Lab Notes for a Scientific Revolution (Physics)

June 15, 2013

Slides from my first Physics Lecture, and a New Draft Paper Summarizing the Experimental Points of Contact which Affirm my Work

This past week I gave my first physics lecture on the research in my recent four published papers establishing that proton and neutrons are actually a particular type of magnetic monopole (based on a theory called Yang-Mills because those are the names of the two fellows who invented its foundations).  In the lecture, I consolidated all four of my papers totaling about 140 pages into a 70 minute lecture (50 minutes talk, 20 minutes Q&A discussion) and 64 slides which you can download from Physics Lecture Slides.

It would probably take someone a couple of weeks to read through and thoroughly understand my four papers.   The slides were designed to allow someone to assimilate the same information within a couple of hours.  Please take a look.

Also, I prepared a new paper which you may read at Fitting the 2H, 3H, 3He, 4H Binding Energies 3  which in ten pages lays out the multiple relationships I have found which very clearly connect to experimental data that had never before been explained.  This is the “tip of the iceberg” in terms of the multiple ways in which nature herself validates my theoretical work at the parts-per-million level.   My hope is that people in the physics community will see these results, realize that there is something real here, and then take the time to backtrack to understand the theoretical foundations that got me to that point.  A sort of “inversion” of my work to lead with the experimental results in order to catalyze interest.  Everything in this paper by the way, is simple arithmetic (as in, numbers calculated and compared to other numbers), and about the only complexity is that you need to understand a tiny bit about matrix multiplication (like that the “Trace” of a square matrix is just the sum of all the entries long its upper left to lower right diagonal).  If you do not want to even sort through the matrix stuff, then just look at equations (14) through (20).  These are pure numbers, and you will see how close I get to the experimental data each and every time.  Nobody has ever before explained this experimental data with such high precision!

People, I am usually careful not to toot too loudly about my work.  But I have to say that this is real, it is fundamental, and it will revolutionize nuclear and particle theory.  The question is no longer if, but when.  The discoveries have been made and they are in print and all they need is attention from the right places.  My “lab notes” and related work will soon spark a “scientific revolution” toward which I have been working for over 40 years.  Real results in hand, I am now doing all that I can to make that happen sooner rather than later.  I welcome any help or support my friends can provide in making that happen.


March 17, 2013

My first published paper “Why Baryons Are Yang-Mills Magnetic Monopoles” at Hadronic Journal, Volume 35, Number 4, 399-467 (2012)

My first paper “Why Baryons Are Yang-Mills Magnetic Monopoles” has now been published in Hadronic Journal, Volume 35, Number 4, 399-467 (2012). Though the Hadronic Journal has not yet put this issue online, I have a hardcopy of this and have uploaded a scan at the link below:

Hadronic Journal, Volume 35, Number 4, 399-467 (2012)

As I have advised on some earlier blog entries, I have two more accepted papers which will be published next month (April 2013) in the Journal of Modern Physics, Special Issue on High Energy Physics.


December 13, 2012

Accepted for Publication: Why Baryons Are Yang-Mills Magnetic Monopoles!

I am very pleased to report that the paper linked below, “Why Baryons Are Yang-Mills Magnetic Monopoles,” has been accepted for publication in Number 4, Volume 35, 2012 pp 401-468 of the Hadronic Journal.  This is due to be released in early January, 2013.

Why Baryons Are Yang-Mills Magnetic Monopoles Final for Publication

As you can see from elsewhere in this blog and in my various newsgroup posts, I have been advocating since 2005, the view that protons and neutrons and other baryons are Yang-Mills magnetic monopoles.  In this paper, I have finally developed the empirical proof, by predicting nuclear binding energies between such monopoles which accord with empirical binding data within a fraction of a percent, and by explaining how the nuclear binding energies relate to the energies which confine quarks within their respective nucleons.

If you want to start somewhere other than at the beginning, go to page 61 where you will see how I derive the up and down quark masses to six digit in MeV accuracy based on the electron rest mass and the deuteron binding energy, and where I show a predicted maximum available binding energy for ^56Fe of 493.028394 MeV.  The empirical data show that this nucleus has an empirical binding energy of 492.253892 MeV, which means that ^56Fe utilizes 99.8429093% of the energy predicted to be available, for actual binding.  The remaining 0.16% is used to continue to confine quarks within the nucleons that comprise ^56Fe, and this utilization of available binding energy is the maximum among all of the known nuclei, and sets the boundary between fusion and fission physics.

