My interest is in
atomic and molecular physics (theoretical
chemistry, one would also say), interaction of radiation
with matter (atoms, molecules, elementary charges)
and the fundamental concepts. Numerous
subfields are encompassed by these very general areas, and it would
be greatly presumptuous of me to say that they are of equal interest
to me. My choice of interesting problems within these subfields
would appear somewhat random, as the saying goes: Not
all those who wander are lost (J.R.R. Tolkien-The
Lord of the Rings), but there is a thread that connects them.In
order to see this thread I will briefly describe early evolution
of my scientific carrier.
My interest for science started at an early age, in my early
teens, a dreamer who tried to understand the world around us. Being a dreamer
is not a sufficient condition to become a scientist, perhaps an artist, because
it is necessary to combine the dreams with hard facts and a good knowledge of
mathematics. As I learned functional analysis and classical physics I was soon
confronted with the “uncharted field”, quantum mechanics. For me it was
uncharted because at school we did not even hear the word “quantum”, let alone
to learn what it is. Having got hold of an introductory text book on the
subject I was struck by the fact that I could not understand a word of it. Not
the math but the concepts, which were totally alien to my classical experience.
Several books were consulted, but the same questions remained, which made me
conclude that it was not the fault of the books but the fault of my approach.
That was confirmed by a professor in physics department of the University, whom
I consulted
about
the meaning of quantum mechanics. His answer was the same that I heard over and
over again in later years in discussion with the colleagues all over the world:
one should renounce pictures (read classical) and accept that only the math is
the legitimate approach to analyze the physics of “small”. The secret is, so
the arguments went, that the rules of classical mechanics are derived from the
rules of quantum mechanics. Based on this observation it is still argued by
many that in the curricula of physics one should start with quantum mechanics
instead of classical. In a way these arguments were a relief for me because
manipulating math is so much easier than trying to figure out pictures of the
things that are analyzed. My efforts were therefore channeled towards learning
the subtleties of mathematical physics, forsaking the dreamer in me. The
notes
on the left from the time of my high school are the proofs that provided one
learns sufficient abstract math, and some functional analysis, it is relatively
easy to enter the field of modern physics. One only has to learn certain basic
postulates, without asking questions about their meaning.
It is no wonder that when deciding on the subject of study
the choice was elementary particle physics.
This is even nowadays a challenge for an adventurous mind because the subject
is plagued by intriguing questions, which would definitely awaken a mind of a
dreamer. Furthermore, the belief was, and still is, perpetuated, primarily by
high energy physicists, that the only true challenge to the physical principles
comes from the field of elementary particle physics and the rest is the “stamp
collecting”. My physics student days were spent in learning, besides the
obligatory courses, the subtleties of mathematical formalism of high energy
physics, being proud to be a member of the selected ones. That nobody could
understand what I was doing, except my “club-members”, I considered more of a
virtue rather than the drawback. My diploma thesis was on the weak
interactions, which at that time was the “in subject”, being at the threshold
of developments that resulted in the unification of three major interactions.
For the thesis I calculated the radiative corrections to the muon decay, a
major exercise. One of the pages of that calculation is shown in the right
figure.
The
diploma work was the crown of my “love affair” with high energy physics, of
which I was, and still am, very proud because lots of solitary hours were spent
to acquire knowledge of the field. One page of that work is in the left figure.
I should have felt grand fulfillment being at the threshold of graduation,
because I was ready to start contributing novelty into the field rather than
reading and redoing somebody else work. Yet I felt emptiness because part of me
was not involved in all these, the dreamer. I had knowledge of the facts, and
especially the math, but there were lots of questions unanswered, those who one
might characterize as “questions you always wanted to ask but were afraid to do
so”. That part of me prevailed when after graduation I got offer for PhD in
theoretical chemistry, at Sussex University.
The decision was not simple, because it was the step from the privileged club
to “stamp collecting”. In the end my instinct made decision, and never
regretted. Those questions where the thread that connects (almost) all problems
that I worked, and still working, on.
