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. Author manuscript; available in PMC: 2012 Jul 31.
Published in final edited form as: Stat Med. 2011 May 9;30(16):1933–1951. doi: 10.1002/sim.4264

A proportional hazards regression model for the subdistribution with right-censored and left-truncated competing risks data

Xu Zhang a,*,, Mei-Jie Zhang b, Jason Fine c
PMCID: PMC3408877  NIHMSID: NIHMS377743  PMID: 21557288

Abstract

With competing risks failure time data, one often needs to assess the covariate effects on the cumulative incidence probabilities. Fine and Gray proposed a proportional hazards regression model to directly model the subdistribution of a competing risk. They developed the estimating procedure for right-censored competing risks data, based on the inverse probability of censoring weighting. Right-censored and left-truncated competing risks data sometimes occur in biomedical researches. In this paper, we study the proportional hazards regression model for the subdistribution of a competing risk with right-censored and left-truncated data. We adopt a new weighting technique to estimate the parameters in this model. We have derived the large sample properties of the proposed estimators. To illustrate the application of the new method, we analyze the failure time data for children with acute leukemia. In this example, the failure times for children who had bone marrow transplants were left truncated.

Keywords: competing risks, cumulative incidence function, proportional hazards model, subdistribution

1. Introduction

For medical studies involving competing risks, clinicians often wish to estimate and model the cumulative incidence probability of a specific cause of failure. In a published study [1] researchers compared the effectiveness of chemotherapy versus bone marrow transplantation (BMT) on the leukemia-free survival (LFS) for children with acute lymphoblastic leukemia (ALL) in second complete remission. The transplant cohort consisted of data from the International Bone Marrow Transplant Registry (IBMTR). Only patients receiving transplants were included in the IBMTR cohort, thus, the time to failure was left truncated by the transplant time. Leukemia patients were subject to competing risks of treatment failures, cancer relapse and treatment-related mortality (TRM), which is defined as death in complete remission. To understand the effect of prognostic factors on composite treatment failure, it is necessary to disentangle their separate effects on the cumulative incidences of these competing risks. Such analyses must deal appropriately with the left truncation for the BMT individuals.

Traditionally, the standard approach for analyzing competing risks data has been to estimate and model the cause-specific hazards for all causes. Let λk(t; z) be the hazard of the kth cause, conditional on the covariates z. Assuming k = 1, 2, the cumulative incidence function of cause 1 given z is defined as

F1(t;z)=P(Tt,ε=1z)=0texp[0s{λ1(u;z)+λ2(u;z)}du]λ1(s;z)ds,

where T is the failure time and ε indicates the cause of failure. For the right-censored competing risks data, F1(t; z) can be estimated by a plug-in estimator. Here, λk(t; z) must be modeled. Cheng et al. [2] considered the Cox model for both causes, Shen and Cheng [3] studied a special additive risk model, and recently, Scheike and Zhang [4, 5] proposed and studied a flexible Cox–Aalen model allowing some covariates to have time-varying effects. For left-truncated and right-censored competing risks data, the standard approaches to dealing with cause-specific hazard functions can be generalized to the left-truncated versions by adjusting the risk set [6].

For the standard approach, the covariate effect is assessed on each cause-specific hazard, creating a complex nonlinear modeling relationship for the cumulative incidence function. Fine and Gray [7] developed a method to directly model the cumulative incidence function by modeling a subdistribution hazard function, λ1(t;z)=dlog{1F1(t;z)}dt. They proposed a proportional subdistribution hazards model,

λ1(t;z)=λ10(t)exp{β0Tz}. (1)

The cumulative incidence function can be directly modeled as

F1(t;z)=1exp{exp(β0Tz)0tλ10(s)ds}.

Sun et al. [8] and Scheike et al. [9] considered some alternative models for the subdistribution hazard. For the right-censored competing risks data, Fine and Gray proposed using an inverse probability of censoring weighting (IPCW) technique to estimate β0 and the cumulative baseline subdistribution hazard function Λ10(t)=0tλ10(s)ds, and derived large sample properties of proposed estimators.

It is unknown how to fit Fine and Gray’s semiparametric subdistribution hazard model to left-truncated and right-censored competing risks data. The main focus of this paper is to find an appropriate weight for Fine and Gray’s method. Directly adopting Fine and Gray’s approach, one may consider using the left-truncated version Kaplan–Meier estimator of the censoring distribution for the weight. However, it can be easily seen that for an uncensored but truncated sample, the censoring probability weight equals to a constant 1, which leads to an ‘equal weight’ estimating procedure. We showed that, with no covariates, the estimates of a subdistribution hazard with a constant weight is obviously biased when the failure times are left truncated [10]. This indicates that IPCW is not an appropriate weight for left-truncated data.

In this paper, we derived a reciprocal of the truncation–censoring probability weight for a right-censored and left-truncated sample. We proposed two weights. The first weight estimator can be explained by a mass distribution algorithm [10], which leads to a standard left-truncated version of Aalen–Johansen’s estimator for the cumulative incidence function for the no covariate case. The second weight was derived from the conditional censoring distribution after delayed entry time. We have derived large sample properties for the proposed estimators. The performances of these two weights were studied through simulation. The estimators based on the proposed weights are shown to be asymptotically unbiased.

The outline of the remainder of the paper is as follows. In Section 2, we describe the data structure. In Section 3, we develop the inverse weighted estimation for the proportional subdistribution hazards model. Simulation studies are given in Section 4. In Section 5, we analyze a real data set, which was originally studied by Barrett et al. [1], to give an application of the model of interest. Concluding remarks are given in Section 6.

2. Left-truncated competing risks data

Suppose that there are two competing risks. Let Ti be the failure time and let Li and Ci be the left truncation time and the right censoring time, respectively. εi ∈ {1, 2} indicates the cause of failure. For left-truncated and right-censored data, Xi = min(Ti, Ci) and Δi = I{TiCi} are observed only if LiXi, where I{·} is the indicator function. Let Zi be the associated covariates. We assume that, given covariates Zi, Ti is independent from (Li, Ci). The observed data {Li , Xi , Δi , Δi εi , Zi} are independent and identically distributed for i = 1, … , n. Let GL be the distribution function of L.

