+o_{p}(n_{1}^{-1/2}+n_{2}^{-1/2}n_{1}^{-1/4}). (S.5)

Same arguments lead to, under m^y1my2=op(n11/4)\|\widehat{m}_{y1}-m_{y}\|_{2}=o_{p}(n_{1}^{-1/4}),

σ^y22σy2=n21i=n1+1nϵyi2σy2+op(n11/2+n21/2n11/4).\displaystyle\widehat{\sigma}_{y2}^{2}-\sigma_{y}^{2}=n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\epsilon_{yi}^{2}-\sigma_{y}^{2}+o_{p}(n_{1}^{-1/2}+n_{2}^{-1/2}n_{1}^{-1/4}). (S.6)

We also decompose σ^xy\widehat{\sigma}_{xy} into three parts as follows:

σ^xy2σxy\displaystyle\widehat{\sigma}_{xy2}-\sigma_{xy} =\displaystyle= n21i=n1+1n{Xim^x1(𝐙i)}{Yim^y1(𝐙i)}σxy\displaystyle n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\{X_{i}-\widehat{m}_{x1}({\bf Z}_{i})\}\{Y_{i}-\widehat{m}_{y1}({\bf Z}_{i})\}-\sigma_{xy} (S.7)
=\displaystyle= n21i=n1+1n{Ximx(𝐙i)}{Yimy(𝐙i)}\displaystyle n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\{X_{i}-m_{x}({\bf Z}_{i})\}\{Y_{i}-m_{y}({\bf Z}_{i})\}
+n21i=n1+1n{mx(𝐙i)m^x1(𝐙i)}{my(𝐙i)m^y1(𝐙i)}\displaystyle+n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\{m_{x}({\bf Z}_{i})-\widehat{m}_{x1}({\bf Z}_{i})\}\{m_{y}({\bf Z}_{i})-\widehat{m}_{y1}({\bf Z}_{i})\}
+n21i=n1+1n{mx(𝐙i)m^x1(𝐙i)}{Yimy(𝐙i)}\displaystyle+n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\{m_{x}({\bf Z}_{i})-\widehat{m}_{x1}({\bf Z}_{i})\}\{Y_{i}-m_{y}({\bf Z}_{i})\}
+n21i=n1+1n{my(𝐙i)m^y1(𝐙i)}{Ximx(𝐙i)}σxy\displaystyle+n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\{m_{y}({\bf Z}_{i})-\widehat{m}_{y1}({\bf Z}_{i})\}\{X_{i}-m_{x}({\bf Z}_{i})\}-\sigma_{xy}
=\displaystyle= n21i=n1+1nϵxiϵyi+n21i=n1+1n{mx(𝐙i)m^x1(𝐙i)}{my(𝐙i)m^y1(𝐙i)}\displaystyle n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\epsilon_{xi}\epsilon_{yi}+n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\{m_{x}({\bf Z}_{i})-\widehat{m}_{x1}({\bf Z}_{i})\}\{m_{y}({\bf Z}_{i})-\widehat{m}_{y1}({\bf Z}_{i})\}
+n21i=n1+1n{mx(𝐙i)m^x1(𝐙i)}ϵyi+n21i=n1+1n{my(𝐙i)m^y1(𝐙i)}ϵxi\displaystyle+n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\{m_{x}({\bf Z}_{i})-\widehat{m}_{x1}({\bf Z}_{i})\}\epsilon_{yi}+n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\{m_{y}({\bf Z}_{i})-\widehat{m}_{y1}({\bf Z}_{i})\}\epsilon_{xi}
σxy.\displaystyle-\sigma_{xy}.

Under m^x1mx2=op(n11/4)\|\widehat{m}_{x1}-m_{x}\|_{2}=o_{p}(n_{1}^{-1/4}) and m^y1my2=op(n11/4)\|\widehat{m}_{y1}-m_{y}\|_{2}=o_{p}(n_{1}^{-1/4}), we have

E[|n21i=n1+1n{mx(𝐙i)m^x1(𝐙i)}{my(𝐙i)m^y1(𝐙i)}||m^x1,m^y1]\displaystyle E\left[\left|n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\{m_{x}({\bf Z}_{i})-\widehat{m}_{x1}({\bf Z}_{i})\}\{m_{y}({\bf Z}_{i})-\widehat{m}_{y1}({\bf Z}_{i})\}\right||\widehat{m}_{x1},\widehat{m}_{y1}\right]
\displaystyle\leq E[|mx(𝐙)m^x1(𝐙)||my(𝐙)m^y1(𝐙)||m^x1,m^y1]\displaystyle E\left[\left|m_{x}({\bf Z})-\widehat{m}_{x1}({\bf Z})\right|\left|m_{y}({\bf Z})-\widehat{m}_{y1}({\bf Z})\right||\widehat{m}_{x1},\widehat{m}_{y1}\right]
=\displaystyle= |m^x1mx|,|m^y1my|2\displaystyle\left\langle\left|\widehat{m}_{x1}-m_{x}\right|,\left|\widehat{m}_{y1}-m_{y}\right|\right\rangle_{2}
\displaystyle\leq m^x1mx2m^y1my2\displaystyle\|\widehat{m}_{x1}-m_{x}\|_{2}\|\widehat{m}_{y1}-m_{y}\|_{2}
=\displaystyle= op(n11/4)op(n11/4)\displaystyle o_{p}(n_{1}^{-1/4})o_{p}(n_{1}^{-1/4})
=\displaystyle= op(n11/2).\displaystyle o_{p}(n_{1}^{-1/2}).

By Markov’s inequality, we have

n21i=n1+1n{mx(𝐙i)m^x1(𝐙i)}{my(𝐙i)m^y1(𝐙i)}=op(n11/2).\displaystyle n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\{m_{x}({\bf Z}_{i})-\widehat{m}_{x1}({\bf Z}_{i})\}\{m_{y}({\bf Z}_{i})-\widehat{m}_{y1}({\bf Z}_{i})\}=o_{p}(n_{1}^{-1/2}).

