Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions, voting power, and political instability Andrew Gelman Department of Statistics and Department of Political Science Columbia University 25 Oct 2005 Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Topics I Coalition-formation as a prisoner’s dilemma: a potential theoretical explanation for political instability I Mathematical and statistical models of voting power Both topics involve: I I I I Open problems in mathematics (probability theory, cellular automata) Open problems in political science (connections to empirical data) Collaboration with Francis Tuerlinckx, Joe Bafumi, and Jonathan Katz Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Topics I Coalition-formation as a prisoner’s dilemma: a potential theoretical explanation for political instability I Mathematical and statistical models of voting power Both topics involve: I I I I Open problems in mathematics (probability theory, cellular automata) Open problems in political science (connections to empirical data) Collaboration with Francis Tuerlinckx, Joe Bafumi, and Jonathan Katz Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Topics I Coalition-formation as a prisoner’s dilemma: a potential theoretical explanation for political instability I Mathematical and statistical models of voting power Both topics involve: I I I I Open problems in mathematics (probability theory, cellular automata) Open problems in political science (connections to empirical data) Collaboration with Francis Tuerlinckx, Joe Bafumi, and Jonathan Katz Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Topics I Coalition-formation as a prisoner’s dilemma: a potential theoretical explanation for political instability I Mathematical and statistical models of voting power Both topics involve: I I I I Open problems in mathematics (probability theory, cellular automata) Open problems in political science (connections to empirical data) Collaboration with Francis Tuerlinckx, Joe Bafumi, and Jonathan Katz Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Topics I Coalition-formation as a prisoner’s dilemma: a potential theoretical explanation for political instability I Mathematical and statistical models of voting power Both topics involve: I I I I Open problems in mathematics (probability theory, cellular automata) Open problems in political science (connections to empirical data) Collaboration with Francis Tuerlinckx, Joe Bafumi, and Jonathan Katz Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Topics I Coalition-formation as a prisoner’s dilemma: a potential theoretical explanation for political instability I Mathematical and statistical models of voting power Both topics involve: I I I I Open problems in mathematics (probability theory, cellular automata) Open problems in political science (connections to empirical data) Collaboration with Francis Tuerlinckx, Joe Bafumi, and Jonathan Katz Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Topics I Coalition-formation as a prisoner’s dilemma: a potential theoretical explanation for political instability I Mathematical and statistical models of voting power Both topics involve: I I I I Open problems in mathematics (probability theory, cellular automata) Open problems in political science (connections to empirical data) Collaboration with Francis Tuerlinckx, Joe Bafumi, and Jonathan Katz Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Coalitions and political instability First part of the talk Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Coalitions in an election with 9 voters I Several possibilities: I I I I I No coalitions Single coalition of 9 voters Single coalition of 3 voters Three coalitions of 3 voters each Compute Pr (voter is decisive) for: I I I voters in a coalition voters outside the coalition average over all 9 voters Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Coalitions in an election with 9 voters I Several possibilities: I I I I I No coalitions Single coalition of 9 voters Single coalition of 3 voters Three coalitions of 3 voters each Compute Pr (voter is decisive) for: I I I voters in a coalition voters outside the coalition average over all 9 voters Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Coalitions in an election with 9 voters I Several possibilities: I I I I I No coalitions Single coalition of 9 voters Single coalition of 3 voters Three coalitions of 3 voters each Compute Pr (voter is decisive) for: I I I voters in a coalition voters outside the coalition average over all 9 voters Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Coalitions in an election with 9 voters I Several possibilities: I I I I I No coalitions Single coalition of 9 voters Single coalition of 3 voters Three coalitions of 3 voters each Compute Pr (voter is decisive) for: I I I voters in a coalition voters outside the coalition average over all 9 voters Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Coalitions in an election with 9 voters I Several possibilities: I I I I I No coalitions Single coalition of 9 voters Single coalition of 3 voters Three coalitions of 3 voters each Compute Pr (voter is decisive) for: I I I voters in a coalition voters outside the coalition average over all 9 voters Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Coalitions in an election with 9 voters I Several possibilities: I I I I I No coalitions Single coalition of 9 voters Single coalition of 3 voters Three coalitions of 3 voters each Compute Pr (voter is decisive) for: I I I voters in a coalition voters outside the coalition average over all 9 voters Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Coalitions in an election with 9 voters I Several possibilities: I I I I I No coalitions Single coalition of 9 voters Single coalition of 3 voters Three coalitions of 3 voters each Compute Pr (voter is decisive) for: I I I voters in a coalition voters outside the coalition average over all 9 voters Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Coalitions in an election with 9 voters I Several possibilities: I I I I I No coalitions Single coalition of 9 voters Single coalition of 3 voters Three coalitions of 3 voters each Compute Pr (voter is decisive) for: I I I voters in a coalition voters outside the coalition average over all 9 voters Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Coalitions in an election with 9 voters I Several possibilities: I I I I I No coalitions Single coalition of 9 voters Single coalition of 3 voters Three coalitions of 3 voters each Compute Pr (voter is decisive) for: I I I voters in a coalition voters outside the coalition average over all 9 voters Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Coalitions in an election with 9 voters I Several possibilities: I I I I I No coalitions Single coalition of 9 voters Single coalition of 3 voters Three coalitions of 3 voters each Compute Pr (voter is decisive) for: I I I voters in a coalition voters outside the coalition average over all 9 voters Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems “Voting power” vs. “satisfaction” I Voting power: Pr (voter is decisive) I Satisfaction: Pr (your desired outcome wins) Not the same: I I I Consider an election in which 90% of the voters vote for A and 10% vote for B: Almost everyone is satisfied but voters have essentially no power. Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems “Voting power” vs. “satisfaction” I Voting power: Pr (voter is decisive) I Satisfaction: Pr (your desired outcome wins) Not the same: I I I Consider an election in which 90% of the voters vote for A and 10% vote for B: Almost everyone is satisfied but voters have essentially no power. Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems “Voting power” vs. “satisfaction” I Voting power: Pr (voter is decisive) I Satisfaction: Pr (your desired outcome wins) Not the same: I I I Consider an election in which 90% of the voters vote for A and 10% vote for B: Almost everyone is satisfied but voters have essentially no power. Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems “Voting power” vs. “satisfaction” I Voting power: Pr (voter is decisive) I Satisfaction: Pr (your desired outcome wins) Not the same: I I I Consider an election in which 90% of the voters vote for A and 10% vote for B: Almost everyone is satisfied but voters have essentially no power. Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems “Voting power” vs. “satisfaction” I Voting power: Pr (voter is decisive) I Satisfaction: Pr (your desired outcome wins) Not the same: I I I Consider an election in which 90% of the voters vote for A and 10% vote for B: Almost everyone is satisfied but voters have essentially no power. Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems “Voting power” vs. “satisfaction” I Voting power: Pr (voter is decisive) I Satisfaction: Pr (your desired outcome wins) Not the same: I I I Consider an election in which 90% of the voters vote for A and 10% vote for B: Almost everyone is satisfied but voters have essentially no power. Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Coalition-formation as a “prisoner’s dilemma” Payoffs (in terms of your own voting power) from coalition: Your option Stay alone Join a coalition Have other voters formed coalitions? No Yes Moderate Very low High Low I Joining a coalition increases your voting power I But if all voters form a coalition, they all have low voting power I Suboptimal outcome if all players act rationally Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Coalition-formation as a “prisoner’s dilemma” Payoffs (in terms of your own voting power) from coalition: Your option Stay alone Join a coalition Have other voters formed coalitions? No Yes Moderate Very low High Low I Joining a coalition increases your voting power I But if all voters form a coalition, they all have low voting power I Suboptimal outcome if all players act rationally Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Coalition-formation as a “prisoner’s dilemma” Payoffs (in terms of your own voting power) from coalition: Your option Stay alone Join a coalition Have other voters formed coalitions? No Yes Moderate Very low High Low I Joining a coalition increases your voting power I But if all voters form a coalition, they all have low voting power I Suboptimal outcome if all players act rationally Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Coalition-formation as a “prisoner’s dilemma” Payoffs (in terms of your own voting power) from coalition: Your option Stay alone Join a coalition Have other voters formed coalitions? No Yes Moderate Very low High Low I Joining a coalition increases your voting power I But if all voters form a coalition, they all have low voting power I Suboptimal outcome if all players act rationally Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Voting power is not a zero-sum game! I I Consider 2 extremes Everyone votes I I I One voter is chosen at random and gets to decide the outcome I I I Pr (decisive vote) = Pr (election is tied) Assuming random voting, this probability is proportional to √ 1/ n Pr (decisive vote) = 1 for that person and 0 for all others Avg Pr (decisive vote) = 1/n But both systems are “fair”! Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Voting power is not a zero-sum game! I I Consider 2 extremes Everyone votes I I I One voter is chosen at random and gets to decide the outcome I I I Pr (decisive vote) = Pr (election is tied) Assuming random voting, this probability is proportional to √ 1/ n Pr (decisive vote) = 1 for that person and 0 for all others Avg Pr (decisive vote) = 1/n But both systems are “fair”! Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Voting power is not a zero-sum game! I I Consider 2 extremes Everyone votes I I I One voter is chosen at random and gets to decide the outcome I I I Pr (decisive vote) = Pr (election is tied) Assuming random voting, this probability is proportional to √ 1/ n Pr (decisive vote) = 1 for that person and 0 for all others Avg Pr (decisive vote) = 1/n But both systems are “fair”! Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Voting power is not a zero-sum game! I I Consider 2 extremes Everyone votes I I I One voter is chosen at random and gets to decide the outcome I I I Pr (decisive vote) = Pr (election is tied) Assuming random voting, this probability is proportional to √ 1/ n Pr (decisive vote) = 1 for that person and 0 for all others Avg Pr (decisive vote) = 1/n But both systems are “fair”! Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Voting power is not a zero-sum game! I I Consider 2 extremes Everyone votes I I I One voter is chosen at random and gets to decide the outcome I I I Pr (decisive vote) = Pr (election is tied) Assuming random voting, this probability is proportional to √ 1/ n Pr (decisive vote) = 1 for that person and 0 for all others Avg Pr (decisive vote) = 1/n But both systems are “fair”! Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Voting power is not a zero-sum game! I I Consider 2 extremes Everyone votes I I I One voter is chosen at random and gets to decide the outcome I I I Pr (decisive vote) = Pr (election is tied) Assuming random voting, this probability is proportional to √ 1/ n Pr (decisive vote) = 1 for that person and 0 for all others Avg Pr (decisive vote) = 1/n But both systems are “fair”! Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Voting power is not a zero-sum game! I I Consider 2 extremes Everyone votes I I I One voter is chosen at random and gets to decide the outcome I I I Pr (decisive vote) = Pr (election is tied) Assuming random voting, this probability is proportional to √ 1/ n Pr (decisive vote) = 1 for that person and 0 for all others Avg Pr (decisive vote) = 1/n But both systems are “fair”! Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Voting power is not a zero-sum game! I I Consider 2 extremes Everyone votes I I I One voter is chosen at random and gets to decide the outcome I I I Pr (decisive vote) = Pr (election is tied) Assuming random voting, this probability is proportional to √ 1/ n Pr (decisive vote) = 1 for that person and 0 for all others Avg Pr (decisive vote) = 1/n But both systems are “fair”! Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Voting power is not a zero-sum game! I I Consider 2 extremes Everyone votes I I I One voter is chosen at random and gets to decide the outcome I I I Pr (decisive vote) = Pr (election is tied) Assuming random voting, this probability is proportional to √ 1/ n Pr (decisive vote) = 1 for that person and 0 for all others Avg Pr (decisive vote) = 1/n But both systems are “fair”! Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems n=3 n=5 n=7 n=9 n = 11 n = 13 n = 17 n = 21 0.0 0.1 Pr (decisive vote) 0.2 0.3 0.4 0.5 Voting power if you are in a coalition of size m in an electorate of size n 0 5 10 15 coalition size, m Andrew Gelman 20 Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems n = 21 n = 31 n = 51 n = 101 n = 201 n = 501 n = 1001 0.0 Pr (decisive vote) 0.1 0.2 0.3 Voting power if you are in a coalition of size m in an electorate of size n (for larger populations) 0 200 400 600 coalition size, m Andrew Gelman 800 1000 Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Optimal coalition size m in an electorate of size n I I √ Using combinatorics, derive that optimal m is approx 1.4 n Optimal coalition sizes: I I I I I I n = 10 (faculty committee or student club): mopt = 4 n = 100 (U.S. Senate): mopt = 14 n = 435 (House of Representatives): mopt = 30 n = 5,000,000 (Pennsylvania): mopt = 3,000 n = 100,000,000 (United States): mopt = 14,000 Voting power in optimal coalition is approx 0.57n−1/4 (compared to 0.80n−1/2 if there is no coalition) Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Optimal coalition size m in an electorate of size n I I √ Using combinatorics, derive that optimal m is approx 1.4 n Optimal coalition sizes: I I I I I I n = 10 (faculty committee or student club): mopt = 4 n = 100 (U.S. Senate): mopt = 14 n = 435 (House of Representatives): mopt = 30 n = 5,000,000 (Pennsylvania): mopt = 3,000 n = 100,000,000 (United States): mopt = 14,000 Voting power in optimal coalition is approx 0.57n−1/4 (compared to 0.80n−1/2 if there is no coalition) Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Optimal coalition size m in an electorate of size n I I √ Using combinatorics, derive that optimal m is approx 1.4 n Optimal coalition sizes: I I I I I I n = 10 (faculty committee or student club): mopt = 4 n = 100 (U.S. Senate): mopt = 14 n = 435 (House of Representatives): mopt = 30 n = 5,000,000 (Pennsylvania): mopt = 3,000 n = 100,000,000 (United States): mopt = 14,000 Voting power in optimal coalition is approx 0.57n−1/4 (compared to 0.80n−1/2 if there is no coalition) Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Optimal coalition size m in an electorate of size n I I √ Using combinatorics, derive that optimal m is approx 1.4 n Optimal coalition sizes: I I I I I I n = 10 (faculty committee or student club): mopt = 4 n = 100 (U.S. Senate): mopt = 14 n = 435 (House of Representatives): mopt = 30 n = 5,000,000 (Pennsylvania): mopt = 3,000 n = 100,000,000 (United States): mopt = 14,000 Voting power in optimal coalition is approx 0.57n−1/4 (compared to 0.80n−1/2 if there is no coalition) Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Optimal coalition size m in an electorate of size n I I √ Using combinatorics, derive that optimal m is approx 1.4 n Optimal coalition sizes: I I I I I I n = 10 (faculty committee or student club): mopt = 4 n = 100 (U.S. Senate): mopt = 14 n = 435 (House of Representatives): mopt = 30 n = 5,000,000 (Pennsylvania): mopt = 3,000 n = 100,000,000 (United States): mopt = 14,000 Voting power in optimal coalition is approx 0.57n−1/4 (compared to 0.80n−1/2 if there is no coalition) Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Optimal coalition size m in an electorate of size n I I √ Using combinatorics, derive that optimal m is approx 1.4 n Optimal coalition sizes: I I I I I I n = 10 (faculty committee or student club): mopt = 4 n = 100 (U.S. Senate): mopt = 14 n = 435 (House of Representatives): mopt = 30 n = 5,000,000 (Pennsylvania): mopt = 3,000 n = 100,000,000 (United States): mopt = 14,000 Voting power in optimal coalition is approx 0.57n−1/4 (compared to 0.80n−1/2 if there is no coalition) Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Optimal coalition size m in an electorate of size n I I √ Using combinatorics, derive that optimal m is approx 1.4 n Optimal coalition sizes: I I I I I I n = 10 (faculty committee or student club): mopt = 4 n = 100 (U.S. Senate): mopt = 14 n = 435 (House of Representatives): mopt = 30 n = 5,000,000 (Pennsylvania): mopt = 3,000 n = 100,000,000 (United States): mopt = 14,000 Voting power in optimal coalition is approx 0.57n−1/4 (compared to 0.80n−1/2 if there is no coalition) Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Optimal coalition size m in an electorate of size n I I √ Using combinatorics, derive that optimal m is approx 1.4 n Optimal coalition sizes: I I I I I I n = 10 (faculty committee or student club): mopt = 4 n = 100 (U.S. Senate): mopt = 14 n = 435 (House of Representatives): mopt = 30 n = 5,000,000 (Pennsylvania): mopt = 3,000 n = 100,000,000 (United States): mopt = 14,000 Voting power in optimal coalition is approx 0.57n−1/4 (compared to 0.80n−1/2 if there is no coalition) Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Optimal coalition size m in an electorate of size n I I √ Using combinatorics, derive that optimal m is approx 1.4 n Optimal coalition sizes: I I I I I I n = 10 (faculty committee or student club): mopt = 4 n = 100 (U.S. Senate): mopt = 14 n = 435 (House of Representatives): mopt = 30 n = 5,000,000 (Pennsylvania): mopt = 3,000 n = 100,000,000 (United States): mopt = 14,000 Voting power in optimal coalition is approx 0.57n−1/4 (compared to 0.80n−1/2 if there is no coalition) Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems But . . . I Your voting power if there are no coalitions is 0.80n−1/2 I Your voting power if you’re in an optimal coalition is 0.57n−1/4 I But . . . your voting power if everyone divides into optimal coalitions is 0.65n−1/2 I Example of the prisoner’s dilemma of coalition formation Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems But . . . I Your voting power if there are no coalitions is 0.80n−1/2 I Your voting power if you’re in an optimal coalition is 0.57n−1/4 I But . . . your voting power if everyone divides into optimal coalitions is 0.65n−1/2 I Example of the prisoner’s dilemma of coalition formation Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems But . . . I Your voting power if there are no coalitions is 0.80n−1/2 I Your voting power if you’re in an optimal coalition is 0.57n−1/4 I But . . . your voting power if everyone divides into optimal coalitions is 0.65n−1/2 I Example of the prisoner’s dilemma of coalition formation Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems But . . . I Your voting power if there are no coalitions is 0.80n−1/2 I Your voting power if you’re in an optimal coalition is 0.57n−1/4 I But . . . your voting power if everyone divides into optimal coalitions is 0.65n−1/2 I Example of the prisoner’s dilemma of coalition formation Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems But . . . I Your voting power if there are no coalitions is 0.80n−1/2 I Your voting power if you’re in an optimal coalition is 0.57n−1/4 I But . . . your voting power if everyone divides into optimal coalitions is 0.65n−1/2 I Example of the prisoner’s dilemma of coalition formation Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Coalition-formation as a random walk in the space of trees I I Picture of a coalition structure as a tree Possible moves in tree-space: I I I I I Several voters forming a coalition A coalition disbanding or dividing into sub-coalitions A set of coalitions forming a super-coalition A set of coalitions merging into a single coalition Restrict to locally beneficial moves: Pr (decisive) must increase for all voters who are involved in the decision Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Coalition-formation as a random walk in the space of trees I I Picture of a coalition structure as a tree Possible moves in tree-space: I I I I I Several voters forming a coalition A coalition disbanding or dividing into sub-coalitions A set of coalitions forming a super-coalition A set of coalitions merging into a single coalition Restrict to locally beneficial moves: Pr (decisive) must