I believe that this will become big news as this work gains exposure and people begin to see what problems have been solved here.

Happy holidays to all!


April 22, 2012

Back to Blogging, Uploaded a paper I wrote in 1986 about Preonic Grand Unification

It has been almost 3 years since my last Blog post.  Much of my time has been diverted into a condo hotel project in Longboat Key Florida, and the focus I need to do good physics has been impossible to come by.  Then, the other day, Ken Tucker, a frequent participant at sci.physics.foundations, emailed me about some new research showing that electrons have constituent substructure.  That brought me back immediately to the half a year I spent back in 1986 developing a 200-page paper about a preonic substructure for quarks and leptons, which culminated six years of study from 1980 to 1986.  I finished that paper in August 1986, and then took an 18 year hiatus from physics, resuming again in late-2004.

Ken’s email motivated me to dig out this 1986 paper which I manually typed out on an old-fashioned typewriter, scan it into electronic form, and post it here.  Links to the various sections of this paper are below.  This is the first time I have ever posted this.

Keep in mind that I wrote this in 1986.  I tend to study best by writing while I study, and in this case, what I wrote below was my “study document” for Halzen and Martin’s book “Quarks and Leptons” which had just come out in 1984 and was the first book to pull together what we now think of as modern particle physics and the (then, still fairly new) electroweak unification of Weinberg-Salam.

What is in this paper that I still to this day believe is fundamentally important, and has not been given the attention it warrants, is the isospin redundancy between (left-chiral) quarks and leptons.  This to me is an absolute indication that these particles have a substructure, so that a neutrino and an up quark both have contain the same “isospin up” preon, and an electron and a down quark both contain the same “isospin down” preon.  Section 2.11 below is the key section, if you want to cut to the chase with what I was studying some 26 years ago.  I did post about this in February 2008 at, though that post merely showed a 1988 summary I had assembled based on my work in 1986, at the behest of the late Nimay Mukhopadhyay, who at the time was teaching at RPI and had become a good friend and one of my early sources of encouragement.  This is the first time I am posting all of that early up-to-1986 work, in complete detail.

Lest you think me crazy, note that seventeen years later, G. Volovik, in his 2003 book “The Universe in a Helium Droplet,” took a very similar tack, see Figure 12.2 in this excerpt: Volovik Excerpt on Quark and Lepton Preonic Structure.

The other aspect of this 1986 paper that I still feel very strongly about, is taking the Dirac gamma-5 as a fifth-dimension indicator.  I know I have been critiqued by technical arguments as to why this should not be taken as a sign of a fifth dimension, but this fits seamlessly with Kaluza Klein which geometrizes the entirely of Maxwell’s theory and is still the best formal unification of classical electromagnetism and gravitation ever developed.  For those who maintain skepticism of Kaluza-Klein and ask “show me the fifth dimension,” just look to chirality which is well-established experimentally.  Why do we have to assume that this fifth dimension will directly manifest in the same way as space and time, if its effects are definitively observable in the chiral structure of fermions?  Beyond this, I remain a very strong proponent of the 5-D Space-Time-Matter Consortium, see, which regards matter itself as the most direct manifestation of a fifth physical dimension.  Right now, most folks think about 4-D spacetime plus matter.  These folks correctly think about 5-D space-time-matter, no separation.  And Kaluza-Klein, which historically predated Dirac’s gamma-5, is the underpinning of this.

After my hiatus of the past couple of years, I am going to try in the coming months to write some big-picture materials about physics, which will pull together all I have studied so far in my life.  I am thinking of doing a “Physics Time Capsule for 2100” which will try to explore in broad strokes, how I believe physics will be understood at the end of this century, about 88 years from now.