Furthermore,

E[{mx(𝐙)m^x1(𝐙)}ϵy|m^x1]=E[{mx(𝐙)m^x1(𝐙)}|m^x1]E(ϵy)=0,\displaystyle E\left[\{m_{x}({\bf Z})-\widehat{m}_{x1}({\bf Z})\}\epsilon_{y}|\widehat{m}_{x1}\right]=E\left[\{m_{x}({\bf Z})-\widehat{m}_{x1}({\bf Z})\}|\widehat{m}_{x1}\right]E(\epsilon_{y})=0,

and under m^x1mx2=op(n11/4)\|\widehat{m}_{x1}-m_{x}\|_{2}=o_{p}(n_{1}^{-1/4}),

var[n21i=n1+1n{mx(𝐙i)m^x1(𝐙i)}ϵyi|m^x1]\displaystyle\mbox{var}\left[n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\{m_{x}({\bf Z}_{i})-\widehat{m}_{x1}({\bf Z}_{i})\}\epsilon_{yi}|\widehat{m}_{x1}\right]
=\displaystyle= n21var[{mx(𝐙)m^x1(𝐙)}ϵy|m^x1]\displaystyle n_{2}^{-1}\mbox{var}\left[\{m_{x}({\bf Z})-\widehat{m}_{x1}({\bf Z})\}\epsilon_{y}|\widehat{m}_{x1}\right]
=\displaystyle= n21E[{mx(𝐙)m^x1(𝐙)}2ϵy2|m^x1]\displaystyle n_{2}^{-1}E\left[\{m_{x}({\bf Z})-\widehat{m}_{x1}({\bf Z})\}^{2}\epsilon_{y}^{2}|\widehat{m}_{x1}\right]
=\displaystyle= n21E[{mx(𝐙)m^x1(𝐙)}2|m^x1]E(ϵy2)\displaystyle n_{2}^{-1}E\left[\{m_{x}({\bf Z})-\widehat{m}_{x1}({\bf Z})\}^{2}|\widehat{m}_{x1}\right]E(\epsilon_{y}^{2})
=\displaystyle= n21m^x1mx22σy2\displaystyle n_{2}^{-1}\|\widehat{m}_{x1}-m_{x}\|_{2}^{2}\sigma_{y}^{2}
=\displaystyle= op(n21n11/2),\displaystyle o_{p}(n_{2}^{-1}n_{1}^{-1/2}),

so by Chebyshev’s inequality, we have

n21i=n1+1n{mx(𝐙i)m^x1(𝐙i)}ϵyi=op(n21/2n11/4).\displaystyle n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\{m_{x}({\bf Z}_{i})-\widehat{m}_{x1}({\bf Z}_{i})\}\epsilon_{yi}=o_{p}(n_{2}^{-1/2}n_{1}^{-1/4}).

Same arguments lead to, under m^y1my2=op(n11/4)\|\widehat{m}_{y1}-m_{y}\|_{2}=o_{p}(n_{1}^{-1/4}),

n21i=n1+1n{my(𝐙i)m^y1(𝐙i)}ϵxi=op(n21/2n11/4).\displaystyle n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\{m_{y}({\bf Z}_{i})-\widehat{m}_{y1}({\bf Z}_{i})\}\epsilon_{xi}=o_{p}(n_{2}^{-1/2}n_{1}^{-1/4}).

Plugging back to (S.7), we have

σ^xy2σxy=n21i=n1+1nϵxiϵyiσxy+op(n11/2+n21/2n11/4).\displaystyle\widehat{\sigma}_{xy2}-\sigma_{xy}=n_{2}^{-1}\sum_{i=n_{1}+1}^{n}\epsilon_{xi}\epsilon_{yi}-\sigma_{xy}+o_{p}(n_{1}^{-1/2}+n_{2}^{-1/2}n_{1}^{-1/4}). (S.8)

Applying central limit theorem and Slutsky’s theorem to (S.5), (S.6) and (S.8), if n1n2nn_{1}\asymp n_{2}\asymp n, we have

σ^x22σx2=Op(n1/2),σ^y22σy2=Op(n1/2),σ^xy2σxy=Op(n1/2),\displaystyle\widehat{\sigma}_{x2}^{2}-\sigma_{x}^{2}=O_{p}(n^{-1/2}),\quad\widehat{\sigma}_{y2}^{2}-\sigma_{y}^{2}=O_{p}(n^{-1/2}),\quad\widehat{\sigma}_{xy2}-\sigma_{xy}=O_{p}(n^{-1/2}),

and thus,

σ^x2σx2=op(1),σ^y2σy2=op(1),σ^xyσxy=op(1).\displaystyle\widehat{\sigma}_{x*}^{2}-\sigma_{x}^{2}=o_{p}(1),\quad\widehat{\sigma}_{y*}^{2}-\sigma_{y}^{2}=o_{p}(1),\quad\widehat{\sigma}_{xy*}-\sigma_{xy}=o_{p}(1).

Plugging back to (S.3), when n1n2nn_{1}\asymp n_{2}\asymp n, we have

R\displaystyle R =\displaystyle= n21/2{12σx3σy+op(1)}Op(n1/2)Op(n1/2)\displaystyle-n_{2}^{1/2}\left\{\frac{1}{2\sigma_{x}^{3}\sigma_{y}}+o_{p}(1)\right\}O_{p}(n^{-1/2})O_{p}(n^{-1/2})
n21/2{12σxσy3+op(1)}Op(n1/2)Op(n1/2)\displaystyle-n_{2}^{1/2}\left\{\frac{1}{2\sigma_{x}\sigma_{y}^{3}}+o_{p}(1)\right\}O_{p}(n^{-1/2})O_{p}(n^{-1/2})
+n21/2{σxy4σx3σy3+op(1)}Op(n1/2)Op(n1/2)\displaystyle+n_{2}^{1/2}\left\{\frac{\sigma_{xy}}{4\sigma_{x}^{3}\sigma_{y}^{3}}+o_{p}(1)\right\}O_{p}(n^{-1/2})O_{p}(n^{-1/2})
n21/2{3σxy8σx5σy+op(1)}Op(n1/2)2n21/2{3σxy8σxσy5+op(1)}Op(n1/2)2\displaystyle-n_{2}^{1/2}\left\{\frac{3\sigma_{xy}}{8\sigma_{x}^{5}\sigma_{y}}+o_{p}(1)\right\}O_{p}(n^{-1/2})^{2}-n_{2}^{1/2}\left\{\frac{3\sigma_{xy}}{8\sigma_{x}\sigma_{y}^{5}}+o_{p}(1)\right\}O_{p}(n^{-1/2})^{2}
=\displaystyle= Op(n1/2).\displaystyle O_{p}(n^{-1/2}).