The Questions (at least some of them):
Although one accepts dualism as
the fundamental principle of matter, it is hard to acquiesce with it. The
question is not of acceptance but of fundamental logic: if the dualism is
allowed then one should also allow trialism, quadrilism, etc., depending on
what suits ones premises. I cannot see the use of similar logic in, say, the
criminal law. Nevertheless, if this is the fact of Nature then so be it, but
based on this principle it is hard to describe certain phenomena. One of them
is tunneling. I spent fruitless hours watching waves on the surface of water in
order observe something that would resemble tunneling. Electromagnetic waves
show analogous effect (total internal reflection), but it could be given
relatively simple meaning (the field instead of being a plane wave transforms
into a decaying one). Furthermore, it was not clear to me how to reconcile
manifestation on the screen of the particle property with that of wave property
to describe the interference experiment. Explanation by the collapse of the
wave function, which is the modern way of treating this phenomenon, pushes
physics into mysticism (this and other explanations of the same kind are used
as the basis for numerous mystic societies that awoke ghosts at midnight sessions - brows the internet for their locations). The
effect of similar kind is the EPR paradox, which in all frankness I did not
understand then and now. If one says that initial total momentum of two
particles is zero, and the momentum of one is measured then by the conservation
law the other is known, no matter where the two particles are located. That was
the most primitive observation of mine; later a more sophisticated one was
given. A very famous is the Aharon-Bohm effect, which my student seminar was,
supporting it very anxiously, but eventually I admitted to myself that I did
not understand it. I did not have prejudice to support either the concept of
force or potential, yet I could not figure out how is it possible that one
effects dynamics of particle and the other does not.
Anyone starting the course in
quantum mechanics is given the answer to the basic question: what makes an
atom, say hydrogen, stable. In the
standard scenario it is said that classical mechanics does not explain
stability because of the effect of the radiation reaction force on trajectory
of the electrons. On the other hand, quantum mechanics predicts stability
because the electrons have the lowest energy state. Now, this comparison is
truly unfair, because in classical mechanics one assumes radiation reaction
force whilst in the quantum one does not. Classical atom without that force is
also perfectly stable. The proof that quantum mechanics does not predict
stability of atoms is the positronium, for which one easily calculates the
ground state (and in fact it is observed) but it does not have infinite
lifetime. The orthodox elementary particle physicist would shrug off this
argument with nonchalant ease by saying that the positronium consists of
particle and antiparticle, and therefore they annihilate. However, the argument
does not explain anything, because the logic is twisted. The antiparticle is
defined as the one that annihilates with its counterpart particle, but there is
no physical explanation how and why this happens. So the question why, for
example, hydrogen atoms is stable whilst positronium is not is a mystery.
That opens a question of the
nature of annihilation, but in my opinion a more important one is about
creation of particles. Again, the answer that solves (nearly) everything is
that the effects are not surprising because of the relationship between mass
and energy, the rest mass of particles goes into the energy of the photons and
vice verse. The answer is far from being satisfactory, because the relationship
is the energy balance and not the mechanism how this happens. And the latter is
precisely physics and the former is math. The mystery is that we are used so
much on thinking that the rest mass of particles is a universal constant, and
yet in the annihilation it vanishes at the expense of the radiation field
(photons, if one prefers it). And what about the reverse process, would it be
fantastic to know the actual physics behind the annihilation/creation
processes?
One of the postulates of physics,
“whose source is deeply buried in the relativistic quantum world”, is the
relationship between spin of the particles and the statistics they obey. The
use of this relationship is enormous; it is the basis of quantum chemistry, the
theoretical description of the chemical Universe. Yet, its physical source is a
mystery, which is why it is a postulate. The question is whether such a
physical source exists, and what is the basis of it. The commutation/anti-commutation
rules for the quantum fields are definitely not it. After all, interactions
among the objects in the Universe determine the symmetries and not math, or
humans who invented symmetries.
“The most accurate theory of all
times” is how quantum electrodynamics is characterized. To a great extent this
is true, but it is presumptions to give it this absolute status. Nevertheless,
its foundations give it the status of a truly mathematical theory, which would
confirm anyone learning its basics. It has no recourse to anything that is
labeled as classical experience, not even quantum. The classical field and the
wave function become abstract mathematical objects with certain rules to
manipulate with them. Yet in the end the results are very good, “the proof of the
pudding is in the eating” as a pragmatics would say. Is this sufficient to give
the QED the status of physical theory? That question puzzled me greatly,
because, for example, annihilation cross for the electron and the positron is
calculated very accurately from the formalism that is based solely upon
calculation of certain matrix elements. In this derivation there is absolutely
no hint about the physics of this process. Why such an abstract theory gives
good results? ; “That is the question”.
