Criticality
University of Brasilia
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Abstract
This article reviews some current interdisciplinary work on so-called 'power
laws'.
Keywords: power laws, criticality, scaling, complexity theory
Introduction
Certain
complex systems, under certain circumstances, have been discovered to behave in
similar, mathematically simple ways. This has been dubbed 'criticality'. In a
critical state there is no reason to look for specific causes of great events.
The smallest force can have gigantic effects and sudden upheavals can occur
seemingly out of nowhere. Fluctuations of something in a critical state are
neither truly random nor easily predicted. The approximate frequency of such upheavals
can be predicted, but not when they will happen or what size they will be. A
recent book (Buchanan 2000b) reviews the current work on the subject to
highlight a deep similarity between the upheavals that affect our lives in
ecosystems, economies, and even political systems. This article draws on the
book. One of the discoveries in modern physics is that criticality often arises
on its own in non-equilibrium systems, and in things in which history matters.
The workings of the systems in which upheavals occur may sometimes reflect
simple and universal underlying processes that can be captured by simple
mathematical 'games' that share a common skeletal logic. Scientists in other
fields have taken advantage of this breakthrough already. As observed, in the
13 years since its discovery, the idea of criticality has spread like wildfire
to scientific disciplines ranging from geophysics to biology, economics, and
history (Bak 2000).
Critical
State Universality
The
theoretical work on criticality is based on simple models that can be studied
by either mathematical analysis or computer simulations. Understanding the
critical state in any system from one class is to immediately understand all
systems in that class. The models are more metaphorical than those used in
theoretical physics, for instance. Like all theoretical modeling it must stand
the test of comparison with nature, though. The test comes by adding a few of
the neglected details back in, and seeing if they change the results in any
essential way.
The
principle of universality or ubiquity means that one should focus on the
simplest mathematical game belonging to an equivalent universal class. Details
are not important in deciding the outcome. Even crude models can work exactly
like the real thing. Details have no influence because things in a critical
state have no inherent typical scale in either time or space.
Power
Laws
In a
critical state, something known as a 'power law' comes into play to reveal a
hidden order and simplicity behind complexity (see an example
). A power
law means that there is no such thing as a normal or typical event, and that
there is no qualitative difference between the larger and smaller fluctuations.
Upheavals are not unusual. A big event need not have a cause. The causes that
trigger a small change on one occasion may initiate a devastating change on
another, and no analysis of the conditions at the initial point will suffice to
predict the event.
Power
laws are incompatible with bell-shaped normal curves. A bell-shaped curve
establishes that an average gives someone a good idea of what to expect. A
normal distribution is supposedly the norm in nature. Its widespread
applicability is a consequence of the central limit theorem: in any case in
which a large number of independent influences contribute to the outcome of
some event, that outcome will result in a bell curve. That is not to say that
everything follows a bell curve, though. An equally large number of things do
not. Some are governed by power laws.
If,
for instance, one throws frozen potatoes at a wall, they will break into
fragments of varying size. If one collects all the pieces up, from the
microscopic ones to the large, and puts them into different piles according to
weight, a power law for fracture emerges: each time the weight of the fragments
is reduced by two, there will be six times as many. Power laws have been
discovered for events ranging from forest fires and earthquakes to mass
extinctions and stock market crashes.
Self-Similarity
Mandelbrot
(1963) discovered that if he took a small section of the record of the price of
cotton on the Chicago mercantile exchange, and stretched it out so that it
became as long as the entire record, it looked much like the whole. He had
discovered self-similarity. Following that, he invented the geometry of
fractals (Mandelbrot 1982). Self-similarity or scale-invariance (every part is
a tiny image of the whole) is reflected in a power law.
The
geometric regularity of any power law implies a lack of any typical scale, a
feature that shows up clearly in the critical point image, which is a fractal.
What counts in the critical state is the simple underlying features of geometry
that control how influences can propagate. Fractals and power laws are at work
in settings where the critical state underlies their dynamics. Fractals can be
produced by chaos, but they also arise in processes of growth or evolution. To
understand fractals and power laws, one needs a historical physics, not an
equilibrium physics. This is so because the notion of history has no meaning in
equilibrium.
Financial
markets demonstrate several of the properties that characterize complex
systems. What is more, they are highly complex, open systems in which many
subunits interact nonlinearly in the presence of feedback and stable governing
rules. Earlier attempts to find chaos in financial data, for instance, have
been disappointing (e.g. Da Silva 2001) exactly because the phenomenon is
likely to emerge in systems that are only moderately complex. Although it
cannot be ruled out that financial markets follow chaotic dynamics (fake
randomness), the work on 'econophysics' (discussed below) assumes that asset
price dynamics are stochastic processes, which may be governed by power laws.