Anyway, here is my entire 1986 paper:

Preonic Grand Unification and Quantum Gravitation: Capsule Outline and Summary

Abstract and Contents

Section 1.1: Introduction

Section 1.2: Outline and Summary

Section 2.1: A Classical Spacetime Introduction to the Dirac Equation, and the Structure of Five-Dimensional Spacetime with a Chiral Dimension

Section 2.2: Particle/Antiparticle and Spin-Up/Spin-Down Degrees of Quantum Mechanical Freedom in Spacetime and Chirality, Gauge Invariance and the Dirac Wavefunction

Section 2.3: Determination and Labeling of the Spinor Eigensolutions to the Five-Dimensional Dirac Equation, and the High and Low Energy Approximations

Section 2.4: The Fifth-Dimensional Origin of Left and Right Handed Chiral Projections and the Continuity equation in Five Dimensions: Hermitian Conjugacy, Adjoint Spinors, and the Finite Operators Parity (P) and Axiality (A)

Section 2.5: Conjugate and Transposition Symmetries of the Dirac Equation in Five Dimensions, the Finite Operators for Conjugation (C) and Time Reversal (T), and Abelian Relationships Among C, P, T and A

Section 2.6: Charge Conjugation, and the Definitions and Feynman Diagrams for “Electron” and “Positron” Spinors

Section 2.7: Simple Unpolarized s,t,u Scattering Channels with a Covariant Propagator, and the Covariant (Real and Virtual) Polarization States of Massive and Massless Vector Bosons

Section 2.8: Prelude to Preons: The Spinor Decomposition of Four Real Spacetime Dimensions ct,x,y,z into Two Complex Spinor Dimensions Using the Covariant Polarization States of Vector Bosons

Section 2.9: Introduction to Isospin Preons in Electroweak Theory: The Preonic Decomposition of Four Real Electroweak Bosons A, W+, W-, Z into Two Complex Preons Denoting “Isospin Up” and “Isospin Down”

Section 2.10: Summarization of Prior Discussion, and on the Fundamental Importance of Preons in Particle Physics

Section 2.11: The Four-Preon Flavor SU(4) Unification of the Electromagnetic, Weak and Colorless Strong Interactions Excluding Quantum Gravitation; and the Colorless Flavor Classification of Left Handed Real Fermion and Boson Chiral Projections, for a Single Fermion Generation

Section 2.12: The Four-Preon Flavor SU(4)xU(1) Unification of Electromagnetic, Weak, Colorless Strong and Quantum Gravitational Interactions; and the Colorless Flavor Classification of Left and Right Handed Real Fermion and Boson Chiral Projections, for a Single Fermion Generation

Addendum to Section 2.12

Section 2.13: The Six-Preon Unification of Flavor SU(4)xU(1) with High Energy Color SU(4)xU(1) and Two Overlapping Degrees of Freedom; the Flavor and Color Classification of Real Fermions and Vector Bosons for a Single Generation; and the Derivation of Electroweak and Strong/Hyperweak Massless and Massive Neutral Current Vector Bosons

Section 2.14: On the Replication of Fermion Generations: Four Generational Grand Unification with Eighteen Preons and Nine Independent Flavor/Color/Generation Degrees of Freedom, and a Preonic Discussion of Mesons and Meson Decay

References and Bibliography

December 26, 2008

S=2, mu=0 Meson Mass Spectrum, and some interesting possible ties to experimental meson data

Before I head out on holiday, I also wanted to post one more item:

In equation (11.8) of my earlier post at:

I showed the matrix inverse for mesons based on the values of S=2 and mu=0 using the parameters of the theory developed in that work (which is based on the post I made a few hours ago).

I finished a detailed calculation of the predicted meson masses as a fraction of “.5vg” and put them in ascending order, in the following one-page listing:

This is the type of theoretical result that we need to try to fit to experimental meson masses.  That is, this is where the “rubber meets the road.”

In this regard, I point that there are good reasons from the underlying theory to compare and take the ratios of numbers in the above with the 1+/-i factors, and to consider the SU(3) vector to be (uds) from the old quark flavor models (as opposed to the (RGB) of color).

One of these ratios is that of what is the 4,5 mass matrix element to the 1,2 element:


and this should be related to the ratio of the meson K^0=d s-bar to pi^0=d d-bar.  That experimental ratio is, in fact:

K^0/pi^0 = 497.614 MeV / 134.9766 MeV = 3.6867

This is *very* close (they differ by 1.5 parts per thousand!), and could be an experimental validation of the whole theory, since the only thing not accounted for theoretically are QED corrections!

