According to a14 July 2006 Fox News article by Bill O'Reilly:
"... we have ... Iran ... developing nuclear weapons and provoking war in the Middle East. ... Iran is behind the terror attacks on Israeli forces. The whole thing is part of World War III ... Iran is protected by China and Russia. ... China wants Iranian oil. ...".
According to abacktoislam web page with map, Iran's dominant religion, ShiaIslam (dark green),
is concentrated in the oil-rich Persian Gulf. Russian and Chineseproblems with Islamic terrorism are in Sunni regions (light green),so a China-Russia-Iran policy of securing Shia Persian Gulf oil andsimultaneously suppressing Sunni dissidents in Russia and China wouldbe consistent with the interests of all three countries as well asthe other members of the Shanghai Cooperation Organization ( SCO).
According to a14 July 2006 WorldNetDaily article:by Jerome R. Corsi:
"... Iran's war to remove Israel from the Middle East has begun. ... This week, that World War has entered a shooting phase. ... Iran has given its surrogate terrorist organizations, Hezbollah and Hamas, operational orders to launch rocket attacks on Israel, in part to create enough chaos that the diversion would take international pressure off Iran. Now that Israel has decided to return fire, the Jewish state has no alternative but to win. ...Iran knows that no serious sanctions will ever emerge from the Security Council, not as long as Russia and China remain permanent Security Council members.
Last year, Russia sold Iran a $1 billion TOR-M1 mobile missile defense system that Iran plans to deploy around their nuclear installations.
China has also concluded a $600 billion oil and natural gas deal with Iran that should make Iran the leading supplier of oil and natural gas to China for decades to come.
Meanwhile, below the radar of public awareness in the U.S., Russia and China have moved to make their Shanghai Compact a mutual defense pact, not just an economic trading agreement. ...
Last month, Iran's Ahmadinejad traveled to Shanghai to join Russia and China in their most recent round of Shanghai Compact discussions. ...
The United States and Israel have no doubt that Iran is proceeding with a nuclear weapons program. The Eros-B satellite Israel has positioned in an orbit that circles over Iran ... observed ... the systematic delivery into Natanz of centrifuge parts that can be assembled underground, advancing Tehran's goal to have 3,000 of the most sophisticated centrifuges in the world operational, enriching weapons-grade uranium right now.
Ahmadinejad believes that the world is at a historic moment when Israel might ... be destroyed ...
will ... the end game in the Middle East ... involve a worldwide nuclear conflict pitting the U.S. against Russia and China. ...[ ? ]...
The only certainty in this unstable scenario is that Israel has decided it is now time to go to war, regardless what anyone in the world thinks, including President Bush. ...".
The timing of this world crisis seems to be consistent withTerrence McKenna's 2007 Timewave Peak:
According to a 14 July 2006 Telegrapharticle by Edmund Conway:
"... Laurence Kotlikoff ...[in]... research ... for the Federal Reserve Bank of St Louis, a leading constituent of the US Federal Reserve said that, by some measures, the US is already bankrupt. ... According to his central analysis, "the US government is, indeed, bankrupt, insofar as it will be unable to pay its creditors, who, in this context, are current and future generations to whom it has explicitly or implicitly promised future net payments of various kinds''. ... The total fiscal gap could be ... $65.9 trillion ... because President George W Bush has made major tax cuts in recent years, and because the bill for Medicare ... and Medicaid ... will increase greatly due to demographics. ... One solution is an immediate and permanent doubling of personal and corporate income taxes. Another is an immediate and permanent two-thirds cut in Social Security and Medicare benefits. A third alternative ... would be to immediately and permanently cut all federal discretionary spending by 143pc. ...If investors lose confidence in the US's future, and suspect the country may at some point allow inflation to erode away its debts, they may reduce their holdings of US Treasury bonds. ...".
A happy note is that the USA can be self-sufficient in food, butwith nothing (beyond Mickey Mouse) to trade for manufactured goods,it may have to make do with what it now has. In other words, the USAmay have to live with 2000-vintage manufactured goods kept in repairby chewing gum and paper clips, much as Cuba has had to live with1950-vintage automobiles.
A People's Archiveinterview with Freeman Dyson (number 78) discusses Dyson's work onQED showing the equivalence of the Feynman and Schwinger approaches.Dyson wanted to show Oppenheimer and the Princeton IAS the QEDsuccess. Oppenheimer's reaction reminds me of the attitude of thesuperstring establishment toward alternative models (including mine).Here are some excerpts from interview 78 with Dyson:
"… we met Oppenheimer and I wanted to talk about this in the seminar at the Institute … Oppenheimer wasn't enthusiastic at all. It came as a big shock to me that we'd done this wonderful stuff and I desperately wanted to tell Oppenheimer about it, that was the whole point in coming to Princeton. And Oppenheimer just brushed us off and said, "Well, you know, that's not leading anywhere,' …… This is of course a common situation; that the people who have failed to clean up a subject then don't believe that it can be cleaned up … And then if somebody comes along and says, "Look, it works," they don't believe.
