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Network Modeling of Cooperation in Public Goods Games
Elgar Pichler1 (elgar.pichler@gmail.com) Avi M. Shapiro2 (ashapiro@seas.harvard.edu)
1Department of Chemistry and Chemical Biology, Northeastern University
2Department of Applied Mathematics, Harvard University
Introduction
Well-functioning societies feature high levels of cooperation and strong
connections between individuals [2].
Many classic results of game theory show mutual defection (as opposed
to cooperation) to be a Nash Equilibrium in well-mixed populations.
We simulate the coevolutionary dynamics of PGG players (nodes) who
can choose their strategies, either to cooperate or to defect, and who
can adapt by altering their social connections (edges).
Certain network structures of individuals allow for high levels of
cooperation in PGGs even when players can change their strategy and
connections only based on their individual payoff and satisfaction, but
without specific information about neighbors’ strategies.
Public Goods Game (PGG)
PGG Description:
In a PGG, cooperators contribute a certain amount to the public good
and defectors do not. All players then receive an equal share of the sum
of all contributions multiplied by a synergy factor, r ≥ 1. We can write
the payoffs for cooperators and defectors,
πC = r
n
N
−1, πD = r
n
N
where n is the number of cooperators and N is the number of players.
Example:
At a given time step, a player
at node 1 has 3 neighbors and
thus collects a total payoff
from 4 separate PGGs.
1
2
PGG1
PGG2
PGG Networks:
PGGs as 2D cellular automata with nearest neighbor interactions only
were investigated in [3]. We generalize this PGG model by allowing
connections between arbitrary nodes in a non-planar network topology.
PGGs on such graphs have applications in peer-to-peer, mobile, and
vehicular networks.
Coevolutionary Rules
At time step t, player i may change strategy and/or neighbors with
independent probabilities based on satisfaction
si(t) = πi(t)−ai(t)+ηi(t),
where πi is the current total payoff, ηi is a Gaussian noise, and ai is
aspiration, defined
ai(t) = απi,max(t)+(1−α)πi,min(t),
which depends on greediness 0 ≤ α ≤ 1, another important control
parameter. πi,max/min reflect finite memory of past max/min payoffs.
Simulation Methodology
Coded in Python using NetworkX library, run on multicore Linux clusters
Network variables monitored: number of components, largest component
size, clustering coefficient, degree distribution
PGG variables monitored: aspiration, payoff, satisfaction, strategy
PGG consists of 1000 players and is a function of synergy r and
greediness α. Simulations were stopped at t = 20000.
Initial conditions: Barabási-Albert graph [1], all players are defectors
Simulation Results – Time Series
The model evolution is best captured by the variables cooperation, the
cooperator fraction, instability, the fraction of players changing strategies or
neighbors, and agglomeration, the average node degree. In these results,
r = 4 and α = 0.65.
High cooperation is
achieved through
instability triggering
higher agglomeration.
0 10000 20000
t
0.0
0.5
1.0
instability
cooperation
cooperation
instability
0
15
30
agglomeration
agglomeration
The evolution is
stochastic and undergoes
large but short spikes. To
observe larger trends, we
average over a moving
window of 100 time steps
in all other plots.
0.0
0.5
1.0 cooperator fraction
no time averaging
0 10000 20000
t
0.0
0.5
1.0
moving average
over 100 steps
Several simulations for
each parameter pair reveal
consistently similar
behavior, although shifted
in time.
0.0
0.5
1.0 cooperation
0.0
0.5
1.0 instability
0 10000 20000
t
0
15
30 agglomeration
Simulation Results – PGG Network Development
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227
t = 0 t = 10000 t = 15000 t = 20000
Simulation Results – Network Topology
Over time, the network topology changes due to player (dis)satisfaction.
Average node degree increases but the distribution changes more
dramatically, and is no longer scale-free by t = 20000.
10
0
10
1
10
2
10
3
degree
10
-3
10
-2
10
-1
10
0
degree
distribution
r=4, =0.65
r=3, =0.65
0 10000 20000
t
0
15
30
average
nodedegree
r=4, =0.65
r=3, =0.65
Simulation Results – Phase Diagram
Cooperation is not only possible but dominates for a region of parameter
values r and α. The transition to a cooperative regime is sharp in time
as well as in parameter space. The following phase diagram shows the
cooperator fraction at t = 20000 averaged over 5 simulations.
cooperator fraction
5 10 15 20 25 30
r
0.0
0.2
0.4
0.6
0.8
0.0
0.2
0.4
0.6
0.8
1.0
0 10000 20000
t
0.0
0.5
1.0
r=4, =0.65
r=3, =0.65
Interestingly, the largest cooperation is found for high greediness and low
values of synergy.
Conclusions
In PGGs played on networks, stable cooperative behavior arises for a wide
range of parameters, even if initial conditions are seemingly
disadvantageous to cooperativity.
During the transition to a cooperative regime, the number of low degree
nodes decreases and the initial scale-free structure is destroyed.
