INW2 Inaugural Lecture |
Inaugural lecture of the The arrow of time Ilya Prigogine
©ICRANet
Introduction
Mr. Mayor, Authorities, Dear Colleagues and Friends:
First of all, I am very sorry that I cannot speak Italian. I have always admired very much
Italy, which is the land of the two cultures. Italy has produced outstanding scientists,
as well as, outstanding artists and great philosophers.
The determinism in nature I like to quote a letter of Einstein to Tagore. Einstein wrote, "If the moon would be asked why it follows its eternal path around the earth, he may answer that he is gifted with self-consciousness and that his decision was made once and for all." We smile, because we know that his path abides by Newton's Laws. Einstein asks that we should also smile when you believe that you act on your own initiative. Our initiative is simply an illusion, because there is no reason that determinism - which is found in nature - would stop in front of the human brain. In other words, man is an automaton. He may believe that he's free, but he is not free. It would be like we're in a movie. We don't know who was killed, we don't know who's the killer, but somebody knows it - the person who made the movie. In some sense every action, every part of our life, of the life of the universe, is already determined by the initial conditions as they were present in the big bang. Therefore, the pleasure of being invited to this beautiful ceremony, and my friendship with Professor Ruffini, would have been included in the information at the big bang. But that seems very strange, and I could never accept this view.
The problem of time in physics and in philosophy, towards reconciliation.
But as I mentioned, the problem of time, remains
very controversial. When I was young, I asked philosophers "What is time?" And
all the philosophers answered that time is the most complex subject of human endeavour. It
is the problem of ethics, of responsibility. On the other hand, when I asked physicists
when I was young, I asked Pauli, I asked Bohr, they smiled and said, "The problem of
time has been solved by Newton, with some changes introduced by Einstein. There is no
point for a young man to enter into the study of time." But I am a very persistent
person. I have had over my lifetime very few ideas, but I have continued to work on them
for many years. In this sense I've followed the model of Einstein, who once said, "I
have very few ideas, and when I have an idea, it is very difficult to get rid of it."
So it is a fact is that for sixty years, I am working on the problem of time. What is the
astonishing point in this persistence is that in spite of the tragedies of this century,
in spite of problems in my life, I could continue for this long period, and I had the
chance to have very excellent co-workers who helped me to clarify progressively this
problem.
Reversibility and irreversibility in nature
We observe irreversibility on all levels of
observation. There are simple irreversible processes such as physical chemical processes
like heat conduction or viscosity. Every chemical reaction is an irreversible process.
Each of our thoughts is in an irreversible process. We cannot conceive life without
irreversible processes. And I believe you cannot conceive cosmology without irreversible
processes. But how to introduce irreversibility into the basic laws of physics, that is a
different problem. The two great theories of this century - quantum mechanics, and
relativity - negate the direction of time. Therefore there are two tendencies. One
tendency is to state that we introduce the direction of time by approximations which we
introduce in the basic time-reversible laws of physics. Generally these are associated to
some form of coarse-graining. Another version of the same tendency is to emphasize
"decoherence". Decoherence would come from the influence of the external world.
But what about the dynamics of the external world ? I think that both of these directions
of thought are somewhat strange. To imagine that we introduce the direction of time
through our approximations seems to be close to megalomania. We may consider that we are
the children of time, the children of evolution, but it is difficult to imagine that we
are the father of evolution. We would then be in a sense outside nature. But that is very
difficult to believe. Also the idea that cosmology would be at the origin of
irreversibility is very difficult to believe, because irreversibility appears today in
some type of systems and not in others. For example, the two-body problem (as the earth,
moon or sun) can be solved to a high approximation by time reversible laws. But, already
the three-body problem introduces some aspects of irreversibility. If there would be a
cosmological influence then it should likely act on all systems in the same way. Our
problem is to distinguish dynamical systems which are reversible from systems which
present irreversibility.
The irreversibility and the basic physics' laws
Now, let me go a little deeper into the subject.