Another ratio of interest is:


This is because the experimental pi^+/- to pi^0 ratio is:

 pi^+/- / pi^0 = 139.5701 MeV / 134.9766 MeV = 1.0340

This also is rather tantalizing, and is off by just under 2 parts per thousand!

Still trying to figure out the whole fit, but I’ll leave you all with that for now.

Happy new year!


February 7, 2008

Lab Note 3, Part 2: Unification of Particle, Nuclear and Atomic Phenomonology

This lab note will be brief.

On April 28, 2007, I posted a paper which went from baryons and confinement to strings to particle phenomenology to atomic physics and deuterons and a whole range of phenomenology including fermion generation replication which appeared to lend itself to a common, underlying explanation based on the work I have previously discussed with respect to baryons and confinement in particular.  The underlying thread throughout, is to connect spacetime symmetry to internal symmetry using the Pauli fermionic exclusion principle.   I am afraid, however, that this paper may have been buried amidst all of the other postings, so I want to specifically call it to your attention, at the link below:

On The Natural Origin of Baryons, Short-Range Mesons, and QCD Confinement, from Maxwell’s Magnetic Equations for a Yang-Mills Field

In the spirit of “Lab Notes” which are a scientific diary of theoretical explorations, I ask you in particular to look at the second half of this paper, starting at section 6.  In football, there is something known as a “Hail Mary” pass where the quarterback throws the ball all the way down the field hoping for a touchdown.  The second half of the above paper is just that.  While certainly speculative, it seems to me that this ties together a very diverse range of observable phenomenology which has not previously been tied together.   It is probably the most audacious piece of physics writing I have done, and I don’t want it to get lost in the shuffle.

So, if nothing comes of it, so be it.  But, it may well be that someone in the end zone will catch this long pass, and physics will come to rest in a different place from where it rests today.  That is why it is so important to take good lab notes!

February 2, 2008

Lab Note 4: An Interesting Left-Chiral Muliplet Perhaps Indicative of Preonic Structure for Fermions

I return in this brief Lab Note to the underlying spirit of one of the basic premises of this Weblog, which is that these are a series of “Lab Notes.”  We often tend these days to think and speak about “theories,” rather than “notes,” and certainly, many of the “Lab Notes” which I am presenting here are intended to be thought of as “theories,” or “theories-under-development,” as much as “lab notes.”

But when one talks about “Lab Notes,” what should be the prevailing thought is that sometimes, in the course of research, one uncovers an interesting “data point.”   Perhaps that data point goes nowhere; perhaps, when one looks hard at that data point and follows it up carefully, it leads in a whole new direction and changes many things in physics.

It is in this spirit that I present Lab Note 4, “An Interesting Left-Chiral Muliplet Perhaps Indicative of Preonic Structure for Fermions,” which I offer in the spirit of an interesting theoretical “data point” I uncovered back in 1988.  No more, no less.

For some history, I had been auditing some physics courses at nearby Rensselaer Polytechnic Institute (which my daughter Paula is now attending as a Freshman Chemical Engineer), and in the course of my studies there began a dialogue and I later became friends with the tragically-late Professor Nimai Mukhopadhyay, who was a particle physicist. 

At the time, particularly because of the “isospin redundancy” between quarks and leptons — which is my way of saying that both quarks and leptons can exist in both an “isospin up” and an “isospin down” state — I began to realize that there are really two distinct “attributes” which specify the “flavor” of an “elementary” fermion, within each generation.   First: is it a “quark” or a “lepton”?  Second, is its isospin “up” or “down.”  And, this, I began to suspect, was indicative of a preon substructure for the fermions — part of which provided the quark versus lepton aspect of flavor, the other part of which provided the up versus down isospin aspect of flavor. 