Also, when n1n2nn_{1}\asymp n_{2}\asymp n, the remainder terms in (S.5), (S.6) and (S.8) all become op(n1/2)o_{p}(n^{-1/2}). Therefore, plugging back into (S.2), we have

n21/2(ρ^2ρ)\displaystyle n_{2}^{1/2}(\widehat{\rho}_{2}-\rho)
=\displaystyle= 1σxσyn21/2i=n1+1n(ϵxiϵyiσxy)σxy2σx3σyn21/2i=n1+1n(ϵxi2σx2)\displaystyle\frac{1}{\sigma_{x}\sigma_{y}}n_{2}^{-1/2}\sum_{i=n_{1}+1}^{n}(\epsilon_{xi}\epsilon_{yi}-\sigma_{xy})-\frac{\sigma_{xy}}{2\sigma_{x}^{3}\sigma_{y}}n_{2}^{-1/2}\sum_{i=n_{1}+1}^{n}(\epsilon_{xi}^{2}-\sigma_{x}^{2})
σxy2σxσy3n21/2i=n1+1n(ϵyi2σy2)+Op(n1/2)\displaystyle-\frac{\sigma_{xy}}{2\sigma_{x}\sigma_{y}^{3}}n_{2}^{-1/2}\sum_{i=n_{1}+1}^{n}(\epsilon_{yi}^{2}-\sigma_{y}^{2})+O_{p}(n^{-1/2})
=\displaystyle= n21/2i=n1+1n(ϵxiϵyiσxσyσxyσxσyσxyϵxi22σx3σy+σxy2σxσyσxyϵyi22σxσy3+σxy2σxσy)+Op(n1/2)\displaystyle n_{2}^{-1/2}\sum_{i=n_{1}+1}^{n}\left(\frac{\epsilon_{xi}\epsilon_{yi}}{\sigma_{x}\sigma_{y}}-\frac{\sigma_{xy}}{\sigma_{x}\sigma_{y}}-\frac{\sigma_{xy}\epsilon_{xi}^{2}}{2\sigma_{x}^{3}\sigma_{y}}+\frac{\sigma_{xy}}{2\sigma_{x}\sigma_{y}}-\frac{\sigma_{xy}\epsilon_{yi}^{2}}{2\sigma_{x}\sigma_{y}^{3}}+\frac{\sigma_{xy}}{2\sigma_{x}\sigma_{y}}\right)+O_{p}(n^{-1/2})
=\displaystyle= n21/2i=n1+1n(ϵ~xiϵ~yiρ2ϵ~xi2ρ2ϵ~yi2)+Op(n1/2)\displaystyle n_{2}^{-1/2}\sum_{i=n_{1}+1}^{n}\left(\widetilde{\epsilon}_{xi}\widetilde{\epsilon}_{yi}-\frac{\rho}{2}\widetilde{\epsilon}_{xi}^{2}-\frac{\rho}{2}\widetilde{\epsilon}_{yi}^{2}\right)+O_{p}(n^{-1/2})
=\displaystyle= n21/2i=n1+1n12(ρϵ~xi22ϵ~xiϵ~yi+ρϵ~yi2)+Op(n1/2).\displaystyle n_{2}^{-1/2}\sum_{i=n_{1}+1}^{n}-\frac{1}{2}\left(\rho\widetilde{\epsilon}_{xi}^{2}-2\widetilde{\epsilon}_{xi}\widetilde{\epsilon}_{yi}+\rho\widetilde{\epsilon}_{yi}^{2}\right)+O_{p}(n^{-1/2}).

Comparing with (11), we have

n21/2(ρ^2ρ)=n21/2i=n1+1nϕeff(Xi,Yi,𝐙i)+Op(n1/2).\displaystyle n_{2}^{1/2}(\widehat{\rho}_{2}-\rho)=n_{2}^{-1/2}\sum_{i=n_{1}+1}^{n}\phi_{\rm eff}(X_{i},Y_{i},{\bf Z}_{i})+O_{p}(n^{-1/2}). (S.9)

Similarly, under m^x2mx2=op(n21/4)\|\widehat{m}_{x2}-m_{x}\|_{2}=o_{p}(n_{2}^{-1/4}) and m^y2my2=op(n21/4)\|\widehat{m}_{y2}-m_{y}\|_{2}=o_{p}(n_{2}^{-1/4}) with n1n2nn_{1}\asymp n_{2}\asymp n, we also have

n11/2(ρ^1ρ)=n11/2i=1n1ϕeff(Xi,Yi,𝐙i)+Op(n1/2).\displaystyle n_{1}^{1/2}(\widehat{\rho}_{1}-\rho)=n_{1}^{-1/2}\sum_{i=1}^{n_{1}}\phi_{\rm eff}(X_{i},Y_{i},{\bf Z}_{i})+O_{p}(n^{-1/2}). (S.10)

Then, a direct application of (S.9) and (S.10) gives the asymptotic expansion for ρ^\widehat{\rho} as

n1/2(ρ^ρ)=n1/2i=1nϕeff(Xi,Yi,𝐙i)+Op(n1/2).\displaystyle n^{1/2}(\widehat{\rho}-\rho)=n^{-1/2}\sum_{i=1}^{n}\phi_{\rm eff}(X_{i},Y_{i},{\bf Z}_{i})+O_{p}(n^{-1/2}).

