Lithuania Latvia Estonia Kaliningrad Gdansk

Lithuania (2008)

I went in September (2008) to Vilnius to attend the 12th International Conferece on Quantum Optics and Quantum Information. As usual, I brought my camera with me and took a number of photos. I would like share some of them with you.


Hermann Minknowski (1864-1909)

Hermann Minknowski was born in Kaunas (Lithuania), and studied in Koenigsberg, Germany. After World War II, Koenigsberg became the Russian city of Kaliningrad. This city was the geographical environment for Immanuel Kant to produce his philosophy, which served as the philosophical base for Einstein. You may click on the following links for While Koenigsberg was a port city like Venice, Kaunas was in its hinterland. Here are two maps telling where they are.

The University of Koenigsberg (Albertina University) had many mathematicians interested in physics. They were particularly interested in Maxwell's equations. We are now using the form of Maxwell's equations developed there. Minkowski continued his research in those equations after he left Koenigsberg.

He was a professor of mathematics and physics at the University of Zurich, while Einstein was a student there. There he completed the proof that Maxwell's equations are covariant under Lorentz transformations. He published his result in 1908.

Is this the end of the story of the Lorentz covariance of Maxwell's equations? No. This problem was not completely settled until 1990. We shall talk about this next time.

Another important contribution Minkowski made is the Minkowski space where

is a Lorentz-invariant quantity. If we do not change the x and y variables,

We are quite familiar with the two-dimensional geometry associated with hyperbolic condition. But this geometry is still is strange to us. I am not the first one to feel in this way. It was Paul A. M. Dirac who invented the light-cone coordinate system to deal with this problem. However, the problem with Dirac was that he never draws pictures in his papers, unlike John A. Wheeler.

Let us write the above formula as

If we introduce the "light-cone" variables

the Minkowskian geometry becomes the geometry of rectangles, with u and v for two perpendicular sides. If the area of the rectangle remains constant, one side becomes contracted when the other side expands. This is the geometry of squeeze.

I learned this geometry during my high-school years. Since 1973, most of my papers are based on this squeeze geometry. This geometry is not only useful for Lorentz-boosted particles, but also provides the basic mathematical language for optical sciences.


copyright@2008 by Y. S. Kim, unless otherwise specified.
The portrait of Hermann Minkowski is from http://library.thinkquest.org/05aug/01273/whoswho.html.

This page was constructed by Y.S.Kim whose home page is

  • http://ysfine.com/home.

    Lithuania Latvia Estonia Kaliningrad Gdansk


    Photos from Riga (June 2010)



      Impressed? Come to me!
      In reality, the second photo was taken first. This is how I can make a story by re-arranging photos.

    Sergei Eisenstein.

    Eisenstein's Background in Riga

      If anyone has a distinctive new idea, it is usually a product of his/her childhood environment. For instance, Kant's philosophy was based on the geographical condition of Koenigsberg (now Kaliningrad) where Kant spent 80 years of his entire life. Here is my webpage dedicated to this subject.

      Eisenstein could not be an exception. In order to find out what environment he had during his early years, I went in June of 2010 to Riga (Latvia) where he was born and raised. While talking with Latvians there, I learned that his father came from Saint Petersburg and became a very prominent architect. There are still some beautiful buildings designed by him. Great! I went to those buildings and could see immediately how Eisenstein became so creative.

      To make a long story short, let us look at one of those buildings designed by his father.

    • This architect of course had his reasons to bring many things from different places. However, his design forces us to think beyond what we see. The architect was Sergei Eisenstein's father.

      Very definitely, Sergei was strongly influenced by his father. He looks at the photos he has taken, and then thinks carefully about what idea he could produce from those photos. This is what Eisenstein's creativity is all about.

      Let us translate this into your issue. You have published many papers in the past. Look at them again, and try to construct a new idea from them.