For left-truncated and right-censored competing risks data, we define the underlying counting processes NiL,1(t)=I{LiTit,εi=1} and a modified risk indicator YiL,1(t)=I{(LitTi){(LiTit),εi=2}}. Note that NiL,1(t) and YiL,1(t) are not observable for all time t. Let ri(t)=I{Li≤(Tit)≤Ci}, where xy = min(x, y), then observed counting process Ni1(t)=ri(t)NiL,1(t)=I{LiXt,Δiεi=1} and observed modified risk indicator Yi1(t)=ri(t)YiL,1(t)=I{LitXi)(LiXit,Δiεi=2)} are computable for all time t.

3. Inverse weight for right-censored and left-truncated competing risks data

Estimation of the regression parameters in (1) with complete data follows the definition of a subdistribution hazard. Fine and Gray proposed maximizing the following partial likelihood:

i=1n[λ10(Ti)exp(βTZi)jRiλ10(Ti)exp(βTZj)]I(εi=1),

where Ri is the risk set at time Ti and is specially defined to include the alive subjects and the subjects failing from the other cause prior to Ti. For the right-censored competing risks data, Fine and Gray proposed using an inverse probability censoring weight and obtaining the MLE by solving the following weighted score estimating equation:

i=1n0[Zi(t)jκj(t)Yj1(t)Zjexp(βTZj)jκj(t)Yj1(t)exp(βTZj)]κi(t)dNi1(t)=0, (2)

where YiL,1(t), NiL,1(t), ri(t) agree with the definitions in Section 2 with Li = 0, weight κi(t)=ri(t)G^C(t)G^C(Xit), and G^C(t) is the Kaplan–Meier estimate of P(C>t). The IPCW technique has been routinely adopted for inferences about the cumulative incidence function with right-censored competing risks data [8, 9].

We propose the new weights to adjust for censoring and truncation and employ a weighted score estimation equation similar to equation (2) with proposed weights. Let GL,C(t|Z) = P(LtC|LX, Z). The proposed weights can be explained by E{ri(t)/GL,C(Xit|Zi)|Ti , LiXi , εi , Zi} = 1. In Sections 3.1 and 3.2, we introduce two inverse weights under the assumption that Ti is independent of Li and Ci given Zi . The large sample inferences are given in Section 3.3.

3.1. Weight 1

In Appendix A, we show that GL,C(XitZi)=b(XitZi)S(XitZi), where b(t|Zi ) = P(LitXi|LiXi , Zi) and S(t|Zi)= P(Ti>t|Zi). It follows that GL,C(Xit|Zi) can be estimated

G^L,C(XitZi)=b^(XitZi)S^(XitZi),

where b^(tZi) and S^(tZi) are the predicted estimators based on regression models. Here, we derived a time-dependent weight

w^i(tZi)=ri(t)G^L,C(XitZi)=ri(t)S^(XitZi)b^(XitZi).

Following Fine and Gray’s [7] approach, we consider a modified weight by multiplying a term b^(t)S^(t) to w^i(t)

w^i(1)(tZi)=ri(t)S^(XitZi)b^(t)b^(XitZi)S^(t), (3)

where b^(t)=n1iI{LitXi}, S^(t) is the left-truncated version of Kaplan–Meier estimator for the overall survival.

3.2. Weight 2

The left truncation time can be considered as delayed entry time since we observe only subjects from truncation time. Let T=L+T~ and C=L+C~. In theory, T~ and C~ may take negative values, although data are observed only if X~=(T~C~)=(TC)L0, i.e. only if T~0 and C~0. In Appendix A, we show that

GL,C(XtZ)=GC~X~0{(Xt)LZ}×K(XtZ),

where GC~X~0(tZ)=P(C~0X~0,t0,Z) and K(t|Z)= P(Lt|LX , Z).

Note that one can estimate GC~X~0(tZ) using the right-censored data {XiLi , 1–Δi , Zi; i = 1, … , n} and denoted as GC~X~0(tZ) and K(t|Z) can be estimated based on observed data {Li , Zi; i = 1, … , n} and denoted as K^(tZ). This leads to an alternative weight

w^i(2)(tZi)=ri(t)G^C~X~0{(Xit)LiZi}×K^(XitZi). (4)

The proposed weights are unknown in practice. It can be estimated nonparametrically if the weight function is independent of the covariates, i.e. GL,C(t|Z)= P(LtC|LX, Z) = P(LtC|LX). When the weight depends on the covariates, it needs to be estimated by a predicted value for each individual based on regression models, such as Aalen’s additive regression model. If there are few discrete covariates, a stratified nonparametric weight estimator can be used. For simplicity, we present nonparametric weight estimators

w^i(1)(t)=ri(t)S^(Xit)b^(t)b^(Xit)S^(t), (5)
w^i(2)(t)=ri(t)G^C~X~0{(Xit)Li}×K^(Xit), (6)

where GC~X~0(t) is the Kaplan–Meier estimator using the right-censored sample {XiLi , 1–Δi , i = 1, … , n}, and K^(t)=n1iI{Lit}.

Remarks

  1. For the left-truncated and right-censored competing risks data, when there is no covariate presented, the cumulative incidence function F1(t) is commonly estimated by an Aalen–Johansen estimator
    F^1AJ(t)=0tS^(u)dΛ^1(u),
    where Λ^1(u) is left-truncated version Nelson–Aalen estimator for cause 1 specific hazard. Adopting Efron’s [11] redistribution-to-right technique to the left-truncated and right-censored competing risks data, we showed that F1(t) can be estimated by a product-limit estimator of the subdistribution hazard using weight 1 given in (5)
    F^1PL(t)=1ut{1i=1nw^i(1)(u)dNiL,1(u)j=1nw^j(1)(u)YjL,1(u)},
    and we showed that F^1AJ(t)=F^1PL(t) (see [10] for detail). However, the product-limit estimator based on the alternative weight, w^i(2)(t), is not identical to the standard Aalen–Johansen’s nonparametric estimator of F^1AJ(t).
  2. We noted that model mis-specification is a critical issue for the covariate adjusted weight. Some exploratory study suggests the utilization of Aalen’s model for the covariate adjusted weight.

  3. Our aim of converting w^i(tZi) to w^i(1)(tZi) is to reduce the high variability contained in the original weight. The final nonparametric weight, w^i(1)(t), agrees with the stabilized form of the IPCW weights adopted in the same model for right-censored data [7]. The initial application of IPCW is characterized by the inverse of a censoring probability [12]. In dealing with dependent censoring, Robins and Finkelstein [13] aimed to discover the effects of covariate processes, V(t), and suggested a different IPCW weight G^C(t)G^C(t;V(t)). For this weight, G^C(t) is the Kaplan–Meier estimate and G^C(t;V(t)) is the adjusted survival estimate given the covariate processes up to time t.They stated that the weight 1G^C(t;V(t)) can be alternatively used, but the first IPCW weight has the advantage of efficiency. The term ‘stabilized weight’ appeared in the work on the causal inference of treatments [14] (see Section 6.1), where reduction in variability was mentioned as the motivation for adopting weight in the stabilized form.