S.2 Additional Simulation Results

nn RPCO RPCS RPCF PaCo RHSIC RRIT RCIT RCoT
100 0.036 0.074 0.062 0.072 0.052 0.044 1.000 1.000
200 0.032 0.054 0.038 0.050 0.048 0.040 0.300 0.222
500 0.068 0.068 0.072 0.072 0.052 0.044 0.094 0.096
1000 0.058 0.068 0.058 0.056 0.034 0.040 0.058 0.060
2000 0.046 0.046 0.042 0.044 0.050 0.076 0.074 0.050
5000 0.042 0.050 0.040 0.042 0.058 0.046 0.054 0.056
Table S.1: Empirical levels of eight tests under Model 2 based on 500 experiments.
Figure S.1: Boxplots of p-values of eight tests for Model 2 under the null hypothesis, with sample sizes n=100,200,500,1000,2000,5000n=100,200,500,1000,2000,5000. The red line represents 0.05.
ρ\rho nn RPCO RPCS RPCF PaCo RHSIC RRIT RCIT RCoT
-0.25 100 0.682 0.588 0.644 0.670 0.310 0.456 1.000 1.000
-0.25 200 0.962 0.930 0.950 0.952 0.622 0.778 0.714 0.750
-0.25 500 1.000 1.000 1.000 1.000 0.970 0.986 0.946 0.978
-0.25 1000 1.000 1.000 1.000 1.000 1.000 1.000 0.982 0.998
-0.25 2000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 0.998
-0.25 5000 1.000 1.000 1.000 1.000 1.000 1.000 0.998 1.000
-0.50 100 1.000 0.996 1.000 1.000 0.948 0.970 1.000 1.000
-0.50 200 1.000 1.000 1.000 1.000 1.000 1.000 0.972 0.998
-0.50 500 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
-0.50 1000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
-0.50 2000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
-0.50 5000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
-0.75 100 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
-0.75 200 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
-0.75 500 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
-0.75 1000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
-0.75 2000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
-0.75 5000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
-1.00 100 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
-1.00 200 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
-1.00 500 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
-1.00 1000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
-1.00 2000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
-1.00 5000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
-0.025 100 0.070 0.086 0.078 0.078 0.056 0.060 1.000 1.000
-0.025 200 0.056 0.064 0.048 0.054 0.044 0.052 0.186 0.204
-0.025 500 0.108 0.118 0.122 0.120 0.054 0.072 0.136 0.118
-0.025 1000 0.132 0.136 0.136 0.138 0.076 0.080 0.112 0.130
-0.025 2000 0.160 0.164 0.162 0.164 0.100 0.114 0.118 0.130
-0.025 5000 0.434 0.426 0.434 0.430 0.140 0.284 0.244 0.264
-0.050 100 0.056 0.066 0.056 0.070 0.060 0.044 1.000 1.000
-0.050 200 0.098 0.104 0.106 0.108 0.076 0.072 0.196 0.254
-0.050 500 0.196 0.216 0.206 0.204 0.094 0.160 0.196 0.188
-0.050 1000 0.364 0.350 0.370 0.372 0.168 0.244 0.220 0.264
-0.050 2000 0.606 0.598 0.610 0.598 0.276 0.418 0.362 0.422
-0.050 5000 0.956 0.952 0.954 0.950 0.608 0.818 0.714 0.780
-0.075 100 0.160 0.160 0.140 0.152 0.076 0.076 1.000 1.000
-0.075 200 0.192 0.210 0.188 0.200 0.086 0.116 0.294 0.274
-0.075 500 0.360 0.336 0.356 0.362 0.138 0.240 0.240 0.272
-0.075 1000 0.652 0.632 0.642 0.640 0.278 0.438 0.360 0.434
-0.075 2000 0.910 0.902 0.916 0.916 0.574 0.740 0.672 0.726
-0.075 5000 1.000 1.000 1.000 1.000 0.944 0.976 0.926 0.968
-0.100 100 0.144 0.164 0.140 0.160 0.086 0.102 1.000 1.000
-0.100 200 0.312 0.306 0.288 0.296 0.122 0.190 0.336 0.330
-0.100 500 0.624 0.620 0.624 0.624 0.236 0.416 0.416 0.426
-0.100 1000 0.904 0.882 0.896 0.900 0.502 0.718 0.656 0.706
-0.100 2000 0.994 0.996 0.992 0.992 0.820 0.962 0.888 0.910
-0.100 5000 1.000 1.000 1.000 1.000 0.996 0.992 0.986 0.998
Table S.2: Empirical powers of eight tests under Model 1 based on 500 experiments, where the alternative distributions include (1) ρ=0.25,0.5,0.75,1\rho=-0.25,-0.5,-0.75,-1 and (2) ρ=0.025,0.05,0.075,0.1\rho=-0.025,-0.05,-0.075,-0.1.
Figure S.2: Boxplots of p-values of eight tests for Model 1 under the alternative hypothesis, with sample sizes n=100,200,500,1000,2000,5000n=100,200,500,1000,2000,5000, where the alternative distributions include ρ=0.25,0.5,0.75,1\rho=0.25,0.5,0.75,1. The red line represents 0.05.
Figure S.3: Boxplots of p-values of eight tests for Model 1 under the alternative hypothesis, with sample sizes n=100,200,500,1000,2000,5000n=100,200,500,1000,2000,5000, where the alternative distributions include ρ=0.025,0.05,0.075,0.1\rho=0.025,0.05,0.075,0.1. The red line represents 0.05.