increase for all voters who are involved in the decision Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Coalition-formation as a random walk in the space of trees I I Picture of a coalition structure as a tree Possible moves in tree-space: I I I I I Several voters forming a coalition A coalition disbanding or dividing into sub-coalitions A set of coalitions forming a super-coalition A set of coalitions merging into a single coalition Restrict to locally beneficial moves: Pr (decisive) must increase for all voters who are involved in the decision Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Coalition-formation as a random walk in the space of trees I I Picture of a coalition structure as a tree Possible moves in tree-space: I I I I I Several voters forming a coalition A coalition disbanding or dividing into sub-coalitions A set of coalitions forming a super-coalition A set of coalitions merging into a single coalition Restrict to locally beneficial moves: Pr (decisive) must increase for all voters who are involved in the decision Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Coalition-formation as a random walk in the space of trees I I Picture of a coalition structure as a tree Possible moves in tree-space: I I I I I Several voters forming a coalition A coalition disbanding or dividing into sub-coalitions A set of coalitions forming a super-coalition A set of coalitions merging into a single coalition Restrict to locally beneficial moves: Pr (decisive) must increase for all voters who are involved in the decision Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Coalition-formation as a random walk in the space of trees I I Picture of a coalition structure as a tree Possible moves in tree-space: I I I I I Several voters forming a coalition A coalition disbanding or dividing into sub-coalitions A set of coalitions forming a super-coalition A set of coalitions merging into a single coalition Restrict to locally beneficial moves: Pr (decisive) must increase for all voters who are involved in the decision Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Coalition-formation as a random walk in the space of trees I I Picture of a coalition structure as a tree Possible moves in tree-space: I I I I I Several voters forming a coalition A coalition disbanding or dividing into sub-coalitions A set of coalitions forming a super-coalition A set of coalitions merging into a single coalition Restrict to locally beneficial moves: Pr (decisive) must increase for all voters who are involved in the decision Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Coalition-formation as a random walk in the space of trees I I Picture of a coalition structure as a tree Possible moves in tree-space: I I I I I Several voters forming a coalition A coalition disbanding or dividing into sub-coalitions A set of coalitions forming a super-coalition A set of coalitions merging into a single coalition Restrict to locally beneficial moves: Pr (decisive) must increase for all voters who are involved in the decision Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems A potential explanation for political instability I Locally beneficial moves are nontransitive I Similar to cartels in economics I How easily can an individual voter compute ∆ Pr (decisive), in order to decide whether a particular move is a good idea? I Approximate calculations (similar to “expected utility” calculations for economic actors) I Also, as with economics, can imagine reaching a global optimum using side payments Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems A potential explanation for political instability I Locally beneficial moves are nontransitive I Similar to cartels in economics I How easily can an individual voter compute ∆ Pr (decisive), in order to decide whether a particular move is a good idea? I Approximate calculations (similar to “expected utility” calculations for economic actors) I Also, as with economics, can imagine reaching a global optimum using side payments Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems A potential explanation for political instability I Locally beneficial moves are nontransitive I Similar to cartels in economics I How easily can an individual voter compute ∆ Pr (decisive), in order to decide whether a particular move is a good idea? I Approximate calculations (similar to “expected utility” calculations for economic actors) I Also, as with economics, can imagine reaching a global optimum using side payments Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems A potential explanation for political instability I Locally beneficial moves are nontransitive I Similar to cartels in economics I How easily can an individual voter compute ∆ Pr (decisive), in order to decide whether a particular move is a good idea? I Approximate calculations (similar to “expected utility” calculations for economic actors) I Also, as with economics, can imagine reaching a global optimum using side payments Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems A potential explanation for political instability I Locally beneficial moves are nontransitive I Similar to cartels in economics I How easily can an individual voter compute ∆ Pr (decisive), in order to decide whether a particular move is a good idea? I Approximate calculations (similar to “expected utility” calculations for economic actors) I Also, as with economics, can imagine reaching a global optimum using side payments Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems A potential explanation for political instability I Locally beneficial moves are nontransitive I Similar to cartels in economics I How easily can an individual voter compute ∆ Pr (decisive), in order to decide whether a particular move is a good idea? I Approximate calculations (similar to “expected utility” calculations for economic actors) I Also, as with economics, can imagine reaching a global optimum using side payments Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Open problems I Conjecture: the coalition-formation process is inherently unstable for n > 3 I Local calculations of changes in voting power Generalizing the model: I I I I I I Weighted voting Network structure of voters Unequal probabilities pi for individual voters Different preferences for different issues Fitting to real data (legislative committees, courts, political parties, . . . ) Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Open problems I Conjecture: the coalition-formation process is inherently unstable for n > 3 I Local calculations of changes in voting power Generalizing the model: I I I I I I Weighted voting Network structure of voters Unequal probabilities pi for individual voters Different preferences for different issues Fitting to real data (legislative committees, courts, political parties, . . . ) Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Open problems I Conjecture: the coalition-formation process is inherently unstable for n > 3 I Local calculations of changes in voting power Generalizing the model: I I I I I I Weighted voting Network structure of voters Unequal probabilities pi for individual voters Different preferences for different issues Fitting to real data (legislative committees, courts, political parties, . . . ) Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Open problems I Conjecture: the coalition-formation process is inherently unstable for n > 3 I Local calculations of changes in voting power Generalizing the model: I I I I I I Weighted voting Network structure of voters Unequal probabilities pi for individual voters Different preferences for different issues Fitting to real data (legislative committees, courts, political parties, . . . ) Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Open problems I Conjecture: the coalition-formation process is inherently unstable for n > 3 I Local calculations of changes in voting power Generalizing the model: I I I I I I Weighted voting Network structure of voters Unequal probabilities pi for individual voters Different preferences for different issues Fitting to real data (legislative committees, courts, political parties, . . . ) Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Open problems I Conjecture: the coalition-formation process is inherently unstable for n > 3 I Local calculations of changes in voting power Generalizing the model: I I I I I I Weighted voting Network structure of voters Unequal probabilities pi for individual voters Different preferences for different issues Fitting to real data (legislative committees, courts, political parties, . . . ) Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Open problems I Conjecture: the coalition-formation process is inherently unstable for n > 3 I Local calculations of changes in voting power Generalizing the model: I I I I I I Weighted voting Network structure of voters Unequal probabilities pi for individual voters Different preferences for different issues Fitting to real data (legislative committees, courts, political parties, . . . ) Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Open problems I Conjecture: the coalition-formation process is inherently unstable for n > 3 I Local calculations of changes in voting power Generalizing the model: I I I I I I Weighted voting Network structure of voters Unequal probabilities pi for individual voters Different preferences for different issues Fitting to real data (legislative committees, courts, political parties, . . . ) Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Coalitions and voting power Optimal coalition sizes Political instability Open problems Open problems I Conjecture: the coalition-formation process is inherently unstable for n > 3 I Local calculations of changes in voting power Generalizing the model: I I I I I I Weighted voting Network structure of voters Unequal probabilities pi for individual voters Different preferences for different issues Fitting to real data (legislative committees, courts, political parties, . . . ) Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Mathematical and statistical models of voting power Second part of the talk Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Voting power in a 2-level electoral system I I U.S. Electoral College, or E.U. Council of Ministers Electoral college: I I I nj voters in state j ej electoral votes contribute to U.S. total Your vote is decisive if: I I Your state is tied, and Your state’s electoral votes are decisive, if your state is tied Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Voting power in a 2-level electoral system I I U.S. Electoral College, or E.U. Council of Ministers Electoral college: I I I nj voters in state j ej electoral votes contribute to U.S. total Your vote is decisive if: I I Your state is tied, and Your state’s electoral votes are decisive, if your state is tied Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Voting power in a 2-level electoral system I I U.S. Electoral College, or E.U. Council of Ministers Electoral college: I I I nj voters in state j ej electoral votes contribute to U.S. total Your vote is decisive if: I I Your state is tied, and Your state’s electoral votes are decisive, if your state is tied Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Voting power in a 2-level electoral