  4. Similarly, the stabilized form for weight 2 can be considered
    ri(t)G^C~X~0{tLi}×K^(t)G^C~X~0{(Xit)Li}×K^(Xit).
    A limited simulation indicates that using this modified weight, the variability among the regression coefficient estimates has been greatly reduced. However, the bias becomes much greater (see Table III). More investigation is needed to find out the stabilized form for weight 2.
Table III.

Simulation results for comparing weight 2 and modified weight 2 (β11=0.5, β12=−0.5).

Weight 2
Modified weight 2
E(β^)
SD(β^)
E(β^)
SD(β^)
p C per cent L per cent β 11 β 12 β 11 β 12 β 11 β 12 β 11 β 12
C depends on L
0.7 25 25 0.511 −0.482 0.137 0.137 0.514 −0.477 0.112 0.116
50 25 0.503 −0.498 0.168 0.168 0.502 −0.476 0.130 0.135
25 50 0.527 −0.453 0.142 0.154 0.532 −0.428 0.120 0.123
50 50 0.515 −0.477 0.178 0.174 0.518 −0.427 0.139 0.139
0.5 25 25 0.521 −0.474 0.151 0.150 0.524 −0.467 0.130 0.131
50 25 0.518 −0.489 0.184 0.191 0.518 −0.470 0.145 0.157
25 50 0.533 −0.450 0.162 0.166 0.546 −0.421 0.134 0.139
50 50 0.536 −0.465 0.201 0.196 0.553 −0.404 0.154 0.158

3.3. Large sample inferences

The proposed weights can be utilized to estimate the parameters in model (1) by solving a weighted score estimating equation (2). For simplicity, we present large sample results based on nonparametric estimated weights. Similar asymptotic results can be derived for covariate adjusted weights which depend on the regression models used in the weight estimation. For weight w^i(k)(t), k = 1, 2, β can be estimated by solving U(k)(β^(k))=0, where

U(k)(β)=i=1n0{Zij=1nw^j(k)(t)YjL,1(t)Zjexp(ZjTβ)j=1nw^j(k)(t)YjL,1(t)exp(ZjTβ)}×w^i(k)(t)dNiL,1(t).

The cumulative baseline subdistribution hazards can be estimated by

Λ^10(k)(t)=i=1n0tw^i(k)(u)dNiL,1(u)jw^j(k)(u)YjL,1(u)exp(ZjTβ^(k)).

Using the basic empirical process theory as in Fine and Gray [7], we show briefly in Appendix B that, under the standard regular conditions [15] and assumption that Ti is independent of (Li, Ci) given Zi, β^(k) is a consistent estimator. n12(β^(k)β0) converges in distribution to a zero-mean Gaussian random vector, and its covariance matrix can be consistently estimated by

Σ^β(k)={n1I(k)(β^(k))}1×{n1i(W^β,i(k))2}×{n1I(k)(β^(k))}1,

where explicit expressions for I(k)(β) and W^β,i(k) are given in Appendix B.

Furthermore, we can show that n12{Λ^10(k)(t)Λ10(t)} converges weakly to a zero-mean Gaussian process, and the variance function can be consistently estimated by

Σ^Λ10(k)(t)=n1i=1n{W^Λ10,i(k)(t)}2,

where explicit expressions for W^Λ10,i(k)(t) are given in Appendix C.

The predicted cumulative incidence curve for a given set of covariate values is an important summary curve to show the treatment efficacy for a particular cause of failure over time. It can be predicted by a plug-in estimator

F^1(k)(t;z)=1exp{exp(zTβ^(k))0tdΛ^10(k)(u)}.

Using the functional delta method, we show that n12{F^1(k)(t;z)F1(t;z)} converges weakly to a zero-mean Gaussian process, and the variance function can be estimated by

Σ^F1(k)(t)=n1{1F^1(k)(t;z)}2i=1n{W^F1,i(k)(t;z)}2,

where explicit expressions for W^F1,i(k)(t;z) are given in Appendix D.

3.4. The censoring/truncation time is associated with some covariates

In this subsection, we consider the methods to estimate the covariates adjusted weight. When the censoring/truncation time depends on some discrete covariates, one can utilize the stratified nonparametric weight as given below. The data set can be summarized as {Lri, Xri, Δri, Δriεri, Zri}, for r = 1, ⋯ , R, and i = 1 , ⋯ , nr, where R is the number of strata. Let S^r(t) and b^r(t) be the relevant estimators for the rth strata. The stratified version of weight 1 has the form,

w~ri(t)=rri(t)S^r(Xrit)b^(t)b^r(Xrit)S^(t). (7)

As shown in Appendices B–D, variances of the regression parameter estimators consist of two parts. The first part corresponds to a model where the weight function is known. Scheike et al. [9] showed that the results based only on the first part lead to slightly conservative, but acceptable variance estimators. For simplicity, we present variance estimation based only on the major (first) part for stratified weight (see Appendix E for details). In our simulation study, we show that this simplified variance estimation approach leads to acceptable results.

When the censoring/truncation time is associated with a large number of covariates, one should consider constructing appropriate regression models and find the covariate adjusted weight. The covariate adjusted version of weight 1 requires estimation of P(T>t|z), P(L>t|LX, z) and P(X>t|LX, z). We consider Aalen’s model as the underlying regression models allowing time-varying effects. Let λT(t; z), λL|LX(t; z), λX|LX(t; z) be the hazard rate functions of the relevant random variables. We use the estimators S^T(t;z)=exp{0tλ^T(t;z)}, S^LLX;z=exp{0tλ^LLX(t;z)}, S^XLX;z=exp{0tλ^XLX(t;z)}, where the cumulative hazard estimates are obtained from the corresponding Aalen’s models. We further estimate b^(t;z)=S^XLX(t;z)S^LLX(t;z), and then the adjusted weight has the form

w~i(t)=ri(t)S^T(Xit;Zi)b^(t)b^(Xit;Zi)S^(t).

Using the regression model-based weight, the asymptotic expression of the weighted score function can be extended similarly, which contains some complex terms. The simple variance estimation method may be considered.