Figure S.4: Boxplots of p-values of eight tests for Model 1 under the alternative hypothesis, with sample sizes n=100,200,500,1000,2000,5000n=100,200,500,1000,2000,5000, where the alternative distributions include ρ=0.25,0.5,0.75,1\rho=-0.25,-0.5,-0.75,-1. The red line represents 0.05.
Figure S.5: Boxplots of p-values of eight tests for Model 1 under the alternative hypothesis, with sample sizes n=100,200,500,1000,2000,5000n=100,200,500,1000,2000,5000, where the alternative distributions include ρ=0.025,0.05,0.075,0.1\rho=-0.025,-0.05,-0.075,-0.1. The red line represents 0.05.
ρ\rho nn RPCO RPCS RPCF PaCo RHSIC RRIT RCIT RCoT
-0.25 100 0.722 0.556 0.630 0.708 0.282 0.444 1.000 1.000
-0.25 200 0.922 0.860 0.902 0.916 0.576 0.742 0.716 0.776
-0.25 500 1.000 1.000 1.000 1.000 0.960 0.980 0.886 0.980
-0.25 1000 1.000 1.000 1.000 1.000 1.000 1.000 0.976 1.000
-0.25 2000 1.000 1.000 1.000 1.000 1.000 1.000 0.990 1.000
-0.25 5000 1.000 1.000 1.000 1.000 1.000 0.998 0.998 1.000
0.25 100 0.738 0.690 0.726 0.720 0.368 0.484 1.000 1.000
0.25 200 0.934 0.906 0.940 0.936 0.606 0.784 0.704 0.778
0.25 500 1.000 1.000 1.000 1.000 0.970 0.984 0.924 0.994
0.25 1000 1.000 1.000 1.000 1.000 1.000 1.000 0.972 0.998
0.25 2000 1.000 1.000 1.000 1.000 1.000 1.000 0.986 1.000
0.25 5000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
-0.50 100 1.000 0.994 1.000 1.000 0.946 0.954 1.000 1.000
-0.50 200 1.000 1.000 1.000 1.000 1.000 1.000 0.974 1.000
-0.50 500 1.000 1.000 1.000 1.000 1.000 1.000 0.992 1.000
-0.50 1000 1.000 1.000 1.000 1.000 1.000 1.000 0.998 1.000
-0.50 2000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
-0.50 5000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
0.50 100 1.000 0.994 1.000 1.000 0.966 0.972 1.000 1.000
0.50 200 1.000 1.000 1.000 1.000 1.000 1.000 0.970 1.000
0.50 500 1.000 1.000 1.000 1.000 1.000 1.000 0.998 1.000
0.50 1000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
0.50 2000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
0.50 5000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
-0.75 100 1.000 1.000 1.000 1.000 1.000 0.998 1.000 1.000
-0.75 200 1.000 1.000 1.000 1.000 1.000 1.000 0.992 1.000
-0.75 500 1.000 1.000 1.000 1.000 1.000 1.000 0.996 1.000
-0.75 1000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
-0.75 2000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
-0.75 5000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
0.75 100 1.000 1.000 1.000 1.000 1.000 0.998 1.000 1.000
0.75 200 1.000 1.000 1.000 1.000 1.000 1.000 0.990 1.000
0.75 500 1.000 1.000 1.000 1.000 1.000 1.000 0.998 1.000
0.75 1000 1.000 1.000 1.000 1.000 1.000 1.000 0.998 1.000
0.75 2000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
0.75 5000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
-1.00 100 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
-1.00 200 1.000 1.000 1.000 1.000 1.000 1.000 0.998 1.000
-1.00 500 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
-1.00 1000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
-1.00 2000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
-1.00 5000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
1.00 100 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
1.00 200 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
1.00 500 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
1.00 1000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
1.00 2000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
1.00 5000 1.000 1.000 1.000 1.000 1.000 1.000 1.000 1.000
Table S.3: Empirical powers of eight tests under Model 2 based on 500 experiments, where the alternative distributions include ρ=±0.25,±0.5,±0.75,±1\rho=\pm 0.25,\pm 0.5,\pm 0.75,\pm 1.
ρ\rho nn RPCO RPCS RPCF PaCo RHSIC RRIT RCIT RCoT
-0.025 100 0.056 0.064 0.048 0.062 0.048 0.052 1.000 1.000
-0.025 200 0.048 0.056 0.044 0.058 0.064 0.060 0.290 0.246
-0.025 500 0.088 0.082 0.080 0.088 0.052 0.078 0.106 0.118
-0.025 1000 0.126 0.116 0.124 0.126 0.056 0.082 0.112 0.106
-0.025 2000 0.186 0.178 0.186 0.198 0.090 0.124 0.126 0.166
-0.025 5000 0.396 0.406 0.402 0.400 0.180 0.296 0.228 0.262
0.025 100 0.050 0.058 0.056 0.058 0.072 0.054 1.000 1.000
0.025 200 0.060 0.082 0.058 0.058 0.056 0.038 0.300 0.254
0.025 500 0.090 0.094 0.094 0.096 0.062 0.058 0.124 0.108
0.025 1000 0.102 0.118 0.098 0.100 0.068 0.094 0.110 0.110
0.025 2000 0.196 0.212 0.194 0.198 0.088 0.126 0.110 0.148
0.025 5000 0.406 0.408 0.400 0.402 0.148 0.282 0.184 0.248
-0.050 100 0.090 0.086 0.088 0.112 0.058 0.066 1.000 1.000
-0.050 200 0.112 0.098 0.086 0.110 0.082 0.076 0.302 0.242
-0.050 500 0.186 0.184 0.182 0.194 0.092 0.116 0.172 0.176
-0.050 1000 0.332 0.314 0.336 0.344 0.128 0.208 0.222 0.238