system I I U.S. Electoral College, or E.U. Council of Ministers Electoral college: I I I nj voters in state j ej electoral votes contribute to U.S. total Your vote is decisive if: I I Your state is tied, and Your state’s electoral votes are decisive, if your state is tied Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Voting power in a 2-level electoral system I I U.S. Electoral College, or E.U. Council of Ministers Electoral college: I I I nj voters in state j ej electoral votes contribute to U.S. total Your vote is decisive if: I I Your state is tied, and Your state’s electoral votes are decisive, if your state is tied Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Voting power in a 2-level electoral system I I U.S. Electoral College, or E.U. Council of Ministers Electoral college: I I I nj voters in state j ej electoral votes contribute to U.S. total Your vote is decisive if: I I Your state is tied, and Your state’s electoral votes are decisive, if your state is tied Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Voting power in a 2-level electoral system I I U.S. Electoral College, or E.U. Council of Ministers Electoral college: I I I nj voters in state j ej electoral votes contribute to U.S. total Your vote is decisive if: I I Your state is tied, and Your state’s electoral votes are decisive, if your state is tied Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Voting power in a 2-level electoral system I I U.S. Electoral College, or E.U. Council of Ministers Electoral college: I I I nj voters in state j ej electoral votes contribute to U.S. total Your vote is decisive if: I I Your state is tied, and Your state’s electoral votes are decisive, if your state is tied Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Your voting power in a presidential election I Voting power = Pr (your vote is decisive): I I I Pr (your state is tied) × Pr (your state’s electoral votes are decisive, if your state is tied) Simple calculation based on random voting model: I I √ Pr (your state is tied) ∝ 1/ nj Pr (your state’s electoral votes are decisive) ∝ ej I √ Combining: voting power ∝ ej / nj I According to this model, higher voting power in large states Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Your voting power in a presidential election I Voting power = Pr (your vote is decisive): I I I Pr (your state is tied) × Pr (your state’s electoral votes are decisive, if your state is tied) Simple calculation based on random voting model: I I √ Pr (your state is tied) ∝ 1/ nj Pr (your state’s electoral votes are decisive) ∝ ej I √ Combining: voting power ∝ ej / nj I According to this model, higher voting power in large states Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Your voting power in a presidential election I Voting power = Pr (your vote is decisive): I I I Pr (your state is tied) × Pr (your state’s electoral votes are decisive, if your state is tied) Simple calculation based on random voting model: I I √ Pr (your state is tied) ∝ 1/ nj Pr (your state’s electoral votes are decisive) ∝ ej I √ Combining: voting power ∝ ej / nj I According to this model, higher voting power in large states Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Your voting power in a presidential election I Voting power = Pr (your vote is decisive): I I I Pr (your state is tied) × Pr (your state’s electoral votes are decisive, if your state is tied) Simple calculation based on random voting model: I I √ Pr (your state is tied) ∝ 1/ nj Pr (your state’s electoral votes are decisive) ∝ ej I √ Combining: voting power ∝ ej / nj I According to this model, higher voting power in large states Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Your voting power in a presidential election I Voting power = Pr (your vote is decisive): I I I Pr (your state is tied) × Pr (your state’s electoral votes are decisive, if your state is tied) Simple calculation based on random voting model: I I √ Pr (your state is tied) ∝ 1/ nj Pr (your state’s electoral votes are decisive) ∝ ej I √ Combining: voting power ∝ ej / nj I According to this model, higher voting power in large states Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Your voting power in a presidential election I Voting power = Pr (your vote is decisive): I I I Pr (your state is tied) × Pr (your state’s electoral votes are decisive, if your state is tied) Simple calculation based on random voting model: I I √ Pr (your state is tied) ∝ 1/ nj Pr (your state’s electoral votes are decisive) ∝ ej I √ Combining: voting power ∝ ej / nj I According to this model, higher voting power in large states Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Your voting power in a presidential election I Voting power = Pr (your vote is decisive): I I I Pr (your state is tied) × Pr (your state’s electoral votes are decisive, if your state is tied) Simple calculation based on random voting model: I I √ Pr (your state is tied) ∝ 1/ nj Pr (your state’s electoral votes are decisive) ∝ ej I √ Combining: voting power ∝ ej / nj I According to this model, higher voting power in large states Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Your voting power in a presidential election I Voting power = Pr (your vote is decisive): I I I Pr (your state is tied) × Pr (your state’s electoral votes are decisive, if your state is tied) Simple calculation based on random voting model: I I √ Pr (your state is tied) ∝ 1/ nj Pr (your state’s electoral votes are decisive) ∝ ej I √ Combining: voting power ∝ ej / nj I According to this model, higher voting power in large states Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Your voting power in a presidential election I Voting power = Pr (your vote is decisive): I I I Pr (your state is tied) × Pr (your state’s electoral votes are decisive, if your state is tied) Simple calculation based on random voting model: I I √ Pr (your state is tied) ∝ 1/ nj Pr (your state’s electoral votes are decisive) ∝ ej I √ Combining: voting power ∝ ej / nj I According to this model, higher voting power in large states Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Random voting model I I I I Voters are flipping coins √ Implies that voting power ∝ ej / nj Focus on voting power as a function of nj Key prediction of random voting model: I I Large elections should be much closer (in percentage terms) than small elections “Law of large numbers” I Classical voting power calculations can also be defined combinatorially (Mathematically, same as the random voting model) I But does the model describe reality? Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Random voting model I I I I Voters are flipping coins √ Implies that voting power ∝ ej / nj Focus on voting power as a function of nj Key prediction of random voting model: I I Large elections should be much closer (in percentage terms) than small elections “Law of large numbers” I Classical voting power calculations can also be defined combinatorially (Mathematically, same as the random voting model) I But does the model describe reality? Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Random voting model I I I I Voters are flipping coins √ Implies that voting power ∝ ej / nj Focus on voting power as a function of nj Key prediction of random voting model: I I Large elections should be much closer (in percentage terms) than small elections “Law of large numbers” I Classical voting power calculations can also be defined combinatorially (Mathematically, same as the random voting model) I But does the model describe reality? Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Random voting model I I I I Voters are flipping coins √ Implies that voting power ∝ ej / nj Focus on voting power as a function of nj Key prediction of random voting model: I I Large elections should be much closer (in percentage terms) than small elections “Law of large numbers” I Classical voting power calculations can also be defined combinatorially (Mathematically, same as the random voting model) I But does the model describe reality? Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Random voting model I I I I Voters are flipping coins √ Implies that voting power ∝ ej / nj Focus on voting power as a function of nj Key prediction of random voting model: I I Large elections should be much closer (in percentage terms) than small elections “Law of large numbers” I Classical voting power calculations can also be defined combinatorially (Mathematically, same as the random voting model) I But does the model describe reality? Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Random voting model I I I I Voters are flipping coins √ Implies that voting power ∝ ej / nj Focus on voting power as a function of nj Key prediction of random voting model: I I Large elections should be much closer (in percentage terms) than small elections “Law of large numbers” I Classical voting power calculations can also be defined combinatorially (Mathematically, same as the random voting model) I But does the model describe reality? Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Random voting model I I I I Voters are flipping coins √ Implies that voting power ∝ ej / nj Focus on voting power as a function of nj Key prediction of random voting model: I I Large elections should be much closer (in percentage terms) than small elections “Law of large numbers” I Classical voting power calculations can also be defined combinatorially (Mathematically, same as the random voting model) I But does the model describe reality? Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Random voting model I I I I Voters are flipping coins √ Implies that voting power ∝ ej / nj Focus on voting power as a function of nj Key prediction of random voting model: I I Large elections should be much closer (in percentage terms) than small elections “Law of large numbers” I Classical voting power calculations can also be defined combinatorially (Mathematically, same as the random voting model) I But does the model describe reality? Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Random voting model I I I I Voters are flipping coins √ Implies that voting power ∝ ej / nj Focus on voting power as a function of nj Key prediction of random voting model: I I Large elections should be much closer (in percentage terms) than small elections “Law of large numbers” I Classical voting power calculations can also be defined combinatorially (Mathematically, same as the random voting model) I But does the model describe reality? Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems 0.0 Proportional vote differential 0.2 0.4 0.6 0.8 Checking the random voting model . . . . . . . .. . . .. . . ... . ... . ... .. .. . . .. . . . . ..... .. . . . . . . . . . .. ... . . . . . .... . . . . . . . . . . .... . .. .... . . . . . . ........... . .. . .. . . . ... . . . ............ ... .. ... .. .. . . . . . . . . . . . . . . . . . . . ..... . .. .. . .. . .. . . .. . . . . .... . . . .. . .... . . . . . .. . . . . . ... . . .......... .. ......... .... . . .... . . . . . . . ...... . .. ....... . .. . . . . . . . .. .... . .. .. .... . . . . .. . . . .... .. . ..... .... ..... . ... . . . . . . .. . .. . . ... ... .. ... .. . . . .. . ............ . ....... ... . ... .. .. . . .. .. . ............. ... .......... ........... . ... . .. .. . . . .. .. .... . . . .. . . . . . .. . . . 