4. Simulation studies

We considered two simulation studies. For the first simulation study, the weight function is assumed to be independent of the covariates. We examine the performances of two nonparametric weight estimators. In the second simulation study, we simulated data similar to the BMT example data analyzed in Section 5, for which the weight function depended on a binary covariate. We compared the performances of a stratified nonparametric weight estimator with a non-stratified weight estimator.

4.1. Study 1

The underlying regression models include two covariates. Given covariate values z1 and z2, the cumulative incidence functions are given by

F1(t;z1,z2)=1{1p(1eγ1t)}exp(β11z1+β12z2)

and

F2(t;z1,z2)=(1p)exp(β11z1+β12z2)×{1eγ2texp(β21z1+β22z2)}.

The covariate effect on the cumulative incidence function of cause 1 can be assessed via a proportional subdistribution hazards model. γ1 and γ2 were set at 0.7 and 0.5, respectively. We let p = 0.7 to generate settings with a dominant risk, and p = 0.5 for settings with roughly equivalent risks. We considered both continuous covariates and discrete covariates. The continuous covariates Z1 and Z2 were generated from a standard normal distribution, and we set (β11, β12)=(0.5, –0.5) and (β21, β22)=(0.5, 0.5). The discrete covariates Z1 and Z2 were generated from a Bernoulli distribution with equal probability to fall on 1 or 0, and we set (β11, β12)=(1, 1) and (β21, β22)=(−1, 1).

In our simulation, the failure time is independent of the censoring and truncation time. Regarding C and L, they can be independent or C depends on L. Both were considered in our simulation to illustrate the difference in performance between weight 1 and 2. For the settings with independent C and L, the truncation time was generated from an exponential distribution with a hazard rate γl, and the censoring time was generated from a Uniform distribution in the interval [a, b]. A simulated observation would be discarded if either T <L or C <L. In order to obtain a sample with size n, a larger number of realizations of (T, C, L, Z1, Z2) need to be generated. The truncation rate is the percentage of the discarded observations out of all generated realizations. The censoring rate is the percentage of the censored observations out of n, based on the observed sample. In this study, we considered two levels of truncation rate (25 and 50 per cent) and three levels of the censoring rate (0, 25 and 50 per cent). Values of γl, a and b were selected so that the average truncation rate and censoring rate, based on 1000 replicates, coincided with the predetermined rates.

For the settings in which C depends on L, the left truncation time was still generated from an exponential distribution, and C~ was generated from N(μ, σ2). To obtain the predetermined censoring and truncation rates, μ and σ vary in the ranges 0.6–2.9 and 0.3–0.9, respectively. If TL or C~<0, the observation would be discarded; if not, we let the censoring time to be the sum of L and C~. T would be censored if it is greater than the censoring time.

For each setting, we simulated 1000 replicates with n = 200. The regression coefficients β11 and β12 should be estimated by the methods described in Section 3.3. We report the average estimated regression coefficients, E(β^), the sample standard deviation of β^, SD(β^) and the average of estimated standard error, E(se^). Tables I and II show the simulation results.

Table I.

Simulation results for continuous covariates (β11=0.5, β12=−0.5).

Weight 1
Weight 2
E(β^)
SD(β^)
E(se^)
E(se^)
E(β^)
SD(β^)
p C per cent L per cent β 11 β 12 β 11 β 12 β 11 β 12 β 11 β 12 β 11 β 12 β 11 β 12
C and L are independent
0.7 0 25 0.512 −0.496 0.113 0.105 0.103 0.104 0.513 −0.481 0.119 0.116 0.119 0.120
25 25 0.504 −0.497 0.114 0.114 0.110 0.112 0.506 −0.481 0.122 0.125 0.128 0.130
50 25 0.499 −0.509 0.129 0.130 0.127 0.128 0.499 −0.494 0.147 0.152 0.166 0.168
0 50 0.517 −0.488 0.135 0.133 0.118 0.120 0.516 −0.458 0.139 0.140 0.135 0.138
25 50 0.509 −0.495 0.128 0.134 0.120 0.122 0.511 −0.461 0.136 0.142 0.140 0.145
50 50 0.503 −0.499 0.141 0.138 0.132 0.133 0.506 −0.472 0.160 0.165 0.178 0.180
0.5 0 25 0.509 −0.499 0.125 0.124 0.119 0.119 0.515 −0.478 0.133 0.134 0.145 0.150
25 25 0.508 −0.507 0.131 0.132 0.126 0.127 0.512 −0.486 0.142 0.147 0.158 0.157
50 25 0.503 −0.517 0.147 0.151 0.143 0.144 0.507 −0.491 0.167 0.172 0.198 0.200
0 50 0.525 −0.489 0.155 0.146 0.137 0.137 0.535 −0.446 0.163 0.154 0.176 0.174
25 50 0.527 −0.497 0.147 0.148 0.139 0.139 0.538 −0.449 0.151 0.158 0.183 0.182
50 50 0.507 −0.501 0.160 0.155 0.150 0.150 0.516 −0.449 0.178 0.178 0.221 0.226
C depends on L
0.7 25 25 0.511 −0.500 0.116 0.120 0.111 0.112 0.511 −0.482 0.137 0.137 0.132 0.135
50 25 0.501 −0.507 0.133 0.140 0.130 0.131 0.503 −0.498 0.168 0.168 0.164 0.166
25 50 0.523 −0.487 0.132 0.130 0.122 0.125 0.527 −0.453 0.142 0.154 0.144 0.150
50 50 0.514 −0.499 0.151 0.147 0.139 0.142 0.515 −0.477 0.178 0.174 0.190 0.195
0.5 25 25 0.517 −0.497 0.135 0.134 0.126 0.126 0.521 −0.474 0.151 0.150 0.159 0.162
50 25 0.509 −0.512 0.151 0.159 0.147 0.146 0.518 −0.489 0.184 0.191 0.198 0.199
25 50 0.521 −0.494 0.149 0.151 0.141 0.141 0.533 −0.450 0.162 0.166 0.186 0.186
50 50 0.523 −0.502 0.172 0.169 0.159 0.160 0.536 −0.465 0.201 0.196 0.228 0.233

Table II.

Simulation results for discrete covariates (β11=1, β12=1).