-0.050 2000 0.592 0.562 0.580 0.588 0.232 0.402 0.266 0.374
-0.050 5000 0.944 0.946 0.942 0.946 0.618 0.816 0.606 0.790
0.050 100 0.076 0.096 0.094 0.102 0.060 0.072 1.000 1.000
0.050 200 0.112 0.144 0.130 0.134 0.074 0.092 0.344 0.268
0.050 500 0.220 0.238 0.238 0.230 0.114 0.144 0.170 0.182
0.050 1000 0.370 0.400 0.384 0.384 0.162 0.252 0.216 0.268
0.050 2000 0.636 0.644 0.638 0.634 0.274 0.472 0.312 0.450
0.050 5000 0.972 0.974 0.968 0.970 0.600 0.810 0.644 0.794
-0.075 100 0.124 0.104 0.090 0.122 0.064 0.074 1.000 1.000
-0.075 200 0.166 0.128 0.142 0.176 0.078 0.106 0.352 0.268
-0.075 500 0.398 0.338 0.364 0.386 0.158 0.280 0.248 0.326
-0.075 1000 0.668 0.626 0.642 0.664 0.298 0.446 0.366 0.490
-0.075 2000 0.942 0.926 0.940 0.942 0.528 0.744 0.590 0.730
-0.075 5000 1.000 1.000 1.000 1.000 0.950 0.980 0.906 0.972
0.075 100 0.108 0.140 0.126 0.124 0.086 0.100 1.000 1.000
0.075 200 0.190 0.194 0.204 0.186 0.100 0.106 0.370 0.308
0.075 500 0.392 0.392 0.404 0.392 0.160 0.256 0.260 0.304
0.075 1000 0.636 0.634 0.640 0.630 0.304 0.448 0.338 0.446
0.075 2000 0.926 0.920 0.924 0.918 0.528 0.752 0.606 0.758
0.075 5000 0.998 0.998 0.998 0.998 0.924 0.962 0.876 0.972
-0.100 100 0.178 0.122 0.144 0.190 0.078 0.076 1.000 1.000
-0.100 200 0.280 0.212 0.252 0.282 0.106 0.170 0.396 0.370
-0.100 500 0.614 0.566 0.578 0.612 0.216 0.412 0.356 0.434
-0.100 1000 0.886 0.852 0.880 0.888 0.506 0.700 0.508 0.668
-0.100 2000 0.998 0.994 0.998 0.998 0.830 0.924 0.820 0.924
-0.100 5000 1.000 1.000 1.000 1.000 1.000 1.000 0.950 0.998
0.100 100 0.166 0.190 0.182 0.178 0.084 0.132 1.000 1.000
0.100 200 0.314 0.318 0.312 0.306 0.156 0.204 0.398 0.386
0.100 500 0.608 0.610 0.630 0.618 0.242 0.430 0.324 0.448
0.100 1000 0.900 0.894 0.894 0.890 0.486 0.736 0.508 0.694
0.100 2000 0.992 0.994 0.994 0.992 0.810 0.932 0.780 0.912
0.100 5000 1.000 1.000 1.000 1.000 1.000 0.998 0.946 1.000
Table S.4: Empirical powers of eight tests under Model 2 based on 500 experiments, where the alternative distributions include ρ=±0.025,±0.05,±0.075,±0.1\rho=\pm 0.025,\pm 0.05,\pm 0.075,\pm 0.1.
Figure S.6: Boxplots of p-values of eight tests for Model 2 under the alternative hypothesis, with sample sizes n=100,200,500,1000,2000,5000n=100,200,500,1000,2000,5000, where the alternative distributions include ρ=0.25,0.5,0.75,1\rho=0.25,0.5,0.75,1. The red line represents 0.05.
Figure S.7: Boxplots of p-values of eight tests for Model 2 under the alternative hypothesis, with sample sizes n=100,200,500,1000,2000,5000n=100,200,500,1000,2000,5000, where the alternative distributions include ρ=0.025,0.05,0.075,0.1\rho=0.025,0.05,0.075,0.1. The red line represents 0.05.
Figure S.8: Boxplots of p-values of eight tests for Model 2 under the alternative hypothesis, with sample sizes n=100,200,500,1000,2000,5000n=100,200,500,1000,2000,5000, where the alternative distributions include ρ=0.25,0.5,0.75,1\rho=-0.25,-0.5,-0.75,-1. The red line represents 0.05.
Figure S.9: Boxplots of p-values of eight tests for Model 2 under the alternative hypothesis, with sample sizes n=100,200,500,1000,2000,5000n=100,200,500,1000,2000,5000, where the alternative distributions include ρ=0.025,0.05,0.075,0.1\rho=-0.025,-0.05,-0.075,-0.1. The red line represents 0.05.
RPCS RPCF
ρ\rho nn Bias SD SD^\widehat{\rm SD} RMSE 95% cvg Bias SD SD^\widehat{\rm SD} RMSE 95% cvg
-0.25 100 0.028 0.099 0.094 0.103 0.940 0.016 0.092 0.094 0.093 0.956
-0.25 200 0.008 0.070 0.066 0.070 0.930 0.002 0.065 0.066 0.065 0.944
-0.25 500 0.001 0.047 0.042 0.047 0.916 -0.003 0.044 0.042 0.044 0.930
-0.25 1000 0.004 0.030 0.030 0.031 0.942 0.002 0.030 0.030 0.030 0.958
-0.25 2000 0.001 0.021 0.021 0.021 0.942 0.001 0.021 0.021 0.021 0.942
-0.25 5000 0.001 0.013 0.013 0.013 0.946 0.001 0.013 0.013 0.013 0.954
-0.50 100 0.049 0.089 0.079 0.101 0.884 0.024 0.075 0.077 0.079 0.954
-0.50 200 0.026 0.059 0.055 0.064 0.918 0.009 0.053 0.053 0.054 0.952
-0.50 500 0.010 0.038 0.034 0.039 0.932 0.004 0.032 0.034 0.032 0.968
-0.50 1000 0.006 0.028 0.024 0.028 0.928 0.003 0.025 0.024 0.025 0.956
-0.50 2000 0.003 0.017 0.017 0.017 0.944 0.002 0.016 0.017 0.016 0.954
-0.50 5000 0.002 0.011 0.011 0.011 0.944 0.001 0.011 0.011 0.011 0.940
-0.75 100 0.062 0.067 0.052 0.091 0.824 0.027 0.046 0.048 0.053 0.964
-0.75 200 0.032 0.044 0.034 0.054 0.870 0.012 0.031 0.032 0.033 0.960
-0.75 500 0.013 0.028 0.020 0.031 0.894 0.005 0.021 0.020 0.021 0.938
-0.75 1000 0.007 0.021 0.014 0.022 0.920 0.002 0.014 0.014 0.014 0.944
-0.75 2000 0.003 0.011 0.010 0.012 0.936 0.002 0.010 0.010 0.010 0.940
