About the Author:

 

Jay R. Yablon

 

Several folks who have come to this Web Site have requested more information about my own background.  I have decided to accede to those requests.

 

I was an undergraduate at MIT (class of 1976) and double-majored in computer science and political science, with a strong minor in physics.  I then went to law school and became a patent attorney.  Professionally, I write and prosecute patent applications for inventors in a wide range of physical, mechanical, electrical, optical, and computer arts.  But I have always had a passionate interest in physics, from the standpoint of understanding the intelligence and order which animates our universe.

 

From 1976 to 1986, I spent almost all of my spare time learning particle physics and relativity as an independent research project, seeking to solve two fundamental problems: 1) understanding why the Fermions have the masses they have (per the anecdote below) and 2) finding a unification of all four interactions, which is no small project.

 

During that ten year period, I developed many "tools" toward addressing each of these two problems, but could never quite put all the pieces together.  From 1986 till late-2004, I did no physics at all.  With my wife of 28 years, we raised two children who have matured to fine young adults, and I built from scratch my patent practice which is now very successful and has helped me become reasonably-independent.  I actually had no expectation or idea that I would ever return to physics work.

 

Late in 2004, however, I found myself compelled to return to the physics work I had done 20 years earlier, with a lot more maturity and perspective than I had back in the 1970 and 1980s.  All of the pieces that I had developed from 1976 to 1986 started coming together for me.  I felt that I had the opportunity to study physics intensively for ten years with an eye toward solving the mass problem and unifying the four interactions, then “sleeping on it” for 18 years, and then coming back to everything with a wholly fresh perspective.

 

The paper on Fermion Mass Revelation in Electroweak Interactions captures my ongoing efforts to characterize the Fermion masses from theoretical principles.  For all the importance of “experimental validation,” the Fermion masses are experimental data crying out for a theoretical foundation, yet to date, we have no such foundation.  This paper seeks to lay the foundation to remedy this glaring omission in our understanding of nature.

 

The paper on Electrodynamics and the Spacetime Vacuum; and Could the Quarks Actually Be Magnetic Monopoles?, however, is nearest and dearest to me, and I will take the liberty to talk more about this work here in the hope that you will choose to read what I have to say.

 

This paper captures 10 years of work, 18 years of reflection, and several recent months of new work on the question of grand unification.  I respectfully submit, in all humility, that this paper contains what Dr. Einstein was looking for in his later years, but we just didn't have the scientific data at the time that he would have needed to complete this work.  The closest he came was in his paper on Relativistic Theory of the Non-Symmetric Field with the “surprising” finding “that the gravitational equations for empty space determine their field just as strongly as do Maxwell’s [source-free] equations in the case of the electromagnetic field.”  With this statement, Dr. Einstein was leaving some very important clues in this paper to the next generation of scientists.  I believe he wanted to say that Maxwell equations are the gravitational equations for empty space, but did not feel he could fully support that statement and so the measure of field strength was as far as he got.

 

It is dismaying to me that Relativistic Theory of the Non-Symmetric Field and the clues about unification which it contains has these days largely been dismissed, along with Reinich and Wheeler's geometrodynamic program.  I believed these were all right on target.  I am very conservative as a physicist, which is to say that I believe that in order to explain nature, one should squeeze every possible bit of physics out of the classical theories which have proven themselves over time, before introducing brand new concepts which may turn out (and often turn out) to be unnecessary.  Thus, in the same way that the Fermion Mass paper can really be thought of as “How to Stretch the Electroweak Standard Model, with Nothing Else, as Far as Possible to Reveal the Lepton Masses,  the Classical Electrodynamics paper can be thought of as “How to Stretch only Einstein’s Gravitation and Maxwell’s Electrodynamics to Unify All of Nature’s Interactions.”  Which is to say, I believe, from a very conservative viewpoint, that there is still some very significant untapped potential in these two classical theories (and in the Electroweak Standard Model) that is being widely-overlooked.