First, let me explain why I was so convinced that we have to introduce irreversibility in
the basis of physics. My starting point was thermodynamics. I know of course that
thermodynamics is a phenomenological science. As everybody knows, the basic law of
thermodynamics is the law of increase of entropy. Now the interesting point is that
systems which are close to equilibrium and systems which are far from equilibrium, react
in a quite different way to perturbations. When you perturb a system close to equilibrium
the system goes back to equilibrium like when you perturb a pendulum. The reason is that
there are extremal principles in thermodynamics. For example, the entropy is maximum at
equilibrium, if you perturb the equilibrium, you lower the entropy, and the system reacts
by coming back to the maximum of entropy.
Irreversibility, bifurcations and history
So there is a large number of new phenomena which
are associated to irreversibility, and appear only in systems far from equilibrium. Now,
there are two aspects which I want to emphasize. The first I already mentioned, that
because of these new structures we cannot say they come from our approximations. The
second point is that because of the appearance of these structures the role of probability
becomes evident. In front of a bifurcation, you have many possibilities, many branches.
The system "chooses" one branch; if you repeat the experiment it may choose
another branch. The choice of a branch is associated to probability. In other words, the
future is not given. Once I had obtained these results, I wanted first to see if they are
not giving some insights in other domains of knowledge. For example in biology my student
who is now very well-known, Jean-Louis Deneubourg, has made very nice experiments which
impressed me very much. Imagine an ant nest, a source of food, and two bridges. You see
that after some time all ants are on one bridge. Should you repeat the experiments, they
may be on the other bridge. The mechanism is again an autocatalytic mechanism because each
ant encourages the other ants to be on the same bridge. This is a very simple example of a
bifurcation in biology. Also, human history is full of bifurcations. When we went from the
Palaeolithic Age to the Neolithic Age due to the fact that humans could explore the
resources of vegetation and of metallurgy, we may consider this as a bifurcation; even as
a bifurcation with many branches, because the Chinese Neolithic is different from the
Middle East Neolithic or the Latin American Neolithic. There are of course elements in
common, and a visitor from Egypt would find the towns of the Aztecs very similar to his
own with the temples, the palaces, the squares, and so on. In fact, one can probably say
that every time we find a new resource, material resources like coal, or immaterial
resources like electricity, the world is reorganized, and we have a bifurcation. In the
present, the world is changed by the information technology. This technology has grown at
an unexpected rate.
Science as history of nature
Let's come back to the problem of time. As I
mentioned, on all levels of observation we see a history - a cosmological history, a
biological history, a geological history. It seems that you can only understand the
structures which are around us from a historical perspective, and this historical
perspective corresponds to a succession of bifurcations. So science today emphasizes the
narrative element, becomes a history of nature: I would like to say, it becomes something
like a novel, or a story of 1001 Nights in which Scheherazade tells a story to
interrupt and tell an even nicer story, and so on, and here we have cosmology which leads
to the story of matter, then to life, and to man.
The irreversibility in the example of deterministic Chaos Now let me come to the main point of my lecture, which is how to incorporate the direction of time into dynamics. The mathematical and physical basis of our approach were definitely clarified only about five years ago, first in the frame of chaotic deterministic maps. I would like to mention that my colleague Dean Driebe has published recently a very nice book, Fully Chaotic Maps and Broken Time Symmetry, (Kluwer Academic Publishers, 1999) devoted to this subject, and you can find all of the mathematical aspects in this book, so I can be rather short. The simplest example is the so-called Renyi map. You multiply by two a number between zero and one and you every time after each operation take away what is above unity. Then you can show that two initial conditions differing as slightly as one wants give different trajectories. Now this can be described by "Newton's equations" which in the Renyi map reduce to xn+1 = 2xn (mod1). But the interesting point is that for all deterministic chaotic systems, there exists another representation for ensembles in which the central quantity is probability. The evolution operator of the ensembles can be analyzed in terms of probability, and not in terms of trajectories. How is this possible? In a famous paper Koopman has shown that as long as you remain in the Hilbert space of "nice," square integrable functions, the probabilistic description, and the description in terms of trajectories or wave functions in quantum mechanics, are equivalent. But that is only true as long as you remain in the Hilbert space. This space is a kind of generalized vector space in which there is a norm and a scaler product. But how then does it happen that you obtain here a new result in which probability cannot be reduced to trajectories, and in addition, gives broken time symmetry? It is because the evolution operator can be analyzed as it is done in quantum mechanics into eigenfunctions and eigenvalues, but the eigenfunctions are now generalized functions (called also distributions). The extension of the evolution operator outside the Hilbert space leads to a different formulation of the laws of physics, which incorporate the time symmetry breaking and in which the basic quantity is probability. Of course deterministic chaos is only a simple example; these conclusions apply to other situations, and especially to thermodynamic systems.