Self-Organized
Criticality
Tuning
is crucial to reach a critical point in which any tiny event can trigger a huge
upheaval. Sometimes criticality can be tuned by nature on its own, though. This
is dubbed 'self-organized criticality'. Self-organized criticality seems to
show up in things that are driven slowly away from equilibrium, and in which
the actions of any individual piece are dominated by its interactions with
other elements.
Forest
Fires
Forests
are an good example of self-organized criticality. The network of trees on a
grid seems naturally to tune itself to a critical state in which the next match
might spark a fire of any size, even one that would destroy the entire forest.
A power law for forest fires has been found: when the area covered by a fire is
doubled, it becomes about 2.48 times as rare (Malamud et al. 1998). The
model invented to account for the spread of fires in forests may also be able
to capture the essence of how diseases spread through human populations. In the
toy model of forest fires, people have been plugged in in place of trees and
measles in place of fires (Rhodes and Anderson 1996). The result explained the
distribution of measles epidemics on the Faroe Islands in the North Atlantic.
Even if the trees are people, and the fire is a disease, disturbances still
spread in the same way.
The
Role of Free Will
Individual
free will offers no escape from the inevitability of criticality. Even though
people interact with one another by virtue of their own personal choices, there
nevertheless exists definite mathematical patterns in the activity of a group. These
patterns cannot help to predict what any one person will do, but they may be
able to say what is likely to emerge in the aggregate. What is more, the
mathematics is not complicated. The way people aggregate into cities, for
instance, does not seem to depend on the fact that they are people. The pattern
of population within any city may be described by using simple games from the
theory of phase transitions (Zanette and Manrubia 1997). Cities are possibly
fractals. So there is no typical size for any city, and no reason to see
special historical or geographical situations behind the emergence of the very
largest.
Avalanches
If one
takes a handful of rice (or sand) and drops the grains one by one on to a table
top, a pile of rice is built soon. The pile will not grow taller for ever,
though. Eventually the addition of one more grain will cause an avalanche. Such
a grain is only special because it happened to fall in the right place at the
right time. The addition of a single grain may have no effect, precipitate a
small avalanche, or collapse the whole structure. One can predict the likely
frequency of the avalanches, but not when they will happen or what size each
will be. It may come as no surprise that big avalanches occur less frequently
than small ones. What is surprising is that there is a power law: each time the
size of an avalanche of rice grains is doubled, it becomes twice as rare (Bak et
al. 1987). The apparent complexity of the pile collapses to a hidden order
and simplicity.
Earthquakes
If
fault systems in the earth's crust are in a critical state as well, then
predicting when earthquakes will strike, and how destructive they will be,
should prove impossible. Actually earthquake prediction research has been
conducted for over 100 years with no obvious successes (Geller 1997). An
earthquake occurs when the slow movement of the earth's continental plates does
not directly bring about any reorganizations of the earth's crust, since
friction holds the rocks in place. The movements of the plates simply put the
rocks under stress. Only when the stress builds up past some threshold do the
rocks move and reorganize themselves, suddenly and violently. Earthquakes thus
come from the build up and release of stress and seem to be distributed in
energy according to a power law. If the size of an earthquake is doubled, the
Gutenberg-Richter power law says those quakes become four times less frequent.
The bigger the quake, the rarer it is. Such a number corresponds to a
particular type of self-similar, fractal pattern. The distribution is scale
invariant, that is, what triggers small and large quakes is precisely the same.
Mass
Extinctions
Life
on earth suffers sporadic and catastrophic episodes of collapse. There have
been at least five mass extinctions of species in the earth's history (a brief
account is provided by Vines 1999). Most biologists do not believe that
evolution is itself capable of causing upheavals. There is evolution, and there
are the upheavals caused by exogenous shocks.
However,
mass extinctions are possibly intrinsic outcomes of the dynamics of evolution.
Indeed a power law for the distribution of extinction sizes that fits the
fossil record well has been found (Solé and Manrubia 1996). Such a power law
happens to be identical to that for earthquakes: every time the size of an
extinction (as measured by the number of families of species that become
extinct) is doubled, it becomes four times as rare. Thus mass extinctions need
not have big, exogenous causes; they might be provoked by small, endogenous
events.