As the PGG system approaches steady state – at t = 20000, our system
has not reached steady state – the expected behavior of the overall
system will stabilize while short time extreme fluctuations can still occur.
References
[1] Réka Albert and Albert-László Barabási.
Statistical mechanics of complex networks.
Reviews of Modern Physics, 74:47, 2002.
[2] Martin A. Nowak.
Five rules for the evolution of cooperation.
Science, 314(5805):1560–1563, Dec 2006.
[3] Carlos P. Roca and Dirk Helbing.
Emergence of social cohesion in a model society of greedy, mobile individuals.
Proc Natl Acad Sci USA, 108(28):11370–11374, Jul 2011.

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Poster_2014_PGG_SIAM-WNS

  • 1. Network Modeling of Cooperation in Public Goods Games Elgar Pichler1 (elgar.pichler@gmail.com) Avi M. Shapiro2 (ashapiro@seas.harvard.edu) 1Department of Chemistry and Chemical Biology, Northeastern University 2Department of Applied Mathematics, Harvard University Introduction Well-functioning societies feature high levels of cooperation and strong connections between individuals [2]. Many classic results of game theory show mutual defection (as opposed to cooperation) to be a Nash Equilibrium in well-mixed populations. We simulate the coevolutionary dynamics of PGG players (nodes) who can choose their strategies, either to cooperate or to defect, and who can adapt by altering their social connections (edges). Certain network structures of individuals allow for high levels of cooperation in PGGs even when players can change their strategy and connections only based on their individual payoff and satisfaction, but without specific information about neighbors’ strategies. Public Goods Game (PGG) PGG Description: In a PGG, cooperators contribute a certain amount to the public good and defectors do not. All players then receive an equal share of the sum of all contributions multiplied by a synergy factor, r ≥ 1. We can write the payoffs for cooperators and defectors, πC = r n N −1, πD = r n N where n is the number of cooperators and N is the number of players. Example: At a given time step, a player at node 1 has 3 neighbors and thus collects a total payoff from 4 separate PGGs. 1 2 PGG1 PGG2 PGG Networks: PGGs as 2D cellular automata with nearest neighbor interactions only were investigated in [3]. We generalize this PGG model by allowing connections between arbitrary nodes in a non-planar network topology. PGGs on such graphs have applications in peer-to-peer, mobile, and vehicular networks. Coevolutionary Rules At time step t, player i may change strategy and/or neighbors with independent probabilities based on satisfaction si(t) = πi(t)−ai(t)+ηi(t), where πi is the current total payoff, ηi is a Gaussian noise, and ai is aspiration, defined ai(t) = απi,max(t)+(1−α)πi,min(t), which depends on greediness 0 ≤ α ≤ 1, another important control parameter. πi,max/min reflect finite memory of past max/min payoffs. Simulation Methodology Coded in Python using NetworkX library, run on multicore Linux clusters Network variables monitored: number of components, largest component size, clustering coefficient, degree distribution PGG variables monitored: aspiration, payoff, satisfaction, strategy PGG consists of 1000 players and is a function of synergy r and greediness α. Simulations were stopped at t = 20000. Initial conditions: Barabási-Albert graph [1], all players are defectors Simulation Results – Time Series The model evolution is best captured by the variables cooperation, the cooperator fraction, instability, the fraction of players changing strategies or neighbors, and agglomeration, the average node degree. In these results, r = 4 and α = 0.65. High cooperation is achieved through instability triggering higher agglomeration. 0 10000 20000 t 0.0 0.5 1.0 instability cooperation cooperation instability 0 15 30 agglomeration agglomeration The evolution is stochastic and undergoes large but short spikes. To observe larger trends, we average over a moving window of 100 time steps in all other plots. 