Irreversibility and thermodynamical systems Thermodynamic systems, as I mentioned already, are large systems in which the number of particles tends to infinity, the volume tends to infinity, and the ratio number of particles of a volume remains finite. Now it is well-known already for equilibrium thermodynamics that this leads to new phenomena, like phase transitions. If you would take a system of let's say 100 particles, there would be no well defined melting point or freezing point. The existence of these singularities is due to the thermodynamic limit, (number of particles N® ¥ , volume V® ¥ , N/V finite mean energy) and what we have shown is that irreversibility is again due to the limiting process involved in thermodynamic systems. Indeed one can show that even if you start with Hilbert space, the persistent interactions which are going on in a thermodynamic system, kick the system outside the Hilbert space. The mathematics is very simple and presented in a paper together with Tomio Petrosky (Extension of classical dynamics: The case of anharmonic lattices, I. Prigogine and T. Petrosky, in Gravity Particles and Space-Time, eds. P. Pronin and & G. Sardanashvily, World Scientific, Singapore, 1996). The evolution operator L (the Liouville -von Neumann operator) for particles has real eigenvalues inside the Hilbert space, but in general complex eigenstates (associated to relaxation time) outside the Hilbert space. That is in a somewhat simplified way, the origin of irreversibility.
The mathematics of time There is a mathematics of time. The situation is somewhat similar to gravitation which needs non euclidean geometry. We obtain outside the Hilbert space a probability distribution which can no more be expressed in terms of trajectories, and this limiting process leads to time symmetry breaking. We obtain two semigroups, one dealing with the evolution from the past to the future, the other dealing with the evolution of the future to the past. Of course we have to make the choice of one of the semigroups. In a sense this situation is similar to the problem of matter and anti-matter. There is a symmetry between matter and anti-matter, but our universe is made mainly by matter and anti-matter is only the temporary result of high-energy experiments, at least so far as we know. And here also we see again that the universe is less symmetric than we thought. The classical view was that the direction of time does not exist, that past and future playing a symmetrical role. Now we see that is not true, that the time symmetry is broken in large systems. This means of course that Newton's equations or Schrödinger's equations are not valid in the thermodynamic limit. That doesn't mean that classical mechanics or quantum mechanics are wrong; that means only that the formulation of classical mechanics or quantum mechanics has to be modified for this class of dynamical systems.
The extension of classical mechanics or quantum mechanics, example in field theory and in elementary particle physics
The extension of classical mechanics or quantum
mechanics to thermodynamic systems applies also to field theory. In field theory the
system is described by an infinite number of variables. A free field is an integrable
system; it is again a system which is time symmetrical but the situation changes radically
with interacting fields. If we take free fields such as the Klein-Gordon field or the
Dirac equation, we would have occupation numbers which would be constant. But this is not
what is observed. An excited atomic state falls down to the ground state and there exists
a large number of resonances in elementary particle physics. These aspects illustrate the
role of irreversible processes on the most fundamental level which we have at present
(excluding the string theory which still remains a controversial subject). Again the
spectral analysis of interacting fields outside of the Hilbert space lead to
semigroups with complex eigenvalues which are responsible for the appearance of unstable
particles with finite lifetimes. The conclusion that for interacting fields we have to go
outside the Hilbert space was stated by Dirac at the end of his life. He wanted to avoid
Schrödinger's equation as the Hilbert space is killed by the time evolution.
Conclusions
Let's come to the conclusions. What is the concept
of nature to which we've come? The Newtonian model of reality was that of an automaton.
Still we have a great difficulty to believe we are an automaton. The concept of nature in
quantum mechanics corresponds in some sense to the opposite view, as "reality"
would be associated to the transition from "potentialities" to
"actualities" due to our measurements. That means that the observer would
be responsible for reality. This is also difficult to imagine. Then we would play a
central role in the creation of reality. |