-0.75 5000 0.003 0.006 0.006 0.007 0.938 0.002 0.006 0.006 0.006 0.952
RPCO PaCo
ρ\rho nn Bias SD SD^\widehat{\rm SD} RMSE 95% cvg Bias SD SD^\widehat{\rm SD} RMSE 95% cvg
-0.25 100 0.010 0.092 0.093 0.092 0.956 0.010 0.094 0.093 0.095 0.954
-0.25 200 -0.002 0.064 0.066 0.064 0.954 -0.001 0.065 0.066 0.065 0.942
-0.25 500 -0.004 0.044 0.042 0.044 0.938 -0.003 0.044 0.042 0.044 0.930
-0.25 1000 0.001 0.030 0.030 0.030 0.948 0.002 0.030 0.030 0.030 0.952
-0.25 2000 0.000 0.021 0.021 0.021 0.946 0.000 0.021 0.021 0.021 0.942
-0.25 5000 0.000 0.013 0.013 0.013 0.952 0.001 0.013 0.013 0.013 0.952
-0.50 100 0.006 0.075 0.075 0.075 0.934 0.007 0.076 0.075 0.076 0.950
-0.50 200 0.002 0.053 0.053 0.053 0.948 0.004 0.053 0.053 0.053 0.948
-0.50 500 0.001 0.032 0.034 0.032 0.966 0.002 0.032 0.034 0.032 0.964
-0.50 1000 0.001 0.025 0.024 0.025 0.954 0.002 0.025 0.024 0.025 0.952
-0.50 2000 0.000 0.016 0.017 0.016 0.954 0.002 0.016 0.017 0.016 0.952
-0.50 5000 0.000 0.011 0.011 0.011 0.942 0.001 0.011 0.011 0.011 0.942
-0.75 100 0.002 0.042 0.044 0.042 0.954 0.003 0.044 0.044 0.044 0.948
-0.75 200 0.002 0.031 0.031 0.031 0.942 0.004 0.031 0.031 0.031 0.950
-0.75 500 0.001 0.020 0.020 0.020 0.938 0.003 0.021 0.020 0.021 0.932
-0.75 1000 -0.001 0.014 0.014 0.014 0.938 0.002 0.014 0.014 0.014 0.948
-0.75 2000 -0.001 0.009 0.010 0.009 0.950 0.002 0.010 0.010 0.010 0.950
-0.75 5000 0.000 0.006 0.006 0.006 0.966 0.002 0.006 0.006 0.006 0.954
Table S.5: Results based on 500 estimates of ρ\rho under Model 1, with ρ=0.25,0.5,0.75\rho=-0.25,-0.5,-0.75.
RPCS RPCF
ρ\rho nn Bias SD SD^\widehat{\rm SD} RMSE 95% cvg Bias SD SD^\widehat{\rm SD} RMSE 95% cvg
0.00 100 0.018 0.111 0.099 0.112 0.912 0.016 0.105 0.099 0.106 0.924
0.00 200 0.006 0.072 0.070 0.072 0.934 0.004 0.069 0.070 0.069 0.954
0.00 500 0.004 0.048 0.045 0.048 0.926 0.002 0.048 0.045 0.048 0.928
0.00 1000 0.003 0.032 0.032 0.032 0.930 0.002 0.031 0.032 0.031 0.942
0.00 2000 0.002 0.023 0.022 0.023 0.954 0.001 0.022 0.022 0.022 0.958
0.00 5000 0.001 0.014 0.014 0.014 0.950 0.001 0.014 0.014 0.014 0.960
0.25 100 -0.007 0.104 0.093 0.104 0.916 0.003 0.096 0.093 0.096 0.934
0.25 200 -0.009 0.074 0.066 0.074 0.918 -0.003 0.069 0.066 0.069 0.936
0.25 500 0.000 0.045 0.042 0.045 0.930 0.003 0.043 0.042 0.044 0.944
0.25 1000 -0.005 0.032 0.030 0.032 0.920 -0.003 0.029 0.030 0.030 0.942
0.25 2000 -0.003 0.021 0.021 0.021 0.944 -0.002 0.020 0.021 0.020 0.948
0.25 5000 -0.002 0.014 0.013 0.014 0.950 -0.001 0.013 0.013 0.013 0.946
0.50 100 -0.027 0.086 0.077 0.090 0.918 -0.011 0.076 0.075 0.076 0.954
0.50 200 -0.021 0.062 0.054 0.065 0.920 -0.007 0.053 0.053 0.053 0.950
0.50 500 -0.008 0.039 0.034 0.040 0.892 -0.002 0.035 0.034 0.035 0.936
0.50 1000 -0.005 0.030 0.024 0.030 0.912 0.000 0.024 0.024 0.024 0.942
0.50 2000 -0.003 0.022 0.017 0.022 0.910 -0.001 0.017 0.017 0.017 0.938
0.50 5000 -0.002 0.013 0.011 0.014 0.924 0.000 0.011 0.011 0.011 0.948
0.75 100 -0.049 0.070 0.050 0.085 0.842 -0.019 0.049 0.046 0.053 0.946
0.75 200 -0.029 0.045 0.034 0.054 0.888 -0.010 0.030 0.032 0.032 0.962
0.75 500 -0.019 0.037 0.021 0.041 0.884 -0.006 0.019 0.020 0.020 0.962
0.75 1000 -0.010 0.027 0.014 0.028 0.882 -0.003 0.014 0.014 0.015 0.948
0.75 2000 -0.005 0.016 0.010 0.017 0.928 -0.002 0.010 0.010 0.010 0.942
0.75 5000 -0.003 0.012 0.006 0.013 0.918 -0.001 0.006 0.006 0.006 0.952
RPCO PaCo
ρ\rho nn Bias SD SD^\widehat{\rm SD} RMSE 95% cvg Bias SD SD^\widehat{\rm SD} RMSE 95% cvg
0.00 100 0.005 0.105 0.099 0.105 0.948 0.004 0.112 0.099 0.112 0.910
0.00 200 -0.002 0.068 0.070 0.068 0.962 -0.003 0.071 0.070 0.071 0.950
0.00 500 0.000 0.047 0.045 0.047 0.932 0.000 0.048 0.045 0.048 0.924
0.00 1000 0.001 0.031 0.032 0.031 0.942 0.001 0.031 0.032 0.031 0.942
0.00 2000 0.001 0.022 0.022 0.022 0.954 0.001 0.022 0.022 0.022 0.956
0.00 5000 0.001 0.014 0.014 0.014 0.956 0.001 0.014 0.014 0.014 0.958
0.25 100 0.003 0.096 0.093 0.096 0.942 0.003 0.100 0.093 0.100 0.922
0.25 200 -0.003 0.068 0.066 0.068 0.932 -0.004 0.070 0.066 0.070 0.926
0.25 500 0.003 0.043 0.042 0.043 0.948 0.003 0.044 0.042 0.044 0.940
0.25 1000 -0.002 0.029 0.030 0.029 0.946 -0.003 0.029 0.030 0.029 0.940
0.25 2000 -0.001 0.020 0.021 0.020 0.956 -0.002 0.020 0.021 0.020 0.950
0.25 5000 -0.001 0.013 0.013 0.013 0.952 -0.001 0.013 0.013 0.013 0.946
0.50 100 0.001 0.074 0.074 0.074 0.952 -0.002 0.080 0.075 0.080 0.938
0.50 200 0.000 0.053 0.053 0.053 0.948 -0.002 0.054 0.053 0.054 0.952
0.50 500 0.001 0.034 0.033 0.034 0.938 0.000 0.035 0.034 0.035 0.930
0.50 1000 0.002 0.024 0.024 0.024 0.934 0.001 0.025 0.024 0.025 0.936