Weight 1
Weight 2
E(β^)
SD(β^)
E(se^)
E(β^)
SD(β^)
E(se^)
p C per cent L per cent β 11 β 12 β 11 β 12 β 11 β 12 β 11 β 12 β 11 β 12 β 11 β 12
C and L are independent
0.7 0 25 1.003 1.014 0.165 0.178 0.164 0.167 1.003 1.018 0.191 0.194 0.184 0.186
25 25 1.009 1.011 0.188 0.186 0.182 0.182 1.002 1.010 0.210 0.207 0.202 0.201
50 25 1.001 0.995 0.220 0.218 0.217 0.217 1.006 1.006 0.255 0.268 0.263 0.264
0 50 1.010 1.024 0.187 0.209 0.177 0.188 0.985 1.018 0.207 0.207 0.202 0.206
25 50 1.010 1.018 0.191 0.202 0.188 0.190 0.993 1.011 0.218 0.227 0.213 0.214
50 50 1.003 1.004 0.232 0.223 0.219 0.219 1.000 0.999 0.269 0.265 0.275 0.274
0.5 0 25 1.009 1.011 0.189 0.193 0.180 0.182 0.992 1.013 0.212 0.214 0.205 0.204
25 25 1.012 1.009 0.205 0.200 0.196 0.195 0.998 1.000 0.223 0.223 0.220 0.220
50 25 1.007 0.995 0.236 0.238 0.231 0.229 0.993 1.000 0.287 0.279 0.283 0.282
0 50 1.004 1.025 0.220 0.230 0.200 0.209 0.958 1.040 0.234 0.230 0.224 0.229
25 50 1.001 1.023 0.218 0.214 0.208 0.210 0.954 1.029 0.238 0.236 0.236 0.237
50 50 1.010 0.993 0.244 0.250 0.236 0.234 0.984 0.999 0.290 0.296 0.299 0.301
C depends on L
0.7 25 25 1.005 1.014 0.186 0.188 0.181 0.181 1.004 1.009 0.212 0.214 0.207 0.207
50 25 1.004 1.014 0.220 0.223 0.218 0.218 1.012 1.018 0.275 0.285 0.265 0.267
25 50 1.011 1.006 0.201 0.201 0.190 0.193 0.995 1.009 0.228 0.232 0.222 0.222
50 50 1.010 1.015 0.223 0.236 0.223 0.224 1.005 1.010 0.282 0.289 0.285 0.285
0.5 25 25 1.017 1.006 0.199 0.208 0.196 0.194 1.002 1.010 0.231 0.248 0.226 0.225
50 25 1.001 1.004 0.238 0.243 0.234 0.232 1.013 1.005 0.297 0.298 0.291 0.289
25 50 0.989 1.011 0.220 0.221 0.211 0.213 0.948 1.021 0.248 0.243 0.242 0.244
50 50 1.003 1.017 0.259 0.258 0.246 0.245 0.972 1.021 0.311 0.317 0.317 0.316

It can be concluded from the above tables that the regression parameter estimates using the proposed weight estimators are very close to the true values under all the settings considered in this simulation study. For most of the settings, β^(1) and β^(2) yield indistinguishable results. Only with highly truncated settings, β^(1) departs slightly more from the true value than β^(2). The proposed variance estimators seem to satisfactorily measure the variations of the regression parameter estimates. Σ^β(2) gives well performance with discrete covariates, but slightly overestimates the true variance with continuous covariates. For the settings we considered, Σ^β(1) slightly underestimates the true variance. It can be observed that, in all the settings, the standard errors of β^(2) are noticeably higher than those of β^(1). This is due to the utilization of a stabilized weight for β^(1) as suggested by Robins and Finkelstein [13], as well as Robins et al. [14]. Weight 2 used for β^(2) is an unstabilized weight. A stabilized form for weight 2 is provided in Remark 4 of Section 3.2. We conducted a limited simulation to compare estimation performances between weight 2 and modified weight 2. Table III shows the simulation results, revealing that, for the modified weight, the variation among regression coefficient estimates is greatly reduced, but the bias increases. Further study is needed to investigate the proper stabilized form for weight 2.

4.2. Study 2

We conducted a simulation study to investigate the problem of dependent censoring and truncation, as well as the performance of the covariate adjusted weight. We generated a single binary covariate and let the underlying cumulative incidence functions to be

F1(t;z)=1{10.7(1e0.5t)}exp(β1z)

and

F2(t;z)=(10.7)exp(β1z){1e0.5exp(β2z)t}.

The censoring time and truncation time were generated from exponential distributions with the following hazard functions:

λC(t;z)=0.4exp(βCz)andλL(t;z)=1.8exp(βLz).

βC and βL have been set to different values for the first four settings. For the last setting, we generated the truncation times for z = 1 group only, which is similar to the BMT example data considered in Section 5.

Both the nonparametric weight estimator given in equation (5) and its stratified version have been implemented on the simulated settings. The simulation result given in Table IV shows that the stratified weight performed very well for the settings with dependence between the covariate and the truncation time, as well as the censoring time. The results based on the nonparametric weight are acceptable although the required assumptions are not fully satisfied. For the stratified weight, the estimated standard errors based on the simple variance estimation method are very close to the degree of the variability among the regression parameter estimates. It is practically feasible to employ this method to obtain a computationally efficient estimator.

Table IV.

Simulation results for settings with C, L dependent on one binary covariate (β1=1.0).

Nonparametric weight given in (5)
Stratified weight given in (7)
(βC, βL) (C per cent, L per cent) E(β^1) SD(β^1) E(se^) E(β^1) se(β^1) E(se^)
(−0.5, 0.7) (32, 29) 0.989 0.208 0.213 0.993 0.206 0.214
(0.5, 0.7) (43, 32) 0.943 0.245 0.230 0.996 0.245 0.231
(−0.5, −0.7) (36, 45) 1.074 0.211 0.209 1.006 0.213 0.212
(0.5, −0.7) (44, 49) 0.993 0.245 0.232 1.006 0.213 0.212
(−0.5, N/A) (36, 33*) 1.081 0.198 0.198 0.995 0.218 0.209

In the last setting, failure time is only truncated for z=1 group and the group-based truncation rate is given in the table.

5. A real example

Chemotherapy should be administered to children with relapsed leukemia until they achieve their second remission. There are two options to continuously treat children in their second remission: chemotherapy or BMT. Barrett et al. [1] conducted a study to compare effectiveness of these two treatments on the LFS. The response variable of their study was the time from the beginning of second remission to either leukemia relapse or TRM. The study cohort consisted of reported cases from two sources, the International Bone Marrow Transplant Registry (IBMTR) and the Pediatric Oncology Group (POG). The IBMTR cohort consists of 376 children who received transplantation in second complete remission, and the POG cohort collects 540 children who had been continuously treated by chemotherapy. It should be noted that the patients who died while waiting for BMT were not reported to IBMTR. Thus, the survival times of the children in the transplantation group were left truncated by the transplantation times. Meanwhile, the survival time in both groups was subject to right censoring. The censoring rate is 29 per cent for the BMT, and 44 per cent for the chemotherapy group. The end of the study was the major reason of censoring.