 

The first part of this paper – recognizing that Maxwell’s equations can be expressed simply as the vacuum equation Ruv=0 – is something I already discovered back in 1984, after studying Reinich and Wheeler in great detail (my original, never-published paper is in the US Copyright Office, dated 1984, but you may copy it if you wish).  I have posted a PDF scan of that 1984 paper on the page with the classical electrodynamics paper, which you can link to here as well.  (Chapter 6 has the detailed “field strength” calculation based on Einstein, which is merely summarized in one paragraph in the 2004-2005 paper.)  The problem was that this identity of Maxwell’s equations with Ruv=0 only works if there exist non-zero monopole sources, as well as third rank antisymmetric sources which I already had “predicted” in 1984, but for which I had no ready physical explanation.  In short, back in 1984, the Ruv=0 expression of Maxwell’s electrodynamics predicted certain objects, including magnetic monopoles, for which I was unable to offer a physical explanation.  I had the mathematics to unify classical electromagnetism with gravitation, but I could not explain the physics.  And so, the theory sat.

 

In late 2004, I returned to this work, and decided that a concerted effort needed to be applied to answer the question "where are the magnetic monopoles”?  By then, I of course recognized fully that Maxwell’s classical electromagnetism needed to be regarded as a U(1) subset of electroweak theory, and that the overall work needed to be considered in the context of non-Abelian field theory.  On December 1, 2004, I came upon the key insight that if one regards the strong interaction gluon fields as the Maxwell “duals” of (a not-presently-known superset of) the SU(2)xU(1) electroweak flavor fields, that the magnetic monopoles immediately become identified with point sources of color, i.e., the quarks.  This solved two long-standing problems all at once: how to interpret the dual fields which previously had no physical explanation (they are gluon fields), and why don’t we observe free magnetic monopoles (because they are color charges a.k.a. quarks and we don’t observe free quarks either).

 

Over the next couple of months, I also came to gradually realize that the mysterious antisymmetric third-rank sources I had uncovered 20 years ago seem to describe tri-colored “baryons,” in integral form over three quark-pair interactions.  What is truly fascinating about this is that even if we did not yet know about baryons containing three quarks, the three terms in Maxwell’s third-rank monopole equations, when calculated through in the context of non-abelian field theory where they don’t zero out, would lead us to find that each baryon is an integral sum over three pairwise, point source, interactions, i.e., that each baryon is a “non-point” object of some spatial extent containing three confined ”point” sources.  Thus, as a good example of the “untapped potential” in Maxwell’s electrodynamics, this means that Maxwell’s equations (written as two tensor equations in spacetime) actually “predict” baryons as we now know them today, but these were set to zero because Maxwell was working only with Abelian fields.

 

Thus, classical gravitation is unified with classical electromagnetism under the umbrella of Ruv=0, and this unification predicts certain “sources” which can only be understood by using non-Abelian fields which in turn lead to colored quarks and baryons and a further unification encompassing electroweak and strong interactions.  By carrying the unification of gravitation and electromagnetism to its logical conclusion and trying to understand the sources arising from this unification, we are compelled to include quantum electroweak and QCD strong interactions also.

 

This approach obviates the need to unify the electroweak and strong interactions as parallel groups (i.e., with some mega group encompassing SU(3)xSU(2)XU(1)), or with extra spacetime dimensions, because it is instead based on G(Flavor)  G(Color), or in duality terms, simply G  *G.  Nature, simply put, is vacuum geometry plus quantum topology, with internal flavor and color.  (No strings attached.)

 

 

 

 

 

 

 

I will always recall a particular moment during high school chemistry class, quite a few years ago, when the teacher told us that the proton mass was about 1860 times as great as the electron mass.  I naturally asked why this was so, and was surprised to find out that nobody really knew the answer.  At that moment, I took up the challenge of trying to understand why the elementary particles have the masses that they have.

 

Fermion Mass Revelation in Electroweak Interactions is an important milestone in this effort.  I appreciate any comments and suggestions you may be able to offer about this work.

 

Very truly yours,

 

Jay R. Yablon

 

jyablon@nycap.rr.com