0.50 2000 0.001 0.017 0.017 0.017 0.932 0.000 0.017 0.017 0.017 0.936
0.50 5000 0.001 0.010 0.011 0.010 0.952 0.000 0.011 0.011 0.011 0.946
0.75 100 0.001 0.046 0.043 0.046 0.932 0.001 0.048 0.043 0.048 0.912
0.75 200 0.001 0.030 0.031 0.030 0.942 -0.001 0.031 0.031 0.031 0.950
0.75 500 -0.001 0.019 0.020 0.019 0.960 -0.002 0.019 0.020 0.019 0.958
0.75 1000 0.000 0.014 0.014 0.014 0.944 -0.002 0.014 0.014 0.015 0.946
0.75 2000 0.000 0.010 0.010 0.010 0.944 -0.002 0.010 0.010 0.010 0.950
0.75 5000 0.000 0.006 0.006 0.006 0.952 -0.001 0.006 0.006 0.006 0.954
Table S.6: Results based on 500 estimates of ρ\rho under Model 2, with ρ=0,0.25,0.5,0.75\rho=0,0.25,0.5,0.75.
RPCS RPCF
ρ\rho nn Bias SD SD^\widehat{\rm SD} RMSE 95% cvg Bias SD SD^\widehat{\rm SD} RMSE 95% cvg
-0.25 100 0.037 0.100 0.094 0.107 0.902 0.024 0.095 0.094 0.098 0.942
-0.25 200 0.028 0.074 0.067 0.080 0.904 0.015 0.072 0.066 0.073 0.920
-0.25 500 0.015 0.042 0.042 0.044 0.946 0.009 0.040 0.042 0.041 0.968
-0.25 1000 0.006 0.032 0.030 0.033 0.928 0.002 0.030 0.030 0.030 0.950
-0.25 2000 0.002 0.020 0.021 0.021 0.966 0.000 0.020 0.021 0.020 0.960
-0.25 5000 0.001 0.013 0.013 0.013 0.954 0.000 0.012 0.013 0.012 0.958
-0.50 100 0.061 0.084 0.080 0.104 0.894 0.036 0.075 0.078 0.083 0.952
-0.50 200 0.040 0.062 0.055 0.073 0.908 0.019 0.054 0.054 0.057 0.952
-0.50 500 0.021 0.043 0.034 0.048 0.888 0.008 0.035 0.034 0.036 0.924
-0.50 1000 0.013 0.031 0.024 0.034 0.904 0.005 0.024 0.024 0.025 0.948
-0.50 2000 0.005 0.019 0.017 0.019 0.942 0.002 0.017 0.017 0.017 0.952
-0.50 5000 0.003 0.011 0.011 0.011 0.926 0.002 0.011 0.011 0.011 0.940
-0.75 100 0.075 0.067 0.054 0.100 0.782 0.043 0.051 0.050 0.067 0.916
-0.75 200 0.049 0.047 0.036 0.068 0.760 0.023 0.034 0.033 0.041 0.932
-0.75 500 0.026 0.038 0.021 0.046 0.780 0.010 0.020 0.020 0.022 0.952
-0.75 1000 0.013 0.025 0.014 0.029 0.860 0.004 0.014 0.014 0.015 0.946
-0.75 2000 0.006 0.018 0.010 0.019 0.902 0.003 0.010 0.010 0.011 0.930
-0.75 5000 0.004 0.010 0.006 0.010 0.908 0.002 0.006 0.006 0.007 0.938
RPCO PaCo
ρ\rho nn Bias SD SD^\widehat{\rm SD} RMSE 95% cvg Bias SD SD^\widehat{\rm SD} RMSE 95% cvg
-0.25 100 0.002 0.094 0.093 0.094 0.930 0.003 0.097 0.093 0.097 0.928
-0.25 200 0.004 0.070 0.066 0.071 0.918 0.005 0.073 0.066 0.073 0.908
-0.25 500 0.004 0.040 0.042 0.040 0.962 0.005 0.041 0.042 0.041 0.958
-0.25 1000 0.000 0.030 0.030 0.030 0.948 0.000 0.030 0.030 0.030 0.944
-0.25 2000 -0.001 0.020 0.021 0.020 0.960 0.000 0.020 0.021 0.020 0.964
-0.25 5000 -0.001 0.012 0.013 0.012 0.956 0.000 0.012 0.013 0.012 0.958
-0.50 100 0.002 0.073 0.075 0.073 0.944 0.005 0.077 0.075 0.077 0.946
-0.50 200 0.002 0.055 0.053 0.055 0.948 0.003 0.056 0.053 0.056 0.946
-0.50 500 0.002 0.035 0.034 0.035 0.938 0.002 0.035 0.034 0.035 0.932
-0.50 1000 0.002 0.024 0.024 0.024 0.952 0.003 0.024 0.024 0.024 0.950
-0.50 2000 0.000 0.017 0.017 0.017 0.956 0.001 0.017 0.017 0.017 0.956
-0.50 5000 0.000 0.011 0.011 0.011 0.952 0.001 0.011 0.011 0.011 0.942
-0.75 100 -0.001 0.044 0.043 0.044 0.940 0.001 0.048 0.044 0.047 0.926
-0.75 200 0.001 0.033 0.031 0.033 0.924 0.003 0.034 0.031 0.034 0.930
-0.75 500 0.001 0.019 0.020 0.019 0.960 0.002 0.020 0.020 0.020 0.956
-0.75 1000 0.000 0.014 0.014 0.014 0.952 0.001 0.014 0.014 0.014 0.944
-0.75 2000 0.000 0.010 0.010 0.010 0.952 0.001 0.010 0.010 0.010 0.942
-0.75 5000 0.000 0.006 0.006 0.006 0.960 0.001 0.006 0.006 0.006 0.948
Table S.7: Results based on 500 estimates of ρ\rho under Model 2, with ρ=0.25,0.5,0.75\rho=-0.25,-0.5,-0.75.
RPCS RPCF
ρ\rho nn Bias SD SD^\widehat{\rm SD} RMSE 95% cvg Bias SD SD^\widehat{\rm SD} RMSE 95% cvg
0 100 0.033 0.117 0.099 0.122 0.874 0.032 0.103 0.099 0.108 0.930
0 200 0.021 0.080 0.070 0.083 0.906 0.023 0.071 0.070 0.075 0.926
0 500 0.015 0.048 0.045 0.051 0.938 0.013 0.045 0.045 0.047 0.944
0 1000 0.013 0.038 0.032 0.040 0.886 0.010 0.034 0.032 0.035 0.918
0 2000 0.008 0.026 0.022 0.027 0.892 0.007 0.024 0.022 0.025 0.914
0 5000 0.003 0.016 0.014 0.016 0.894 0.002 0.015 0.014 0.015 0.938
RPCO PaCo
ρ\rho nn Bias SD SD^\widehat{\rm SD} RMSE 95% cvg Bias SD SD^\widehat{\rm SD} RMSE 95% cvg
0 100 -0.003 0.102 0.099 0.102 0.944 0.144 0.104 0.097 0.178 0.650
0 200 0.002 0.070 0.070 0.070 0.958 0.135 0.068 0.069 0.151 0.536
0 500 -0.001 0.043 0.045 0.042 0.956 0.142 0.043 0.044 0.148 0.096
0 1000 0.002 0.032 0.032 0.032 0.950 0.144 0.031 0.031 0.147 0.000
0 2000 0.000 0.022 0.022 0.022 0.940 0.144 0.022 0.022 0.146 0.000
0 5000 0.000 0.014 0.014 0.014 0.956 0.144 0.013 0.014 0.144 0.000
Table S.8: Results based on 500 estimates of ρ\rho under Model 3, with ρ=0\rho=0.