0 . . . . . . . . lowess fit alpha = -0.16 alpha = -0.5 2*10^6 6*10^6 10^7 Total vote for the two leading candidates Andrew Gelman Coalitions, voting power, and political instability Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Coalitions and political instability Mathematical and statistical models of voting power Conclusions More checks of the random voting model . . . . . alpha = -0.23 lowess fit alpha = -0.5 0 4*10^6 8*10^6 1.2*10^7 Total vote for the two leading candidates Proportional vote differential 0.2 0.4 0.6 0.8 . . . . .. . . .. ... . . ... . . . . .. . . . .... ..... . .. . . . . . . . . .. ... . . .... . .. . . . . ... . . .. . .. .. . .. . . . .. . . . .. .... . .. . . . . .. .. . . . . . . . ....... .. ... . . .. .. . . . .... . . ..... . . . .. . .. . .. . . ... . . .... . .. . . . . ... ... . 0.0 Proportional vote differential 0.2 0.4 0.6 0.8 0.0 . .. .. lowess fit . 0.0 alpha = -0.5 Proportional vote differential 0.2 0.4 0.6 0.8 alpha = 0.06 ........... .. . .. .. . . . . ............... ........................................ ... ......... ... .. . . . .................................. ..... .. . . .... . ......... ... ............... . .. .. . ...................... ............. ........................................... ..... .... .. .. . .. .. . . ................. ........................... ..... ... .. . . .. . . . .......................................................................................... ............ . . . . ........................................................... .. . .. .. .. . . .................................................................................................................................. ... . . . . . . . . . . ................... .... ....... ........... .................. .. . .............................................. ................ ......................... ...... .. .. . . ........................................................................................................................................................................... . . .................. .... . . .................................................................................................................................. .. . ....... . . ............ . . ..................... .. ............................................................................................................................................................................................................. .. . . ................................................................................................................................................................................................. ...... . ... .............. ... ... .. ... ............................................................................................................................ ................................................................................. ............................................................................. . .... .... .. . . .......................................................................................................................................... .................................................................... . .............................. . . . . ................................... .............................................................................................................................................................. .... ... .. . .. ............................................................................................................... .................................................................. . . .. . ............... ............................................................................................................................................................................. ................. . ............ .. .. ....................................... . ...................... .................................................................................................. .... . . ................................................. ......... . .................................................................................................... .............................................................................................................................. .... .. . .......... . . . . ......................... ............................................................... ........................................................................................................................................................................................................................................................................... ....... .. . .. . ................................................................................................................................................................. .......... .. .. .................................................................................................................................... .. . . ............................................... .. .. . . .. .... . .... ....... . .. .. . . .......................................................................................................................... . . .. .. ....................................................................................... ....................... .... .................................... ................... ......................................... .... ......... .................. ......................... . ...... ... .. .. .. . ....... .............. .............................................................. ........................................................................................................................ ......... ... ... . ..................... .......... ............................. ... .. . . .. . ....................................................... .................................................. .......... .................................................... ..................................................................................... . ... ..... ..... ........... ................... .. ................................................................................................................................................... ..... . . ....... lowess fit alpha = -0.11 . . alpha = -0.5 . 0 50000 150000 250000 Total vote for the two leading candidates 0 200000 400000 600000 Total vote for the two leading candidates U.S. statewide offices European national elections U.S. Senate elections . . . . U.S. Congressional elections . . . . . .. . . .. . .. . . . . . .. . . ... . .. .. . ... .. . .... . . ... ... . . . .. . . . . .. . . . . . . ... ..... ........ ... ... . . ..... . .. .. ... . . . .. .. ..... .. ....... .. . .... .. .. .... . .. . . . . .. . . . ......... .......... . .. .. .. . .. ... . . . . . . ...... . . . . . alpha = -0.01 . . lowess fit = -0.5 Proportional vote differential 0.2 0.4 0.6 0.8 0 20000 60000 100000 Total vote for the two leading candidates . . . .. . .. . ... ..... . . . .. . . . .. .. . .... . .. . . . . . . ......... . .. . .. . .. ......... . .... . . . ....... ...... ... .. ... .. .... .. . .. .... .. . . . . . . . . . ... . . . . .............. .... .. ... . .... . ........... ... ..... . ......... ...... . .. . . . . . . . .. . . ..... .. . ...... .... . . ....... ...... . ..... . . . .. . .. . . . . .. .................. .. ... . . ............................................... .... .... . .. . . . .... ... . . ........... ... .. ... ... . .. .... . . . . . ......... ............. .. .... . . . .. . .. .. . ................... ..... .. ..... . .... .. ... . . ...... . .............................................................. .......... ......... .. . .......... ..... .................................... . .... .... ... . . . . . .................................. .. . ... . . .. .... ..... .. ... .. . . . . . .. . .. ........................................................ ..... ........... .. ... ..... ... ....... . . .................................. ....... .. . ..... .. . . . ............................... . ... ........ . . .. ...... . .............................................. ... .... ...... .. . . .. . . . . ......................................................................... .......... .. . . .. . .. . .. . . . . . . . . . . . . . . . ................... .......... .. .. ..... . . .. . . . ......................... .................................................. .. ... ...... .... .. . . .. . . .... .. . ..... ............ . ... . . . . .. . . . . ..................................... . ..... . . . . .................................................. ... . ........ .. .. .. .. . . ... . . ................... . . .. ...................................... .. ... . ... .. . . . .. .......................................................................... ......... ........... . ... . . .. . . .. . .. . . ................................ . . . alpha 0 4*10^6 8*10^6 1.4*10^7 Total vote for the two leading candidates Andrew Gelman 0.0 Proportional vote differential 0.2 0.4 0.6 0.8 U.S. state senate elections 0.0 0.0 Proportional vote differential 0.2 0.4 0.6 0.8 U.S. state house elections . ... .... . .. .. .. . . .. .. . . ... . .. . .. . . . .... ............ .... ........... . .. . .... . . . . . . .. . . . . .. .... . .. .... . . .... . . . ..... ... ... ......... ................. ... . .. .. . .. . .. . ...... ..... .... .. ............. ..... .. ..... . . .. . . .. .. . ... . ... .. . . ....................................... ...................... ... . . .. .. . .. . . . . . ................................................ .. ... .... .. . . .. .. .. .. . . .. .. .. .................. ..................... .... ... . .................. .................... . ........................ .... .. . . .... .. . . . . ........................................................................................................................... ..... ... .. . . ...... . . .......................................................... .... .............. ............... ....... .. ... . . . . . . . . .................................................................................................. ............ ............. .............. .... ..... . ................................................................................... ...... .......... ...... ........... .. . . . . . . . . ............................................................. . . . . . . . . . . . . . . . . . . . . . . . . .. .. . . . . . .. . . . . ........................................................... . ..................... .. . . . . . . ................................................................................................................................................................ ....................... ........... ....... . . . ........................................................................................................................................ ............. . ....... . ............................................................................................................. ............... . . . . ..................................... ................................................. ............... . . . .. .. .................................................................................................................. alpha = 0.08 .............................................................................................................................................................. ..... ........... ........... .. . . . ...................................................... ............. . . . ................................... . . . . .. ........ . ... ... .. ............ .. .... . ... . . . . . . .. ................................................................................................................................................................................................. ............. ... . . .. . . . . . . ...... .. .. . . lowess fit . ............................................................................................................................................................................ ............... .. .. ..... . . . . . . ............................ . . . . . . . . . . . . . . . . .. . . ..................................................... .. . ............................................... ................ ....... ... ... .... . . . ............................................................................................................................................................................. . .. . ... . .. ....................... ..................... .......................................................................... .... .. . ...... ..... .. . .. . . .......... ....... ... .... ........ ... ..... . .... ... . ............................................................. .. .. .................................... ..................................................................................................................... ............... . . ..... .... . . . . . alpha = -0.5 ................................................. ................. ................................................................................................................. .... . .. .. ..... . . . . . . . . . . . . .. . . . . . . . . . . . . ....................................................................................... ..... ... ... ............. . . . .... .. . . .. ................ .......... .. .... .... . . .. . . .. ....... . . .. .... . . . .. . .... . . . . ... .. . . .. . .. ... .. ... . . .. .. .... .. .... . .. ..... .. . . . . . .... ..... .. ... .. ....... ... . . . . ....... .. ....... .. ....... .... .. . .. . ..... ..... . . . . . . . . . . . . .. . . .. . . . . . . .. . .. . . .. . . alpha = -0.07 . . . .. . .. . .. . . .. .. lowess fit . .. . .. . . . alpha = -0.5 0 10^7 3*10^7 Total vote for the two leading candidates Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Voting power by state, 2000 (math and stat models) empirical model Pr (individual voter is decisive) 0.00004 0.00008 0.00012 random voting model CA Pr (individual voter is decisive) 4*10^-8 10^-7 NY TX PA FL OHIL MI WV AR AZ VTNV NH IA ME DE 0 10 20 30 40 Number of electoral votes for the state 50 OH TN OR FL PA MO WI MI MN LA WA VA CO HI SD GA NC MS SC KYAL ND AK MT IL CA IN NJ CT MD WYRI KS OK NE ID DC UT 0 0.0 NJ NC INGA VA TN MA MD MO OKAL MS DC WI AZLA WA CT AKRINM SC WY KY MN HIWV ARIACO NE OR VTIDUTKS ND NH SD DE NV ME MT NM 0 MA TXNY 10 20 30 40 Number of electoral votes for the state Voters in large states do not have an electoral college advantage! Andrew Gelman Coalitions, voting power, and political instability 50 Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems More realistic models using forecasting I A voter in Ohio or Florida has more voting power (is more likely to cast a decisive vote) than a voter in Utah or Texas I Estimate Pr (decisive vote) in each state and each year using hierarchical time-series cross-sectional forecasting model I Empirical comparisons of voting power in large and small states Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems More realistic models using forecasting I A voter in Ohio or Florida has more voting power (is more likely to cast a decisive vote) than a voter in Utah or Texas I Estimate Pr (decisive vote) in each state and each year using hierarchical time-series cross-sectional forecasting model I Empirical comparisons of voting power in large and small states Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems More realistic models using forecasting I A voter in Ohio or Florida has more voting power (is more likely to cast a decisive vote) than a voter in Utah or Texas I Estimate Pr (decisive vote) in each state and each year using hierarchical time-series cross-sectional forecasting model I Empirical comparisons of voting power in large and small states Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems More realistic models using forecasting I A voter in Ohio or Florida has more voting power (is more likely to cast a decisive vote) than a voter in Utah or Texas I Estimate Pr (decisive vote) in each state and each year using hierarchical time-series cross-sectional forecasting model I Empirical comparisons of voting power in large and small states Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems More realistic probability models I Simplest model: votes are independent with probability p instead of 1/2 I I This model is useless: it still predicts a standard deviation that is tiny when n is large We must take the next step and allow votes to be correlated I Probability models on trees (voters within neighborhoods within cities within states within regions within a country) I Two tree models: Ising model and latent Gaussian model Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems More realistic probability models I Simplest model: votes are independent with probability p instead of 1/2 I I This model is useless: it still predicts a standard deviation that is tiny when n is large We must take the next step and allow votes to be correlated I Probability models on trees (voters within neighborhoods within cities within states within regions within a country) I Two tree models: Ising model and latent Gaussian model Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems More realistic probability models I Simplest model: votes are independent with probability p instead of 1/2 I I This model is useless: it still predicts a standard deviation that is tiny when n is large We must take the next step and allow votes to be correlated I Probability models on trees (voters within neighborhoods within cities within states within regions within a country) I Two tree models: Ising model and latent Gaussian model Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems More realistic probability models I Simplest model: votes are independent with probability p instead of 1/2 I I This model is useless: it still predicts a standard deviation that is tiny when n is large We must take the next step and allow votes to be correlated I Probability models on trees (voters within neighborhoods within cities within states within regions within a country) I Two tree models: Ising model and latent Gaussian model Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems More realistic probability models I Simplest model: votes are independent with probability p instead of 1/2 I I This model is useless: it still predicts a standard deviation that is tiny when n is large We must take the next step and allow votes to be correlated I Probability models on trees (voters within neighborhoods within cities within states within regions within a country) I Two tree models: Ising model and latent Gaussian model Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems More realistic probability models I Simplest model: votes are independent with probability p instead of 1/2 I I This model is useless: it still predicts a standard deviation that is tiny when n is large We must take the next step and allow votes to be correlated I Probability models on trees (voters within neighborhoods within cities within states within regions within a country) I Two tree models: Ising model and latent Gaussian model Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Ising model on a tree of voters I Put a 1 or −1 at each node of the tree; correlations along branches I Look at the implied probability distribution for V n , the average of n voters I Standard deviation of V n has the form cn−α I Random voting model implies α = 0.5; actual data fit α = 0.1 Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Ising model on a tree of voters I Put a 1 or −1 at each node of the tree; correlations along branches I Look at the implied probability distribution for V n , the average of n voters I Standard deviation of V n has the form cn−α I Random voting model implies α = 0.5; actual data fit α = 0.1 Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Ising model on a tree of voters I Put a 1 or −1 at each node of the tree; correlations along branches I Look at the implied probability distribution for V n , the average of n voters I Standard deviation of V n has the form cn−α I Random voting model implies α = 0.5; actual data fit α = 0.1 Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Ising model on a tree of voters I Put a 1 or −1 at each node of the tree; correlations along branches I Look at the implied probability distribution for V n , the average of n voters I Standard deviation of V n has the form cn−α I Random voting model implies α = 0.5; actual data fit α = 0.1 Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Ising model on a tree of voters I Put a 1 or −1 at each node of the tree; correlations along branches I Look at the implied probability distribution for V n , the average of n voters I Standard deviation of V n has the form cn−α I Random voting model implies α = 0.5; actual data fit α = 0.1 Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems 0.0 Proportional vote differential 0.2 0.4 0.6 0.8 Estimating the parameter α . . . . . . . .. . . .. . . ... . ... . ... .. .. . . .. . . . . ..... .. . . . . . . . . . .. ... . . . . . .... . . . . . . . . . . .... . .. .... . . . . . . ........... . .. . .. . . . ... . . . ............ ... .. ... .. .. . . . . . . . . . . . . . . . . . . . ..... . .. .. . .. . .. . . .. . . . . .... . . . .. . .... . . . . . .. . . . . . ... . . .......... .. ......... .... . . .... . . . . . . . ...... . .. ....... . .. . . . . . . . .. .... . .. .. .... . . . . .. . . . .... .. . ..... .... ..... . ... . . . . . . .. . .. . . ... ... .. ... .. . . . .. . ............ . ....... ... . ... .. .. . . .. .. . ............. ... .......... ........... . ... . .. .. . . . .. .. .... . . . .. . . . . . .. . . . 0 . . . . . . . . lowess fit alpha = -0.16 alpha = -0.5 2*10^6 6*10^6 10^7 Total vote for the two leading candidates Andrew Gelman Coalitions, voting power, and political instability Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Coalitions and political instability Mathematical and statistical models of voting power Conclusions Estimating the parameter α . . . . . alpha = -0.23 lowess fit alpha = -0.5 0 4*10^6 8*10^6 1.2*10^7 Total vote for the two leading candidates Proportional vote differential 0.2 0.4 0.6 0.8 . . . . .. . . .. ... . . ... . . . . .. . . . .... ..... . .. . . . . . . . . .. ... . . .... . .. . . . . ... . . .. . .. .. . .. . . . .. . . . .. .... . .. . . . . .. .. . . . . . . . ....... .. ... . . .. .. . . . .... . . ..... . . . .. . .. . .. . . ... . . .... . .. . . . . ... ... . 