A beauty in Nature is decay of the
neutron. There is a particle, an essential constituent of matter, but when left
alone it splits into fragments. A classical mind would immediately start
thinking about a model of the neutron, say an orbiting system, but indeed there
would be problems with it. The hurdle may not be insurmountable, I am not aware
that somebody spent long hours thinking of such a model, instead pragmatism
prevailed. At the time when the theoreticians start thinking about
rationalizing the decay of the neutron the QED was well established. In its
foundations are the creation and the annihilation operators, a beautiful way to
avoid any nasty questions about the nature of these processes, which were
gauged specifically for the need of three particles: electron, positron and
photon. Why not define the same operators for the other particles, and use the
same logic for them as in the QED? Indeed that what it was done, but the
problems arose. New particles had to be postulated: neutron, proton and (anti)
neutrino. However, with the simple vector current in the QED it was not
possible to reproduce the experimental data and so a general linear combination
of interactions was assumed that would do that. In the end the famous V-A
current was selected with a coupling constant that had a value not resembling
anything known at that time. Its value was much smaller than the coupling
constant for strong interactions (read nuclear forces) or electromagnetic
interaction (of course in the dimensionless units). The constant was fit to the
experimental value for the lifetime of the neutron. Because of its unique value
the fourth force of Nature was introduced, but its role was only to regulate
the decay of unstable particles. That description of the fourth force (week
force) was puzzle for me because one is accustomed to think of interactions as
regulating the whole process of encounters of particles, and not only one of
its segments, the decay. The same as saying that tunneling should be treated as
separate interaction because it gives rise to decay. Much later, when I learned
more about atomic and molecular physics, I had a comment inphysics today
about this point. Based on this abstract thinking the
whole subject of modern elementary particle physics is built upon. A useful
trick was used, however. Whenever there was disagreement with the experimental
facts it was not the V-A idea that was questioned. Instead the theory was
expended by more and more terms and parameters, when eventually the
electromagnetic interactions could be also incorporated. No wonder that was
possible because the basic mathematical formalism sprung from that of the QED.
One only needed sufficiently large number of terms and parameters that would
describe both interactions in a unified fashion.
Resonances are very intriguing
“objects”, which are either observed as decaying states or a feature in the
cross sections. Decaying states were known long before the concept of
resonances was established, they were manifested as the instability
(radioactivity) of nuclei. Rationale was given in terms of a simple model;
rearrangement of energy in a many particle system (as the nuclei are), a
process similar to dissociative cooling (evaporative cooling of a cup of tea),
but no quantitative results came out of the model. Eventually quantum mechanics
developed sufficiently to produce a different model, the decay is due
tunneling. Based on this model it was possible to give better insight into the
nature of strong (nuclear) interaction. The effect of tunneling gives rise to
another effect, the resonances, which are manifested in the cross sections if
the decaying partners are made to scatter (crudely speaking). Resonances are
characterized by a well defined energy and the energy width of their impact on
the cross section. A great theorem of quantum mechanics then says that this
energy width is simply related to the decay rate of the unstable species. That
connection is then used to understand the decay of elementary particles, and also
to discover new ones. That there are elementary particles (meaning that they
are not composed of more elementary species, the picture that prevailed at the
time of my undergraduate study) which undergo a transformation into the other
similar species was a great discovery; typical example is decay of the neutron.
Few more followed, but with a much shorter lifetime (muon, pion) nevertheless
sufficiently long lived to leave a trace in a detector. However, based on the
relationship between resonances and decaying states a mechanism was found to
discover a much more numerous family of elementary particles, with such a short
lifetime that they do not leave a trace in detector but they are observed as an
effect on the cross sections. Importance of resonances is unquestionable,
sufficiently so to study its true origins and answer few questions of great
importance. One is: should we treat short lived species the elementary
particles or manifestation of the character of interaction among few basic
elementary particles? What about the other model for decaying species, the
dissociative cooling? It was unduly neglected in all the considerations, one
reason being that it is much more difficult to analyze than tunneling (it is a
many body effect) because, for example, perturbation theory would almost
certainly fail.
Those questions sprung from my experience
in the high energy physics, and for many of them I found the answer/understanding
in atomic and molecular physics. It is not that I can now give the
answer to the problems of the elementary particles, but as the saying
“I seek not the answer but to understand the question” goes (citation
taken from the wall of a friend of mine Harry (Kroto) ) I have better
insight into them. It was precisely because of mine belief that
many fundamental problems should be analyzed from the interdisciplinary
point, I initiated the Brijuni conferences.
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