0.0 0.5 1.0 cooperator fraction no time averaging 0 10000 20000 t 0.0 0.5 1.0 moving average over 100 steps Several simulations for each parameter pair reveal consistently similar behavior, although shifted in time. 0.0 0.5 1.0 cooperation 0.0 0.5 1.0 instability 0 10000 20000 t 0 15 30 agglomeration Simulation Results – PGG Network Development 819 433 799 340 298 465 948 735 836 933 8 9 6 5 833 470 280 775 313 973 563 953 188 582 885 535 409 244 878 9 1 558 942 421 808 213 930 300 943 658 7 1 991 397 738 1 5 773 457 572 716 376 844 516 267 542 511 874 299 687 963 812 446 182 467 923 483 618 575 780 593 203 545 1 1 5 7 4 4 514 756 152 167 362 662 784 995 925 734 865 968 653 723 449 705 335 296 440 628 682 416 485 331 832 527 898 263 612 105 866 926 270 810 646 821 902 2 4 229 5 1 356 484 727 494 567 453 1 2 673 382 559 363 295 623 681 581 325 880 333 6 2 359 597 546 317 576 447 689 386 667 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900 8 8 321 484 620 618 3 3 730 311 417 807 145 524 590 699 574 903 161 543 811 534 272 717 966 409 152 566 138 643 346 987 859 221 352 569 681 799 735 669 269 805 5 3 197458 323 902 319 141 959 970 639 962 853 281 675 792 731 513 9 4 353 216 459 172 850 837 496 660 368 646 119 178 400 270 591 182 395 758 411 468 107 823 444 925 765 132 317 404 220 456 338 354 123 635 844 482 401 726 206 279 938 584 740 625 451 691 331 626 601 2 6 759 747 382 909 550 609 908 391 433 166 8 6 637 330 8 4 1 9 143 810 509 714 280 704 858 116 389 9 0 246 375 586 506 905 526 804 889 127 199 608 656 553 3 6 117 778 341 603 462 512 680 950 288 556 985 612 6 8 163 527 822 677 531 426 860 240 5 473 994 3 8 7 8 392 254 243 739 478 228 616 363 762 721 1 563 2 9 282 380 186 989 789 448 253 516 328 467 817 892 108 623 664 3 515 110 170 7 5 5 7 453 431 207 416 749 790 131 359 887 755 983 613 587 716 929 544 244 668 100 651 148 547 7 1 283 211 115 573 294 915 802 705 525 192 436 851706 845 4 5 551 865 434 756 369 926 907 984 700 728 247 548 518 554 812 500 6 6 690 752 185 806 589 3 9 847 440 150 881 528 884 634 992 383 412 8 1 622 732 671 826 275 791 265 320 894 125 746 486 642 990 231 1 0 9 9 450 895 867 201 657 975 358 397 234 570 155 824 136 2 855 6 427 171 832 968 941 313 906 111 438 916 982 819 4 7 961 342 552 225 470 293 873 4 0 2 0 583 1 7 897 976 536 495 157 104 785 991 870 733 878 8 0 2 3 374 564 193 336 9 1 833 260 106 585 825 365 815 396 523 771 655 686 624 698 842 883 836 5 0 607 510 911 242 846 209 238 578 184 344 292 996 696 113 4 2 5 6 376 8 5 236 437 783 6 4 203 712 776 343 3 7 191 5 1 457 9 2 571 271 180 204 694 1 6 7 4 537 307 896 101 545 356 715 296 659 628 481 322 914 7 7 7 449 610 471 423 501 971 964 4 1 188 499 432 425 519 1819 3 264 561 463 688 124 424 693 306 4 6 202 217 588 213 782 445 644 621 995 360 291 3 2 144 219 314 877 798 419 562 652 476 713 129 918 697 250 337 286 748 615 879 465 2 5 960 507 579 848 258 435 232 560 226 273 942 384 517 406 814 529 210 729 904 373 917 520 830 149 492 3 1 999 121 393 224 633 539 604 602 658 174 379 541 439 2 4 349 299 781 348 4 3 266 103 702 3 4 479 866 430 930 263 122 249 647 9 6 596 928 239 257 854 160 796 474 405 592 189 780 198 2 7 168 816 965 761 208 684 993 8 176 614 7 3 861 936 530 235 827 300 597 326 455 398 120 898 284 737 940 179 606 953 674 944 452 679 711 599 227 t = 0 t = 10000 t = 15000 t = 20000 Simulation Results – Network Topology Over time, the network topology changes due to player (dis)satisfaction. Average node degree increases but the distribution changes more dramatically, and is no longer scale-free by t = 20000. 10 0 10 1 10 2 10 3 degree 10 -3 10 -2 10 -1 10 0 degree distribution r=4, =0.65 r=3, =0.65 0 10000 20000 t 0 15 30 average nodedegree r=4, =0.65 r=3, =0.65 Simulation Results – Phase Diagram Cooperation is not only possible but dominates for a region of parameter values r and α. The transition to a cooperative regime is sharp in time as well as in parameter space. The following phase diagram shows the cooperator fraction at t = 20000 averaged over 5 simulations. cooperator fraction 5 10 15 20 25 30 r 0.0 0.2 0.4 0.6 0.8 0.0 0.2 0.4 0.6 0.8 1.0 0 10000 20000 t 0.0 0.5 1.0 r=4, =0.65 r=3, =0.65 Interestingly, the largest cooperation is found for high greediness and low values of synergy. Conclusions In PGGs played on networks, stable cooperative behavior arises for a wide range of parameters, even if initial conditions are seemingly disadvantageous to cooperativity. During the transition to a cooperative regime, the number of low degree nodes decreases and the initial scale-free structure is destroyed. As the PGG system approaches steady state – at t = 20000, our system has not reached steady state – the expected behavior of the overall system will stabilize while short time extreme fluctuations can still occur. References [1] Réka Albert and Albert-László Barabási. Statistical mechanics of complex networks. Reviews of Modern Physics, 74:47, 2002. [2] Martin A. Nowak. Five rules for the evolution of cooperation. Science, 314(5805):1560–1563, Dec 2006. [3] Carlos P. Roca and Dirk Helbing. Emergence of social cohesion in a model society of greedy, mobile individuals. Proc Natl Acad Sci USA, 108(28):11370–11374, Jul 2011.