Following this thinking, I found that if one were to consider the flavor quantum numbers for only the left-chiral fermions, it turned out that the simple gauge group SU(4) could be used to represent the flavor symmetry of these left-chiral fermions, and that four preons, simply, A, B, C, D so as to avoid any preconceptions at all, could be used in pairs so as to construct the left-chiral fermion flavors.  I wrote this up for the 1988 “Excited Baryons” conference at RPI, and Dr. Mukhopadhyay included the writeup with the conference program.  For your consideration as a “lab note,” i.e., as an interesting piece of research data to keep in one’s mind, I link to a copy of that 1988 writeup below:

Left-Chiral Flavor Muliplet 

At this point in time, 20 years later, it is clear to me that I am not the only person to have thought in this way.  For example, G. Volovik, in his 2003 book “The Universe in a Helium Droplet,” includes an excellent discussion in section 12.2, which I have uploaded to the following link:  

Volovik Excerpt on Quark and Lepton Preonic Structure

Volovik makes a separation very similar to what I was going after in 1988, does so very clearly, and also, nicely handles the right-chiral states which drove me to fits back in 1988.  In fact, this excerpt from Volovik is another very important “lab note,” in and of itself, and I commend it to the reader.   The main problem which I perceive with this excerpt from Volovik, however, is his handling of the spins, which motivates the use of “holons” (spin 0) and “spinons” (spin 1/2) to construct a spin 1/2 fermion out of two preons.  In my view, it would be preferred for each of these preons to have spin 1/2, and when combined, for the resulting particle to also have spin 1/2.  That is, we need to find a way to have 1/2 = 1/2 + 1/2.

How we do this is another story which utilizes the fact that a fermion is a four-component Dirac spinor, and that left- and right-chirality each occupy two of the four components.  Thus, for the left- and right-chiral components of a fermion f, each of which has spin 1/2, one can combine those into the whole four-component fermion — which still has spin 1/2.  That is, f=f_{L}+f_{R} may be a way to implement 1/2 = 1/2 + 1/2 within the context of Volovik, thereby avoiding the seemingly-artificial (to me) holons and spinons.  But, that is a topic for another lab note, and this f=f_{L}+f_{R} approach clearly exploits pre-existing chiral properties of fermions. 

In any event, please take a look at my 1988 publication linked above, look also at the linked Volovik excerpt, think about his and my separation of the fermion flavor attributes into quark/lepton and isospin up/down, think about the inelegance of using holons and spinons (at least if you and I have the same sense of elegance), and think about the chiral properties of fermions.  I do continue to believe the believe that the clearly-established “isospin redundancy” between quarks and leptons is the best evidence we have, of a preonic substructure for fermions which is waiting to be better understood, and cast into a suitable formal pedagogical structure.

That concludes this lab note.

January 28, 2008

Lab Note 3, Part 1: Yang Mills Theory, the Origin of Baryons and Confinement, and the Mass Gap

(You may download this Lab Note in a PDF file at: qcd-confinement-handout-10.pdf)

This is part 1 of a Lab Note dealing with the origin of baryons and confinement in Yang-Mills theory, and attempting to lay the foundation for a solution to the so-called “Mass Gap” problem.  I have organized this into eight brief, bite-sized sections.

  1.  What Makes Yang-Mills Gauge Theory Different from an Abelian Gauge Theory like QED?

    In an Abelian Gauge Theory such as QED, a field strength two-form F={\tfrac{1}{2!}} F^{\mu \nu } dx_{\mu } \wedge dx_{\nu } =F^{\mu \nu } dx_{\mu } dx_{\nu } is expressed in terms of a potential one-form A=A^{\mu } dx_{\mu } for a field of vector bosons, in this case photons, using the compact language of differential forms, as:   

F=dA, (1.1) 

where dA=\partial ^{\mu } A^{\nu } dx_{\mu } \wedge dx_{\nu } =\left(\partial ^{\mu } A^{\nu } -\partial ^{\nu } A^{\mu } \right)\, dx_{\mu } dx_{\nu } \equiv \partial ^{[\mu } A^{\nu ]} dx_{\mu } dx_{\nu } .

    In Yang Mills theory, also known as non-Abelian gauge theory, there is an extra term in the field strength, and in particular, if the vector potential one-form is now G=G^{\mu } dx_{\mu } , then:   

F=dG+igG^{2} , (1.2) 

where G^{2} =\left[G,G\right]={\tfrac{1}{2!}} \left[G^{\mu } ,G^{\nu } \right]dx_{\mu } \wedge dx_{\nu } =\left[G^{\mu } ,G^{\nu } \right]dx_{\mu } dx_{\nu } , and g is the group “running charge” strength.     

The only difference is the existence of this extra term igG^{2} ! (more…)

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