The goal of our study was to compare two treatments on the cumulative incidences of leukemia relapse and TRM, respectively, adjusting for significant risk factors. We considered the following risk factors: sex (0 if female; 1 if male), age (0 if ≤10 years; 1 if >10 years), leukocyte count at diagnosis (0 if ≤100000 cells/mm3; 1 if >100000 cells/mm3), the T-cell phenotype (0 if no; 1 if yes), duration of the first remission (0 if ≤18 months; 1 if >18 months), and year of diagnosis (0 if before 1984; 1 if after 1984). For each competing risk, we constructed both the proportional cause-specific hazards model and the proportional subdistribution hazards model. A forward stepwise selection procedure was used to identify significant risk factors with criterion 0.05.

For this example, the nonparametric weight is not appropriate since left truncation is present only in the transplantation group, thus, the truncation time is associated with the covariate for the treatment group. We utilized the stratified weight discussed in Section 3.4, with treatment groups serving as strata. The results of model construction for leukemia relapse are given in Table V. For the model on the cause-specific hazard, duration of the first remission (DCR) and the T-cell phenotype were identified as significant risk factors. However, DCR was the only risk factor significantly associated with the subdistribution hazard. For TRM (see Table VI), T-cell phenotype, year of diagnosis (DXYR84) and sex (Male) were identified as significant risk factors for both models. Age was marginally significant for the model on the cause-specific hazard, but was not significant for the model on the subdistribution hazard.

Table V.

Estimates of regression coefficients and standard errors for leukemia relapse.

Cause-specific hazard
Subdistribution hazard
β^ SE p-Value β^ SE p-Value
BMT −0.875 0.113 <0.001 −1.250 0.123 <0.001
DCR −0.938 0.097 <0.001 −0.806 0.105 <0.001
T-cell 0.306 0.142 0.038

Table VI.

Estimates of regression coefficients and standard errors for TRM.

Cause-specific hazard
Subdistribution hazard
β^ SE p-Value β^ SE p-Value
BMT 1.649 0.232 <0.001 2.013 0.224 <0.001
T-cell 1.060 0.251 <0.001 0.885 0.281 0.002
DXYR84 −0.528 0.201 0.009 −0.692 0.221 0.002
Male −0.398 0.193 0.039 −0.409 0.208 0.049
Age 0.388 0.196 0.048

The predicted cumulative incidence curves of leukemia relapse for two treatments are given in Figure 1, where the significant risk factor, duration of the first remission, is set at >18 months. A 95 per cent log–log transformed pointwise confidence interval is also plotted in the figure. Figure 2 gives the predicted cumulative incidence curves of TRM for a boy without the T-cell phenotype and diagnosed after 1984, together with a 95 per cent log–log transformed confidence interval.

Figure 1.

Figure 1

Predicted cumulative incidences of leukemia relapse for chemotherapy (solid) and BMT (dashes) based on a child with duration of first remission >18 months.

Figure 2.

Figure 2

Predicted cumulative incidences of TRM for chemotherapy (solid) and BMT (dashes) based on a boy without T-cell phenotype and diagnosed after 1984.

6. Concluding remarks

In this paper, we have extended the proportional subdistribution hazards model to the right-censored and left-truncated competing risks data. The crucial adjustment with truncated data is to adopt the reciprocal of the truncation–censoring probability GL,C(Xit|Zi ) as the weight. When the weight does not depend on the covariates Z, we proposed two nonparametric estimators for GL,C(Xit). The first estimator uses the estimate of the survival probability of the all-cause failure time T and the second estimator includes the estimate of P(CL>t). We have shown that the first weight estimator can be fully explained by the mass of a subject at time t [10] and leads to the Aalen–Johansen estimator of the cumulative incidence function, yet the second weight estimator does not have this property.

For the first weight estimator, the stabilized version was proposed and utilized, which causes a noticeably lower degree of the variability in the regression parameter estimates. Further study is needed to improve the second weight estimator and hence reduce the variability of the regression parameter estimates.

The covariate adjusted weight can be potentially adopted. We have shown in this paper that the stratified nonparametric weight is a proper solution when the censoring/truncation time is associated with some discrete covariates. One may consider the covariate adjusted weight based on some regression models. However, it is difficult to choose proper models when certain type of the subdistribution hazard model is given. Such a problem has been indirectly addressed by Latouche et al. [16] by clarifying that a proportional subdistribution hazards model does not coexist with a proportional cause-specific hazards model. We suggested using Aalen’s model and further study in this direction is needed.

Acknowledgements

Dr Mei-Jie Zhang’s research was supported by National Cancer Institute grant RO1 CA54706-13.

Appendix A

Here, we show that GL,C(Xt|Z)=b(Xt|Z)/S(Xt|Z) under the assumption that T is independent of L and C given covariates Z . Since

b(tZ)=P{Lt(TC),L(TC)Z}P(LXZ)=P(Tt,LtCZ)P(LXZ)=P(TtZ)×P(LtCZ)P(LXZ)

it follows that

b(XtZ)=S(XtZ)×P(L(Xt)CZ)P(LXZ)=S(XtZ)×P{L(Xt)CLX,Z}=S(XtZ)GL,C(XtZ).

Next, we show that GL,C(XtZ)=GC~X~0{(Xt)LZ}×K(XtZ), where GC~X~0(tZ)=P(C~tX~0,t0,Z) and K(t|Z)= P(Lt|LX, Z). For the left-truncated and right-censored data, individuals are observed only if LX, which is equivalent to X~=XL0. It follows that

P(L(Xt)CLX,Z)=P(0[(Xt)L]C~X~0,Z)=P(C~[(Xt)L],L(Xt)X~0,Z)=P(C~[(Xt)L](Xt)L0,X~0,Z)×P(L(Xt)LX,Z).

Appendix B: Weak convergence of n−1/2U(k)(β0)

For k = 1, 2, define the following notations:

Sk(p)=n1i=1nw^i(k)(t)YiL,1(t)Zipexp(ZiTβ)p=0,1,2,I(k)(β)=(U(k)(β)β)=i=1n0{Sk(2)(β,t)Sk(0)(β,t)(Sk(1)(β,t)Sk(0)(β,t))2}d{w^i(k)(t)Ni1(t)}.

