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172 6. Comportements mimétiques <strong>et</strong> antagonistes : bulles hyperboliques, krachs <strong>et</strong> chaos<br />

Q UANTITATIVE F INANCE Imit<strong>at</strong>ion and contrarian behaviour: hyperbolic bubbles, crashes and chaos<br />

Probability<br />

1.0<br />

Symm<strong>et</strong>ric dynamics<br />

0.9<br />

0.8<br />

0.7<br />

0.6<br />

0.5<br />

Asymm<strong>et</strong>ric dynamics<br />

0.4<br />

0.3<br />

0.2<br />

0.1<br />

0.0<br />

Effect of periodic<br />

orbits<br />

–0.5 –0.4 –0.3 –0.2 –0.1 0.0<br />

p–1/2<br />

0.1 0.2 0.3 0.4 0.5<br />

Figure 14. Cumul<strong>at</strong>ive distribution function of p − 1/2 for m = 60<br />

polled agents and param<strong>et</strong>ers ρhb = ρbh = 0.72 and<br />

ρhh = ρbb = 0.85 (dashed line) and ρhb = 0.72, ρbh = 0.74,<br />

ρhh = 0.85 and ρbb = 0.87 (continuous line). Note th<strong>at</strong> the<br />

asymm<strong>et</strong>ric dynamics has the effect of shifting the cumul<strong>at</strong>ive<br />

distribution to the right.<br />

7.1. Finite-size effects in other mo<strong>de</strong>ls<br />

We now investig<strong>at</strong>e finite-size effects resulting from a finite<br />

number N of interacting agents trading on the stock mark<strong>et</strong>.<br />

This issue of the role of the number of agents has recently been<br />

investig<strong>at</strong>ed vigorously with surprising results.<br />

Hellthaler (1995) studied the N-<strong>de</strong>pen<strong>de</strong>nce of the<br />

dynamical properties of price time series of the Levy <strong>et</strong> al<br />

mo<strong>de</strong>l (1995, 2000). Egenter <strong>et</strong> al (1999) did the same for the<br />

Kim and Markowitz (1989) and the Lux and Marchesi (1999)<br />

mo<strong>de</strong>ls. They found th<strong>at</strong>, if this number N goes to infinity,<br />

nearly periodic oscill<strong>at</strong>ions occur and the st<strong>at</strong>istical properties<br />

of the price time series become compl<strong>et</strong>ely unrealistic. Stauffer<br />

(1999) reviewed this work and others such as the Levy <strong>et</strong> al<br />

(1995, 2000) mo<strong>de</strong>l: realistically looking price fluctu<strong>at</strong>ions<br />

are obtained for N ∝ 102 , but for N ∝ 106 the prices<br />

vary smoothly in a nearly periodic and thus unrealistic way.<br />

The mo<strong>de</strong>l proposed by Farmer (1998) suffers from the same<br />

problem: with a few hundred investors, most investors are<br />

fundamentalists during calm times, but bursts of high vol<strong>at</strong>ility<br />

coinci<strong>de</strong> with large fractions of noise tra<strong>de</strong>rs. When N<br />

becomes much larger, the fraction of noise tra<strong>de</strong>rs goes to zero<br />

in contradiction to reality. On a somewh<strong>at</strong> different issue,<br />

Huang and Solomon (2001) have studied finite-size effects<br />

in dynamical systems of price evolution with multiplic<strong>at</strong>ive<br />

noise. They find th<strong>at</strong> the exponent of the Par<strong>et</strong>o law<br />

obtained in stochastic multiplic<strong>at</strong>ive mark<strong>et</strong> mo<strong>de</strong>ls is crucially<br />

affected by a finite N and may cause, in the absence of<br />

an appropri<strong>at</strong>e social policy, extreme wealth inequality and<br />

mark<strong>et</strong> instability. Another mo<strong>de</strong>l (apart from ours) where<br />

the mark<strong>et</strong> may stay realistic even for N →∞seems to be<br />

the Cont and Bouchaud percol<strong>at</strong>ion mo<strong>de</strong>l (2001). However,<br />

this only occurs for an unrealistic tuning of the percol<strong>at</strong>ion<br />

concentr<strong>at</strong>ion to its critical value. Thus, in most cases, the<br />

limit N →∞leads to a behaviour of the simul<strong>at</strong>ed mark<strong>et</strong>s<br />