The
Physics of History
The
concept of criticality might be useful in understanding history, which is
punctuated by inexplicable and unforeseeable upheavals. The First World War,
for instance, is the archetypal example of an unanticipated upheaval in world
history (Buchanan 2000b). Figuratively, Hegel and Marx thought of history as
the growth of a tree that follow a simple progression toward some mature,
stable end-point. Some writers (e.g. Fukayama 1992) have speculated that we are
approaching the end of history, as the world seems to be settling into some
ultimate equilibrium of global democracy and capitalism. Toynbee saw regular
cycles in the rise and fall of civilizations. History may instead be completely
random with no perceptible pattern. Historian H. A. L. Fisher has commented
that there is only one safe rule for the historian: that he should recognize in
the development of human destinies the play of the contingent and the
unforeseen (cited by Buchanan 2000c). Nevertheless there seem to be undeniable
trends in history, one of the most obvious being the increase in our scientific
understanding and technology. Perhaps history is chaotic: it looks random in
its workings, and yet it is not random at all. Ferguson (1997) has pointed that
historical chaos reconciles the notions of causality and contingency. Or maybe
history lives in a critical state.
In a
critical history, contingency would become powerful beyond measure. Contingency
takes place when immediate events control a supposed destiny. As observed,
contingency is the hallmark of the critical state (Bak 2000). Kennedy (1987)
has suggested that the large-scale historical rhythm in the interactions
between great powers is largely a consequence of the natural build up and
release of stress driven by national interests. Usually the stress finds its
release through armed conflict, after which the influence of each nation is
brought back into balance with its true economic strength.
Wars
seem to strike with the same statistical pattern as do earthquakes or
avalanches in the rice-pile game. Statistics over five centuries have uncovered
a power law for wars (Levy 1983). Every time the number of deaths is doubled,
wars of that size become 2.62 times less common. Such a power law implies that
when a war starts out no one knows how big it will become. There seem to be no
special conditions to trigger a great conflict. Interestingly the forest-fire
game seems to capture the crucial elements of the way that conflicts spread
(Turcotte 1999). A war may begin in a manner similar to the ignition of a
forest.
On
the History of Science
Kuhn
(1962)'s major achievement was to show that science works even though
scientists are like everyone else, that is, they labor under the burden of
being human. It could be argued that he discovered a pattern of universal
change that runs deeper than he suspected. He identified science as one setting
in which the universal build up and release of stress influences history.
'Normal' scientific work turns up inconsistencies, and leads to the growth of
stress within the existing fabric of ideas. When this maladjustment reaches
some threshold, normal science breaks down. Science cannot go further by
accumulation and extension, and has to rebuild some portion of the existing
network. The system shifts in a 'revolution'. Normal scientific work thus seems
to be analogous to the drifting of continental plates, and scientific
revolutions are akin to earthquakes.
Every
new idea of science is something like a grain falling on the pile of knowledge.
Each scientific research paper is a package of ideas which, when it settles
down in the pre-existing network of ideas, triggers some rearrangement. To
measure the overall size of the intellectual earthquake triggered by a paper,
one may look to the total number of times it is cited by other papers. Here
again there seems to be no typical number of citations for a paper. The
distribution of citations follows a scale-invariant power law (Redner 1998).
Every time the number of citations is doubled, the number of papers receiving
them falls by about eight times.
If the
history of science is in a critical state, the ultimate consequences of any new
idea would not depend on its own inherent profundity so much as on where it
happens to fall within the network of ideas. The mark of the great scientist
would lie not in having deep ideas that revolutionize science but in taking
insights that have the potential to do so and in making that potential real.
Even if scientists were all genetically identical clones, such revolutionary
achievements would still be done by a selected few.
Econophysics
and Economics
If
markets are critically organized, even the great stockmarket crashes would be
simply ordinary (although infrequent) events. In an efficient market, when
supply matches demand, prices have their proper values, that is, values
corresponding to the underlying 'fundamentals'. Market prices could bounce up
and down erratically still, but huge fluctuations could not be accounted for.
Price changes would behave like the bell curve according to most of mainstream
economics. Greater than some typical size, price changes ought to be extremely
rare. Prices would follow a gentle random walk. Black Monday, 19 October 1987
was the largest single-day free fall in market history. The crash was nearly
twice as severe as the stockmarket collapse of 1929, although this time it did
not trigger a depression. What made the Dow Jones industrial average lose more
than 22 per cent of its value in just one day? It is difficult to believe that
there could be a sudden change in the fundamentals which would lead agents
simultaneously within half a day to the view that returns in the future had
gone down by over 20 per cent. A dubious explanation has been that the crash
was caused by portfolio insurance computer programs which sold stocks as the
market went lower.
When
Mandelbrot (1963) looked at how random changes in prices were distributed by
size, he did not find a bell curve. Instead he discovered that price changes
are governed by a power law: price changes do not have a typical size. This
allows one to see large fluctuations in market prices as a result of the
natural, internal workings of markets; they can strike from time to time even
if there are no sudden alterations of the fundamentals. One reason might be
that real-world markets are not in equilibrium. Movements of markets appear to
be unpredictable in the direction up or down. (Other references are Mandelbrot
1997 and Bak et. al 1993.)