Let

sk(p)(β,u)=limnSk(p)(β,u)p=0,1,2,Ω(k)=limnn1I(k)(β).

Taking a Taylor expansion on U(k)(β) around U(β0), we obtain

n12(β^β0)P(Ω(k))1n12U(k)(β0).

Considering weight 1 and following Fine and Gray’s [7] arguments, we have

n12U(1)(β0)Pn12i=1n0{Zi(u)s1(1)(β0,u)s1(0)(β0,u)}wi(1)(u)dMiL,1(u)+n12i=1n0{Zi(u)s(1)(β0,u)s1(0)(β0,u)}b^(u)b^(Xiu){S^(Xiu)S^(u)S(Xiu)S(u)}×ri(u)dMiL,1(u)+n12i=1n0{Zi(u)s1(1)(β0,u)s1(0)(β0,u)}S(Xiu)S(u){b^(u)b^(Xiu)b(u)b(Xiu)}×ri(u)dMiL,1(u),

where wi(1)(t)=ri(t)GL,C(t)GL,C(Xit) and MiL,1(t)=NiL,1(t)0tYiL,1(u)λ10(u)exp(ZiTβ0)du is a martingale.

The first term is the main term, whereas the second and third terms account for the influence due to random weight. The left-truncated Kaplan–Meier estimator in the second term can be further expressed by

S^(Xit)S^(t)=I(Xi<t){S^(Xi)S(Xi)S^(t)+S(Xi)(1S^(t)1S(t))}pS(Xi)S(t)j=1n0I(Xi<u<t)dMj(u)k=1nI(LkuXk),

where Mj(t)=I{Xjt,εj(1,2)}0tI(LjuXj)λ(u)du is the martingale with respect to the self-exciting filtration (see [17, pp. 433 and 434]), and λ(u) is the hazard rate for the failure of all causes.

For the third term,

b^(t)b^(Xit)b(t)b(Xit)=I(Xi<t)[1b^(Xi){b^(t)b(t)}+b(t){1b^(Xi)1b(Xi)}]PI(Xi<tnb(Xi))j=1n{I(LjtXj)b(t)}+I(xi<t)b(t)nb(Xi)2j=1n{b(Xi)I(LjXiXj)}=I(Xi<t)b(t)nb(Xi)j=1n{1b(t)I(LjtXj)1b(Xi)I(LjXiXj)}.

Summarizing the above derivations, we obtain the asymptotically equivalent expression of n−1/2U(1)(β0)

n12U(1)(β0)n12Wβ,i(1)n12i=1n{ϕi+χi+ψi},

where

ϕi=0{Zis1(1)(β0,t)s1(0)(β0,t)}wi(1)(t)dMiL,1(t),χi=0q(u)π(u)dMi(u),q(u)=limnn1j=1n0{Zjs1(1)(β0,s)s1(0)(β0,s)}wj(1)(s)dMjL,1(s)I(Xj<u<s),π(u)=limnn1j=1nI(LjuXj),ψi=limnn1j=1n0{Zjs1(1)(β0,s)s1(0)(β0,s)}wj(1)(s)dMjL,1(s)I(Xj<s)×{I(LisXi)b(s)I(LiXjXi)b(Xj)}.

Note that Wβ,i(1)’s can be viewed as zero-mean iid random vectors. Using the multivariate central limit theorem, n−1/2U(1)(β0) converges in distribution to a zero-mean Gaussian random vector and the covariance matrix can be consistently estimated by

n1i(W^β,i(1))2,

where

W^β^,i(1)=ϕ^i+χ^i+ψ^i,ϕ^i=0{ZiS1(1)(β^(1),t)S1(0)(β^(1),t)}w^i(1)(t)dM^iL,1(t),χ^i=0q^(u)π^(u)dM^i(u),q^(u)=n1i0{ZiS1(1)(β^(1),s)S1(0)(β^(1),s)}w^i(1)(s)dM^iL,1(s)I(Xj<u<s),π^(u)=n1iI(LiuXi),ψ^i=n1j0{ZjS(1)(β^(1),s)S(0)(β^(1),s)}w^j(1)(s)dM^jL,1(s)I(Xj<s)×{I(LisXi)b^(s)I(LiXjXi)b^(Xj)},M^j(t)=I(Xjt,εj{1,2})0tI(LjuXj)dΛ^(u),Λ^(t)=i0tdI(Xiu,εi{1,2})jI(LjuXj).

When utilizing weight 2, we can similarly show that n−1/2U(2)(β0) is asymptotically equivalent to n12Wβ,i(2), which has a zero-mean normal distribution and the covariance matrix can be consistently estimated by

n1i(W^β,i(2))2,

where

W^β,i(2)=γ^i+η^i+θ^i,γ^i=0{ZiS2(1)(β^(2),t)S2(0)(β^(2),t)}w^i(2)(t)dM^iL,1(t),η^i=0α^(u)π^(u)dM^ic(u),α^(u)=n1j=1n0{ZiS2(1)(β^(2),s)S2(0)(β^(2),s)}w^j(2)(s)dM^jL,1(s)I(u{(Xjs)Lj}),θ^i=n1j=1n00{ZiS2(1)(β^(2),s)S2(0)(β^(2),s)}w^j(2)(s)dM^jL,1(s){1I(Li(Xjs))K^(Xjs)},w^i(2)(t)M^iL,1(t)=w^i(2)(t)NiL,1(t)0tw^i(2)(u)YiL,1(u)exp(ZiTβ^(2))dΛ^10(2)(u),M^jc(t)=I(XjLjt,εj=0)0tI(XjLju)dΛ^c(u),Λ^c(t)=i0tdI(XiLiu,εi=0)jI(XjLju).

Appendix C: Weak convergence of n12{Λ^10(k)Λ10(t)}

By Taylor expansion

n12{Λ^10(1)(t)Λ10(t)}Pn12i=1n0tw^i(1)(u)dMiL,1(u)s1(0)(β0,u)0t{s1(1)(β0,u)}Ts1(0)(β0,u)dΛ10(u)n{β^(1)β0}Pn12i=1n0twi(u)dMiL,1(u)s1(0)(β0,u)0t{s1(1)(β0,u)}Ts1(0)(β0,u)dΛ10(u)n{β^(1)β0}+n12i0t{w^i(1)(u)wi(u)}dMiL,1(u)s1(0)(β0,u)Pn12iWΛ10,i(1)(t),

where

WΛ10,i(1)(t)=0twi(u)dMiL,1(u)s1(0)(β0,u)0t{s1(1)(β0,u)}Ts1(0)(β0,u)dΛ10(u)(Ω(1))1(ϕi+χi+ψi)+0v(u,t)π(u)dMi(u)+μi(t)v(u,t)=limnn1j=1n0twj(1)(s)dMjL,1(s)s1(0)(β0,s)I(Xj<u<s),μi(t)=limnn1j=1n0twj(1)(s)dMjL,1(s)s1(0)(β0,s)I(Xj<s){I(LisXi)b(s)I(LiXjXi)b(Xj)}.