0.0 Proportional vote differential 0.2 0.4 0.6 0.8 0.0 . .. .. lowess fit . 0.0 alpha = -0.5 Proportional vote differential 0.2 0.4 0.6 0.8 alpha = 0.06 ........... .. . .. .. . . . . ............... ........................................ ... ......... ... .. . . . .................................. ..... .. . . .... . ......... ... ............... . .. .. . ...................... ............. ........................................... ..... .... .. .. . .. .. . . ................. ........................... ..... ... .. . . .. . . . .......................................................................................... ............ . . . . ........................................................... .. . .. .. .. . . .................................................................................................................................. ... . . . . . . . . . . ................... .... ....... ........... .................. .. . .............................................. ................ ......................... ...... .. .. . . ........................................................................................................................................................................... . . .................. .... . . .................................................................................................................................. .. . ....... . . ............ . . ..................... .. ............................................................................................................................................................................................................. .. . . ................................................................................................................................................................................................. ...... . ... .............. ... ... .. ... ............................................................................................................................ ................................................................................. ............................................................................. . .... .... .. . . .......................................................................................................................................... .................................................................... . .............................. . . . . ................................... .............................................................................................................................................................. .... ... .. . .. ............................................................................................................... .................................................................. . . .. . ............... ............................................................................................................................................................................. ................. . ............ .. .. ....................................... . ...................... .................................................................................................. .... . . ................................................. ......... . .................................................................................................... .............................................................................................................................. .... .. . .......... . . . . ......................... ............................................................... ........................................................................................................................................................................................................................................................................... ....... .. . .. . ................................................................................................................................................................. .......... .. .. .................................................................................................................................... .. . . ............................................... .. .. . . .. .... . .... ....... . .. .. . . .......................................................................................................................... . . .. .. ....................................................................................... ....................... .... .................................... ................... ......................................... .... ......... .................. ......................... . ...... ... .. .. .. . ....... .............. .............................................................. ........................................................................................................................ ......... ... ... . ..................... .......... ............................. ... .. . . .. . ....................................................... .................................................. .......... .................................................... ..................................................................................... . ... ..... ..... ........... ................... .. ................................................................................................................................................... ..... . . ....... lowess fit alpha = -0.11 . . alpha = -0.5 . 0 50000 150000 250000 Total vote for the two leading candidates 0 200000 400000 600000 Total vote for the two leading candidates U.S. statewide offices European national elections U.S. Senate elections . . . . U.S. Congressional elections . . . . . .. . . .. . .. . . . . . .. . . ... . .. .. . ... .. . .... . . ... ... . . . .. . . . . .. . . . . . . ... ..... ........ ... ... . . ..... . .. .. ... . . . .. .. ..... .. ....... .. . .... .. .. .... . .. . . . . .. . . . ......... .......... . .. .. .. . .. ... . . . . . . ...... . . . . . alpha = -0.01 . . lowess fit = -0.5 Proportional vote differential 0.2 0.4 0.6 0.8 0 20000 60000 100000 Total vote for the two leading candidates . . . .. . .. . ... ..... . . . .. . . . .. .. . .... . .. . . . . . . ......... . .. . .. . .. ......... . .... . . . ....... ...... ... .. ... .. .... .. . .. .... .. . . . . . . . . . ... . . . . .............. .... .. ... . .... . ........... ... ..... . ......... ...... . .. . . . . . . . .. . . ..... .. . ...... .... . . ....... ...... . ..... . . . .. . .. . . . . .. .................. .. ... . . ............................................... .... .... . .. . . . .... ... . . ........... ... .. ... ... . .. .... . . . . . ......... ............. .. .... . . . .. . .. .. . ................... ..... .. ..... . .... .. ... . . ...... . .............................................................. .......... ......... .. . .......... ..... .................................... . .... .... ... . . . . . .................................. .. . ... . . .. .... ..... .. ... .. . . . . . .. . .. ........................................................ ..... ........... .. ... ..... ... ....... . . .................................. ....... .. . ..... .. . . . ............................... . ... ........ . . .. ...... . .............................................. ... .... ...... .. . . .. . . . . ......................................................................... .......... .. . . .. . .. . .. . . . . . . . . . . . . . . . ................... .......... .. .. ..... . . .. . . . ......................... .................................................. .. ... ...... .... .. . . .. . . .... .. . ..... ............ . ... . . . . .. . . . . ..................................... . ..... . . . . .................................................. ... . ........ .. .. .. .. . . ... . . ................... . . .. ...................................... .. ... . ... .. . . . .. .......................................................................... ......... ........... . ... . . .. . . .. . .. . . ................................ . . . alpha 0 4*10^6 8*10^6 1.4*10^7 Total vote for the two leading candidates Andrew Gelman 0.0 Proportional vote differential 0.2 0.4 0.6 0.8 U.S. state senate elections 0.0 0.0 Proportional vote differential 0.2 0.4 0.6 0.8 U.S. state house elections . ... .... . .. .. .. . . .. .. . . ... . .. . .. . . . .... ............ .... ........... . .. . .... . . . . . . .. . . . . .. .... . .. .... . . .... . . . ..... ... ... ......... ................. ... . .. .. . .. . .. . ...... ..... .... .. ............. ..... .. ..... . . .. . . .. .. . ... . ... .. . . ....................................... ...................... ... . . .. .. . .. . . . . . ................................................ .. ... .... .. . . .. .. .. .. . . .. .. .. .................. ..................... .... ... . .................. .................... . ........................ .... .. . . .... .. . . . . ........................................................................................................................... ..... ... .. . . ...... . . .......................................................... .... .............. ............... ....... .. ... . . . . . . . . .................................................................................................. ............ ............. .............. .... ..... . ................................................................................... ...... .......... ...... ........... .. . . . . . . . . ............................................................. . . . . . . . . . . . . . . . . . . . . . . . . .. .. . . . . . .. . . . . ........................................................... . ..................... .. . . . . . . ................................................................................................................................................................ ....................... ........... ....... . . . ........................................................................................................................................ ............. . ....... . ............................................................................................................. ............... . . . . ..................................... ................................................. ............... . . . .. .. .................................................................................................................. alpha = 0.08 .............................................................................................................................................................. ..... ........... ........... .. . . . ...................................................... ............. . . . ................................... . . . . .. ........ . ... ... .. ............ .. .... . ... . . . . . . .. ................................................................................................................................................................................................. ............. ... . . .. . . . . . . ...... .. .. . . lowess fit . ............................................................................................................................................................................ ............... .. .. ..... . . . . . . ............................ . . . . . . . . . . . . . . . . .. . . ..................................................... .. . ............................................... ................ ....... ... ... .... . . . ............................................................................................................................................................................. . .. . ... . .. ....................... ..................... .......................................................................... .... .. . ...... ..... .. . .. . . .......... ....... ... .... ........ ... ..... . .... ... . ............................................................. .. .. .................................... ..................................................................................................................... ............... . . ..... .... . . . . . alpha = -0.5 ................................................. ................. ................................................................................................................. .... . .. .. ..... . . . . . . . . . . . . .. . . . . . . . . . . . . ....................................................................................... ..... ... ... ............. . . . .... .. . . .. ................ .......... .. .... .... . . .. . . .. ....... . . .. .... . . . .. . .... . . . . ... .. . . .. . .. ... .. ... . . .. .. .... .. .... . .. ..... .. . . . . . .... ..... .. ... .. ....... ... . . . . ....... .. ....... .. ....... .... .. . .. . ..... ..... . . . . . . . . . . . . .. . . .. . . . . . . .. . .. . . .. . . alpha = -0.07 . . . .. . .. . .. . . .. .. lowess fit . .. . .. . . . alpha = -0.5 0 10^7 3*10^7 Total vote for the two leading candidates Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Latent Gaussian model on a tree of voters I Put a continuous value at each node of the tree; random variation added as you go down the tree I I Look at the implied probability distribution for V n , the average of n voters √ Standard deviation of V n has the form a − b log n I Also fits the data Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Latent Gaussian model on a tree of voters I Put a continuous value at each node of the tree; random variation added as you go down the tree I I Look at the implied probability distribution for V n , the average of n voters √ Standard deviation of V n has the form a − b log n I Also fits the data Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Latent Gaussian model on a tree of voters I Put a continuous value at each node of the tree; random variation added as you go down the tree I I Look at the implied probability distribution for V n , the average of n voters √ Standard deviation of V n has the form a − b log n I Also fits the data Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Latent Gaussian model on a tree of voters I Put a continuous value at each node of the tree; random variation added as you go down the tree I I Look at the implied probability distribution for V n , the average of n voters √ Standard deviation of V n has the form a − b log n I Also fits the data Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Latent Gaussian model on a tree of voters I Put a continuous value at each node of the tree; random variation added as you go down the tree I I Look at the implied probability distribution for V n , the average of n voters √ Standard deviation of V n has the form a − b log n I Also fits the data Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems √ 0.0 Proportional vote differential 0.2 0.4 0.6 0.8 Comparing the models cn−α and a − b log n . . . . . . . .. . . .. . . ... . ... . ... .. .. . . .. . . . .. . . . ... .. . . . . . . . .. ... . . . . . ... . . . . . .. . . . ..... . .. .... . . . . . . ........... . .. . .. . . . ... . . . ............ ... .. ... .. .. . . . . . . . . . . . . . ...... . ... . .... . . . . . . . . .. . . .... .. . .. .. . .... . . . . .. ..... . ... .. .. .... .. . . . ........ .. . . .... ... . .. . . . . . . . . . . . . . . . . . . . .. . .. . .. ...... . ... ... ..... .. . .. . .. . . . .... .. . ..... .... ..... . ... . . . . . . .. . .. . . ... ... .. ... .. . . . .. . ............ . ....... ... . ... .. .. . . .. .. . .............. ... .......... ........... . ... . .. .. . . . .. .. .... . . .. . . . .. . . . . . . 0 . . . . . . . alpha = -0.16 b = 0.01 . 2*10^6 6*10^6 10^7 Total vote for the two leading candidates Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Open problems I General statements about voting power (for example, under what conditions are proportional voting systems roughly “fair”?) I Fitting more realistic tree models to electoral data I Fitting similar models to other data (for example, 5-level survey of smoking in India) I Network models Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Open problems I General statements about voting power (for example, under what conditions are proportional voting systems roughly “fair”?) I Fitting more realistic tree models to electoral data I Fitting similar models to other data (for example, 5-level survey of smoking in India) I Network models Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Open problems I General statements about voting power (for example, under what conditions are proportional voting systems roughly “fair”?) I Fitting more realistic tree models to electoral data I Fitting similar models to other data (for example, 5-level survey of smoking in India) I Network models Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Open problems I General statements about voting power (for example, under what conditions are proportional voting systems roughly “fair”?) I Fitting more realistic tree models to electoral data I Fitting similar models to other data (for example, 5-level survey of smoking in India) I Network models Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Standard voting power measures Data from real elections More complex mathematical/statistical modeling Open problems Open problems I General statements about voting power (for example, under what conditions are proportional voting systems roughly “fair”?) I Fitting more realistic tree models to electoral data I Fitting similar models to other data (for example, 5-level survey of smoking in India) I Network models Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Conclusions I Coalitions I I I Voting power I I I Forming coalitions can help you but hurt others Potential explanation for political instability (even in the absence of “real” disputes) The electoral college favors voters in small states “Voting power” calculations that claim otherwise are based on the falsifiable (and falsified) rule that elections will be extremely close in large states Mathematical models can give insights but must be looped back to real data Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Conclusions I Coalitions I I I Voting power I I I Forming coalitions can help you but hurt others Potential explanation for political instability (even in the absence of “real” disputes) The electoral college favors voters in small states “Voting power” calculations that claim otherwise are based on the falsifiable (and falsified) rule that elections will be extremely close in large states Mathematical models can give insights but must be looped back to real data Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Conclusions I Coalitions I I I Voting power I I I Forming coalitions can help you but hurt others Potential explanation for political instability (even in the absence of “real” disputes) The electoral college favors voters in small states “Voting power” calculations that claim otherwise are based on the falsifiable (and falsified) rule that elections will be extremely close in large states Mathematical models can give insights but must be looped back to real data Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Conclusions I Coalitions I I I Voting power I I I Forming coalitions can help you but hurt others Potential explanation for political instability (even in the absence of “real” disputes) The electoral college favors voters in small states “Voting power” calculations that claim otherwise are based on the falsifiable (and falsified) rule that elections will be extremely close in large states Mathematical models can give insights but must be looped back to real data Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Conclusions I Coalitions I I I Voting power I I I Forming coalitions can help you but hurt others Potential explanation for political instability (even in the absence of “real” disputes) The electoral college favors voters in small states “Voting power” calculations that claim otherwise are based on the falsifiable (and falsified) rule that elections will be extremely close in large states Mathematical models can give insights but must be looped back to real data Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Conclusions I Coalitions I I I Voting power I I I Forming coalitions can help you but hurt others Potential explanation for political instability (even in the absence of “real” disputes) The electoral college favors voters in small states “Voting power” calculations that claim otherwise are based on the falsifiable (and falsified) rule that elections will be extremely close in large states Mathematical models can give insights but must be looped back to real data Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Conclusions I Coalitions I I I Voting power I I I Forming coalitions can help you but hurt others Potential explanation for political instability (even in the absence of “real” disputes) The electoral college favors voters in small states “Voting power” calculations that claim otherwise are based on the falsifiable (and falsified) rule that elections will be extremely close in large states Mathematical models can give insights but must be looped back to real data Andrew Gelman Coalitions, voting power, and political instability Coalitions and political instability Mathematical and statistical models of voting power Conclusions Conclusions I Coalitions I I I Voting power I I I Forming coalitions can help you but hurt others Potential explanation for political instability (even in the absence of “real” disputes) The electoral college favors voters in small states “Voting power” calculations that claim otherwise are based on the falsifiable (and falsified) rule that elections will be extremely close in large states Mathematical models can give insights but must be looped back to real data Andrew Gelman Coalitions, voting power, and political instability