A standard generalization of the BT model is the Plackett–
Luce model, which models ranking N items. In the same notation as BT model: \Pr(y_1 > \cdots > y_N) = \prod_{i=1}^N \frac{p_{y_i}}{\sum_{k=i}^N p_{y_k}} = \frac{p_{y_1}}{p_{y_1} + \dots + p_{y_N}}\frac{p_{y_2}}{p_{y_2} + \cdots + p_{y_N}} \cdots \frac{p_{y_N}}{p_{y_N}} The factor with i=N is always just unity, so for N=2 this reduces to \Pr(y_1 > y_2) = p_{y_1}/(p_{y_1} + p_{y_2}). This can be imagined as
drawing from an urn with replacement. The urn contains balls colored in proportion to p_1, p_2, \dots, p_N, and one draws from the urn with replacement. If a ball has a new color, then that ball is placed as the next-ranked ball. Otherwise, if the ball has a color already drawn, then it is discarded. Given the proportions p_1, p_2, \dots, p_N, the PL model can be sampled by the "exponential race" method. One samples "
radioactive decay times" from N "
exponential clocks", that is, t_1 \sim \mathrm{Exp}(p_1), \dots, t_N \sim \mathrm{Exp}(p_N). Then one ranks the items according to the order in which they decayed. In this interpretation, it is immediately clear that the PL model satisfies
Luce's choice axiom (from the same Luce). Therefore, for any two y, z, \Pr(y > z) = \frac{p_y}{p_y + p_z} reduces to the BT model, and in general, for any subset y_1, \dots, y_M of the choices, \Pr(y_1 > \cdots > y_N) = \frac{p_{y_1}}{p_{y_1} + \cdots + p_{y_M}}\frac{p_{y_2}}{p_{y_2} + \cdots + p_{y_M}} \cdots \frac{p_{y_M}}{p_{y_M}} reduces to a smaller PL model with the same parameters. == Inference ==