Correl<strong>at</strong>ion<br />

1.2<br />

1.0<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0.0<br />

–0.2<br />

Symm<strong>et</strong>ric dynamics<br />

Asymm<strong>et</strong>ric dynamics<br />

0 20 40 60 80 100 120 140 160 180 200<br />

Time lag<br />

Figure 15. Correl<strong>at</strong>ion function for m = 60 polled agents and<br />

param<strong>et</strong>ers ρhb = ρbh = 0.72 and ρhh = ρbb = 0.85 (dashed line)<br />

and ρhb = 0.72, ρbh = 0.74, ρhh = 0.85 and ρbb = 0.87 (continuous<br />

line). Note th<strong>at</strong> the correl<strong>at</strong>ion function of r<strong>et</strong>urns goes to zero<br />

(within the noise level) <strong>at</strong> time lags larger than about 100. This<br />

unrealistic fe<strong>at</strong>ure of a long-range correl<strong>at</strong>ion in the r<strong>et</strong>urns makes it<br />

unnecessary to show the even longer-range correl<strong>at</strong>ion of the<br />

absolute values of the r<strong>et</strong>urns.<br />

which becomes quite smooth or periodic and thus predictable,<br />

in contrast to real mark<strong>et</strong>s. Our mo<strong>de</strong>l, which remains<br />

(d<strong>et</strong>erministically) chaotic, is thus a significant improvement<br />

upon this behaviour. We trace this improvement on the highly<br />

nonlinear behaviour resulting from the interplay b<strong>et</strong>ween<br />

the imit<strong>at</strong>ive and contrarian behaviour. It has thus been<br />

argued (Stauffer 1999) th<strong>at</strong>, if these previous mo<strong>de</strong>ls are good<br />

<strong>de</strong>scriptions of mark<strong>et</strong>s, then real mark<strong>et</strong>s with their strong<br />

random fluctu<strong>at</strong>ions are domin<strong>at</strong>ed by a r<strong>at</strong>her limited number<br />

of large players: this amounts to the assumption th<strong>at</strong> the<br />

hundred most important investors or investment companies<br />

have much more influence than the millions of less wealthy<br />

priv<strong>at</strong>e investors.<br />

There is another class of mo<strong>de</strong>ls, the minority games<br />

(Chall<strong>et</strong> and Zhang 1997), in which the dynamics remains<br />

complex even in the limit N →∞. It has been established<br />

th<strong>at</strong> the fluctu<strong>at</strong>ions of the sum of the aggreg<strong>at</strong>e <strong>de</strong>mand<br />

have an approxim<strong>at</strong>e scaling with similar sized fluctu<strong>at</strong>ions<br />

(vol<strong>at</strong>ility/standard <strong>de</strong>vi<strong>at</strong>ion) for any N and m for the scale<br />

scaled variable 2 m /N, where m is the memory length (Chall<strong>et</strong><br />

<strong>et</strong> al 2000). In a generaliz<strong>at</strong>ion, the so-called grand canonical<br />

version of the minority game (Jefferies <strong>et</strong> al 2001), where the<br />

agents have a confi<strong>de</strong>nce threshold th<strong>at</strong> prevents them from<br />

playing if their str<strong>at</strong>egies have not been successful over the<br />

last T turns, the dynamics can <strong>de</strong>pend more sensitively on N:<br />

as N becomes small, the dynamics can become quite different.<br />

For large N, the complexity remains.<br />

The difference b<strong>et</strong>ween the limit N →∞consi<strong>de</strong>red up<br />

to now in this paper and the case of finite N is th<strong>at</strong> pt is no<br />

longer the fraction of bullish agents. For finite N, pt must<br />

be interpr<strong>et</strong>ed as the probability for an agent to be bullish.<br />

Of course, in the limit of large N, the law of large numbers<br />

275

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