Accelerated failure time model
In the statistical area of survival analysis, an accelerated failure time model (AFT model) is a parametric model that provides an alternative to the commonly used proportional hazards models. Whereas a proportional hazards model assumes that the effect of a covariate is to multiply the hazard by some constant, an AFT model assumes that the effect of a covariate is to accelerate or decelerate the life course of a disease by some constant. This is especially appealing in a technical context where the 'disease' is a result of some mechanical process with a known sequence of intermediary stages.
In full generality, the accelerated failure time model can be specified as
\lambda(t|\theta)=\theta\lambda_0(\theta t) </math> where <math>\theta</math> denotes the joint effect of covariates, typically <math>\theta=\exp(-[\beta_1X_1 + \cdots + \beta_pX_p])</math>. (Specifying the regression coefficients with a negative sign implies that high values of the covariates increase the survival time, but this is merely a sign convention; without a negative sign, they increase the hazard.)
This is satisfied, if the probability density function of the event is taken to be <math>f(t|\theta)=\theta f_0(\theta t)</math>, from which is follows for the survival function that <math>S(t|\theta)=S_0(\theta t)</math>. From this it is easy to see that the moderated life time <math>T</math> is distributed such that <math>T\theta</math> and the unmoderated life time <math>T_0</math> have the same distribution. Consequently, <math>log(T)</math> can be written as
log(T)=-log(\theta)+log(T\theta):=-log(\theta)+\epsilon </math> where the last term is distributed as <math>log(T_0)</math>, i.e. independently of <math>\theta</math>. This reduces the accelerated failure time model into regression analysis (typically a linear model) where <math>-log(\theta)</math> represents the fixed effects, and <math>\epsilon</math> represents the noise. Different distributional forms of <math>\epsilon</math> imply different distributional forms of <math>T_0</math>, i.e. different baseline distributions of the survival time. It is typical of survival-analytic contexts, that many of the observations are censored, i.e. we only know that <math>T_i>t_i</math>, not <math>T_i=t_i</math>. In fact, the former case represents survival, while the later case represents an event/death/censoring during the follow-up. These right-censored observations can pose technical challenges for estimating the model, if the distribution of <math>T_0</math> is unusual.
The interpretation of <math>\theta</math> in accelerated failure time models is straight forward: E.g. <math>\theta=2</math> means that everything in the relevant life history of an individual happens twice as fast. For example, if the model concerns the development of a tumor, it means that all of the pre-stages progress twice as fast as for the unexposed individual, implying that the expected time until a clinical disease is 0.5 of the baseline time. However, this does not mean that the hazard function <math>\lambda(t|\theta)</math> is always twice as high - that would be the proportional hazards model.
Unlike proportional hazards models, in which Cox's semi-parametric proportional hazards model is more widely used than parametric models, AFT models are predominantly fully parametric i.e. a probability distribution is specified for <math>log(T_0)</math>. (Buckley and James proposed a semi-parametric AFT but its use is relatively uncommon in applied research; in a 1992 paper, Wei pointed out that the Buckley–James model has no theoretical justification and lacks robustness, and reviewed alternatives.) This can be a problem, if a degree of realistic detail is required for modelling the distribution of a baseline lifetime. Hence, technical developments in this direction would be highly desirable.
The results of AFT models are easily interpreted. For example, the results of a clinical trial with mortality as the endpoint could be interpreted as a certain percentage increase in future life expectancy on the new treatment compared to the control. So a patient could be informed that he would be expected to live (say) 15% longer if he took the new treatment. Hazard ratios can prove harder to explain in layman's terms.
Distributions used in AFT models
The log-logistic distribution provides the most commonly used AFT model. Unlike the Weibull distribution, it can exhibit a non-monotonic hazard function which increases at early times and decreases at later times. It is similar in shape to the log-normal distribution but its cumulative distribution function has a simple closed form, which becomes important computationally when fitting data with censoring. For the censored observations one needs the survival function, which is the complement of the cumulative distribution function, i.e. one needs to be able to evaluate <math>S(t|\theta)=1-F(t|\theta)</math>.
The Weibull distribution (including the exponential distribution as a special case) can be parameterised as either a proportional hazards model or an AFT model, and is the only family of distributions to have this property. The results of fitting a Weibull model can therefore be interpreted in either framework. However, the biological applicability of this model may be limited by the fact that the hazard function is monotonic, i.e. either decreasing or increasing.
Other distributions suitable for AFT models include the log-normal, gamma and inverse Gaussian distributions, although they are less popular than the log-logistic, partly as their cumulative distribution functions do not have a closed form. Finally, the generalized gamma distribution is a three-parameter distribution that includes the Weibull, log-normal and gamma distributions as special cases.
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