Other
power laws have been discovered. Price fluctuations in the Standard & Poor
500 stock index were found to become about sixteen times less likely each time
the size is doubled (Gopikrishnan et al. 1998). Scaling behavior for
the Standard & Poor 500 has also been detected by Mantegna and Stanley
(1995). A similar power-law holds for the prices of the stocks of individual
companies (Plerou et al. 1999). Power-laws were found too in the Milan
stock exchange (Mantegna 1991) and in foreign exchange markets (Müller et
al. 1990). A scale-invariant power law has also been found for financial
market volatility: the market does not have a typical wildness in its
fluctuations (Liu et al. 1999).
In a
simple game of the stockmarket, Lux and Marchesi (1999) have found
self-similarity, structure on all time scales, and a distribution of price changes
that follows a power law. Interestingly Ghashghaie et al. (1996) have
suggested that foreign exchange market dynamics corresponds to hydrodynamic
turbulence. (Mantegna and Stanley 2000 provide comprehensive references to the
work on econophysics.)
A
power-law for distribution of wealth according to Pareto law has also been
found (Bouchaud and Mezard 2000). If one counts how many people in America have
a net worth of a billion dollars, one will find that about four times as many
have a net worth of about half a billion. Four times as many again are worth a
quarter of a billion, and so on. (A non-technical discussion of this paper is
presented by Buchanan 2000a.)
Power
laws are expected to coexist uneasily with mainstream finance theory, for
instance, which is built on the efficient market hypothesis. Mandelbrot's
earlier findings were not absorbed into mainstream finance, which has since
been relying (although not completely) on Gaussian distributions (the debate
can be appreciated in Cootner 1964). However, econophysicists adopt a more
conciliatory gesture. They see the efficient market as an idealized system and
real markets as only approximately efficient; they think the concept of
efficient markets is still useful in any attempt to model financial markets.
But rather than simply assuming normality, they try to fully characterize the
statistical properties of the random processes observed in financial markets
(Mantegna and Stanley 2000, pp. 12-13).
International
finance economists, by contrast, are likely to welcome the concept of
criticality. After all, as Krugman (1989, p. 61) once remarked, most economists
today believe that "foreign exchange markets behave more like the unstable
and irrational asset markets described by Keynes than the efficient markets
described by modern finance theory". Krugman himself has made an attempt
to incorporate the notion of criticality into economics (Krugman 1996).
If a macroeconomy
is critically organized, a given (monetary or real) shock is not to blame by
itself for destabilizing the economy. How an economy is organized and prepared
to respond to shocks turns to be more important. As observed, "what
survives today of Keynesian economics is not the 'scientific' demonstration
that under-employment equilibrium is possible, but Keynes's intuition that a
market economy is inherently unstable, and that the source of instability lies
in the logic of financial markets. Market capitalism should be neither left
alone nor abolished, but stabilized" (Skidelsky 2000, p. 85). From a
theoretical perspective, absorption of the concept of criticality into
macroeconomics would favor a replacement of the current 'new neoclassical synthesis'
(e.g. Goodfriend and King 1997) by an approach based on the 'Keynes's
intuition' referred to above. Nonetheless one might speculate that policymakers
would have a harder job to do in a critically organized macroeconomy.
Concluding
Remarks
In
what sense can it be true that an earthquake, a forest fire, a mass extinction
and a stockmarket crash are events of the very same type? How could an event as
tumultuous as the 1987 stockmarket crash arrive without any warning? Great
earthquakes, forest fires, mass extinctions, and stockmarket crashes may be
merely the expected large fluctuations that arise universally in
non-equilibrium systems in a critical state. Here the organization of a system
depends in no way on the precise nature of the things involved, but only on the
way that influences can propagate from one thing to the next. Upheavals result
from the natural build up and release of stress.
Just
as it is tempting to seek great causes behind great earthquakes or mass
extinctions, it is also tempting to see great persons behind the great events
in history. However the only general cause for such an event may be the
underlying organizations of the critical state, which make upheavals not only
possible but inevitable. Criticality may also be present in the ways ideas
evolve and change. The character of the critical state is reflected in
remarkably simple, statistical laws: the scale-free power laws that reveal a
lack of any expected size for the next event.
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© copyright 2001 Sergio Da Silva. All rights reserved. I thank Mark Buchanan and Tilly Warren for comments and discussions.
Published by the Brazilian Journal of Business Economics 2(2), pp. 33-45 (2002).