By the central limit theorem, n12{Λ^10(1)Λ10(t)} converges in finite-dimensional distribution to a zero-mean Gaussian process. Using the empirical theory as in Fine and Gray [7], and in Lin et al. [18], we can show that n12WΛ10,i(1)(t) is tight. Thus, n12{Λ^10(1)Λ10(t)} converges weakly to a zero-mean Gaussian process and its variance can be consistently estimated by

Σ^Λ10(1)(t)=n1i=1n{W^Λ10,i(1)(t)}2,

where

W^Λ10,i(1)(t)=0tw^i(1)(u)dM^iL,1(u)S1(0)(β^(1),u)0t(S1(1)(β^(1),u))TS1(0)(β^(1),u)dΛ^10(1)(u){n1I(1)(β^(1))}1(ϕ^i+χ^i+ψ^i)+0v^(u,t)π^(u)dM^i(u)+μ^i(t),v^(u,t)=j0tw^j(1)(s)dM^jL,1(s)S1(0)(β^(1),s)I(Xj<u<s),μ^i(t)=j0tw^j(1)(s)dM^jL,1(s)S1(0)(β^(1),s)I(Xj<s){I(LisXi)b^(s)I(LiXjXi)b^(Xj)}.

Using weight 2, it can be similarly shown that n12{Λ^10(2)Λ10(t)} converges weakly to a zero-mean Gaussian process and its variance can be consistently estimated by Σ^Λ10(2)(t)=n1i=1n{W^Λ10,i(2)(t)}2

W^Λ10,i(2)(t)=0tw^i(2)(u)dM^iL,1(u)S2(0)(β^(2),u)0t(S2(1)(β^(2),u))TS2(0)(β^(2),u)dΛ^10(2)(u){n1I(2)(β^(2))}1(γ^i+η^i+θ^i)+0ρ^(u,t)π^(u)dM^ic(u)+φ^i(t),ρ^(u,t)=n1j=1n0tw^j(2)(s)dM^jL,1(s)S2(0)(β^(2),s)I(u{(Xjs)Lj}),φ^i(t)=j=1n0tw^j(2)(s)dM^jL,1(s)S2(0)(β^(2),s){1I(Li(Xjs))K^(Xjs)}.

Appendix D: Weak convergence of n12{F^1(k)(t;z)F1(t;z)}

Utilizing the functional delta method

n12{F^1(1)(t;z)F1(t;z)}Pn12{1F1(t;z)}{exp(zTβ^(1))exp(zTβ0)}Λ^10(1)(t)+n12{1F1(t;z)}exp(zTβ0){Λ^10(1)(t)Λ10(t)}.

Similarly, if follows that n12{F^1(1)(t;z)F1(t;z)} weakly converges to a zero-mean Gaussian process, and the variance can be consistently estimated by

Σ^F1(1)(t)=n1{1F^1(1)(t;z)}2i=1n{W^F1,i(1)(t;z)}2,

where

W^F1,i(1)(t;z)=0texp(zTβ^(1))w^i(1)(u)dM^iL,1(u)S(0)(β^(1),u)+{h^(1)(t;z)}T{β^(1)}1(ϕ^i+χ^i+ψ^i)+0exp(zTβ^(1))v^(u,t)π^(u)dM^i(u)+exp(zTβ^(1))μ^i(t),h^(1)(t;z)=0t{zS1(1)(β^(1),u)S1(0)(β^(1),u)}exp(zTβ^(1))dΛ^10(1)(u).

For weight 2, the variance of the limiting distribution of n12{F^1(2)(t;z)F1(t;z)} can be consistently estimated by

Σ^F1(2)(t)=n1{1F^1(2)(t;z)}2i=1n{W^F1,i(2)(t;z)}2,

where

W^F2,i(1)(t;z)=0texp(zTβ^(2))w^i(2)(u)dM^iL,1(u)S(0)(β^(2),u)+{h^(2)(t;z)}T{β^(2)}1(γ^i+η^i+θ^i)+0exp(zTβ^(2))ρ^(u,t)π^(u)dM^ic(u)+exp(zTβ^(2))φ^i(t),h^(2)(t;z)=0t{zS2(1)(β^(2),u)S2(0)(β^(2),u)}exp(zTβ^(2))dΛ^10(2)(u).

Appendix E

Let β~ be the solution to the score estimating equation using stratified weight (7). For simplicity, treating the weight function known, the variance of n12{β~β} can be estimated by

Σ~β={n1I(β~)}1×{n1r=1Ri=1nr(ν^ri)2}×{n1I(β~)}1,

where

S(p)(β,t)=n1r=1Ri=1nrw~ri(t)YriL,1(t)Zripexp(ZriTβ)p=0,1,2,I(β)=r=1Ri=1nr0{S(2)(β,t)S(0)(β,t)(S(1)(β,t)S(0)(β,t))2}d{w~ri(t)NriL,1(t)},ν^ri=0{ZriS(1)(β~,t)S(0)(β~,t)}w~ri(t)dM^riL,1(t),w~ri(t)M^riL,1(t)=w^ri(t)NriL,1(t)0tw~ri(u)YriL,1(u)exp(ZriTβ~)dΛ~10(u),Λ~10(t)=r=1Ri=1nr0tdI(Xriu,εri{1,2})l=1Rj=1nlI(LljuXlj).

Let F~1(t;z) be the estimator of the cumulative incidence function given z. Similarly, we estimate the asymptotic variance of F~1(t;z) by

n1{1F~1(t;z)}2r=1Ri=1nr{W~F1,ri(t;z)}2,

where

W~F1,ri(t;z)=0texp(zTβ~)w~ri(u)dM^riL,1(u)S(0)(β~,u)+{h~(t;z)}T{n1I(β~)}1ν^ri,h~(t;z)=0t{zS(1)(β~,u)S(0)(β~,u)}exp(zTβ~)dΛ~10(u).

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