      Eisensteinism does not end here. Humans from their beginning had a habit of looking at the stars during the night and made attempts to make sense out of them. We still carry this habit of watching the sky. We do cosmology, black holes, dark matter, gravitational waves, and many more to come.

      Click here for an article about STEP 2.

    • By 1500 AD, humans observed that some of those heavenly objects follow elliptic or hyperbolic trajectories. Isaac Newton then wrote down a second-order differential equation for both.

      In quantum mechanics, this translates into running waves and standing waves. Here again, Erwin Schroedinger's second-order differential equation takes care of this problem. The question then is how to deal with this problem in Einstein's Lorentz-covariant world. Click here for further discussion.

    • As for the geometry of ellipse and hyperbola, ancient Greeks came up with the using a circular cone. This cone contains both ellipse and hyperbola.

      When I was 15 years old, I learned that the equation

        A x 2 + B y2 = Constant

      can produce both ellipse and hyperbola, and is as good at the circular cone used by those Greeks.

      If this equation looks too childish to you, you can consider a two-by-two unimodular matrix with real elements. It has three independent parameters, but it can be brought to an equi-diagonal form by a rotation. Then the matrix has two independent parameters and takes one of the following three forms.

      The first matrix is a squeezed rotation matrix, and is therefore for an elliptic orbit. The second matrix is for a hyperbolic orbit. The third is for a linear orbit. If we construct a four-by-four matrix, it will be quadratic in the parameter, and thus represent a parabolic orbit.

      The question then is whether these three matrices can be combined into one analytic matrix. The answer is Yes. We can use the mathematical technique called the Bargmann decomposition to combine all three of the above matrices into one expression, given as

      Indeed, this matrix is analytic in both \lambda and \theta variables in the entire applicable region. The boundary between ellipse and hyperbola is given by the diagonal line.

      What I said above is strictly about mathematical aspect of two-by-two matrices. However, it is applicable to at least two important branches of modern physics.

      1. Optics (both quantum and classical) is largely a physics of two-by-two matrices (or ABCD matrices) and Fourier transformations. Click here for two-by-two matrices in optics.

      2. In 1939, Eugene Wigner published his paper on the little groups which dictate the internal space-time symmetries of particles in the Lorentz-covariant world. The three equi-diagonal matrices given above serve as the basis for Wigner's little group.

        Wigner always wanted to translate his 1939 paper into the language of two-by-two matrices. It appears that Wigner's little groups emerge from this simple mathematical property of the two-by-two matrix.

      3. There are many other branches of physics I am not competent to speak about. However, solutions are possible only if the problems are brought into the form of harmonic oscillators or/and two-by-two matrices, since otherwise they cannot be solved.

      I made the above conclusion by looking at the many of my past papers, as Sergei Eisenstein constructed new stories based on the photos he took. Many people complain that my papers contain only two-by-two matrices, ellipses, and hyperbolas. But they cannot complain about what I said above.

    • So far, we have been treating ellipse and hyperbola as different curves. I am not satisfied with this observation. I am interested in whether the hyperbola and ellipse are the same thing. For this purpose, let us write another baby formula, namely

        x2 - y2 = (x + y) (x - y) .

      If (x2 - y2) remains constant as in the case of hyperbola, (x - y) should become smaller as (x + y) becomes large. This means that there is an ellipse for each point on the hyperbolic trajectory.

      In 1962, I had an audience with Paul A. M. Dirac. He told me to study the contents of Lorentz covariance. Since Dirac told me so, I had to read his papers. His papers are like poems, but they do not contain figures. Thus, I decided to translate his poems into one picture. On this project, I have been working with Marilyn Noz since 1973. You may click here for our latest paper on this subject.

      I already talked too much about myself. I could talk more, but I should stop here. I took many photos while in Riga. I have placed some of them on this webpage, and will place more when I have time. Let us look at those photos.

    Lithuania Latvia Estonia Kaliningrad Gdansk


    Estonia










    copyright@2010 by Y. S. Kim, unless otherwise specified.

    Click here for his home page.