So that was how it was, and so we had a very hard time to get Oppenheimer's attention. …
All the old people … including Max Born and Heisenberg and Schroedinger … had radical proposals which turned out to be totally useless …
Feynman … and … Schwinger .. and … I were conservative in the sense that we … actually made the mathematics work and got the right answers. And that came a surprise to Oppenheimer. It was very hard for him even to listen to it. …
finally Uhlenbeck interceded with Oppenheimer … "Let's listen to Dyson," and so Oppenheimer put on a seminar series for me …".
The "totally useless ... radical proposals" of Born, Heisenberg,and Schroedinger remind me of superstring theory.
Sadly, it seems that today there is no Uhlenbeck who will listento alternatives that work.
Oppenheimer's arrogant intolerance of physics views differing fromhis own was further illustrated by his statement ( acting as thethen-current Pope of Princeton's IAS ) about David Bohm'sinterpretation of Quantum Theory:
The source of that quote was Max Dresden (in my opinion impeccablyhonest) and The Bohm biography Infinite Potential, by F. David Peat(Addison-Wesley 1997),page 133. Here are some relevant excerpts fromthat book:
"… Max Dresden … read Bohm's papers … errors were difficult to detect … von Neumann's "proof" … did not rule out the sort of theory that Bohm had proposed. … Oppenheimer [said]…"We consider it juvenile deviationism … we don't waste our time …" [by] actually read[ing] the paper …Dresden … present[ed] Bohm's work in a seminar to the Princeton Institute …
The reception he received came as considerable shock to Dresden. Reactions to the theory were based less on scientific grounds than on accusations that Bohm was a fellow traveler, a Trotskyite, and a traitor. It was suggested that Dresden himself was stupid to take Bohm's ideas seriously. … all in all the overall reaction was that the scientific community should "pay no attention to Bohm's work" … Abraham Pais also used the term "juvenile deviationism". Another physicist said that Bohm was "a public nuisance" …".
It seems that the silent treatment plus ad hominem attacks hasused by the USA physics community against non-conformists for atleast 50 years.
This simplified expository overview is based on July 2006 e-maildiscussion with Ark Jadczyk.
0 - I start with the emergence from the void of a binary choice,like Yin-Yang, which naturally gives a real Clifford algebra, so thatphysics is described by a very large real Clifford algebra (ageneralized hyperfinite II1 von Neumann factor).
Then:
1 - due to real Clifford periodicity it is reducible to Cl(8)tensor product factors (in this message I will ignore sometechnicalities like signature), so Cl(8) describes physicslocally.
2 - Cl(8) vector spacetime is octonionic, and Spin(8) bivector isthe Lie algebra of the physics gauge group, with a Lagrangian (forthis message just looking at spacetime and gauge bosons and ignoringspinor fermions etc)
THIS IS THE FIRST APPEARANCE OF THE IDEA OF THE FORCE STRENGTHBEING MADE UP OF TWO PARTS:
AND
the relevant symmetric space manifold of gauge group localaction.
3 - At low (where we are) energies a specific quaternionicsubmanifold freezes out, splitting the 8-dim spacetime into a 4-dimphysical spacetime plus a 4-dim internal symmetry space.
4 - ignoring for this exposition details about the 4-dim internalsymmetry space, and ignoring conformal stuff (Higgs etc), the 4-dimspacetime Lagrangian gauge boson term is:
the integral over spacetime as seen by gauge boson acting globallyof the gauge force term of the gauge boson acting locally for thegauge bosons of each of the four forces:
Look at the basic Lagrangian of a gauge theory model:
In the conventional picture, for each gauge force the gauge bosonforce term contains the force strength, which in Feynman's picture isthe probability to emit a gauge boson, in an explicit ( like g |F|^2) or an implicit ( incorporated into the |F|^2 ) form.
Either way, the conventional picture is that the force strength gis an ad hoc inclusion.
but
to construct the integral such that the force strength emergesnaturally from the geometry of each gauge force.
To do that, for each gauge force:
1 - make the spacetime over which the integral is taken bespacetime AS IT IS SEEN BY THAT GAUGE BOSON, that is, in terms of thesymmetric space with GLOBAL symmetry of the gauge boson:
2 - make the gauge boson force term have the volume of the Shilovboundary corresponding to the symmetric space with LOCAL symmetry ofthe gauge boson. The nontrivial Shilov boundaries are:
The result is (ignoring technicalities for exposition) thegeometric factor for force strength calculation.
Each force is related to a gauge group:
GLOBAL:
Each gauge group is the global symmetry of a symmetric space
LOCAL:
Each gauge group is the local symmetry of a symmetric space
The nontrivial local symmetry symmetric spaces correspond tobounded complex domains
The nontrivial bounded complex domains have Shilov boundaries
GLOBAL AND LOCAL TOGETHER:
Very roughly (see my web site and papers for details), think ofthe force strength as
That is (again very roughly and intuitively):
the geometric strength of the force is given by the product of
When you calculate the product volumes (using some trickynormalization stuff that I am ignoring in this exposition, but whichARE dealt with on my web site etc), you see that roughly:
Volume product for gravity is the largest volume
so since (as Feynman says) force strength = probability to emit agauge boson means that the highest force strength or probabilityshould be 1
I normalize the gravity Volume product to be 1, and so roughlyget:
There are two further main components of a force strength:
CONSIDER MASSIVE GAUGE BOSONS:
I consider gravity to be carried by virtual Planck-mass blackholes, so that the geometric strength of gravity should be reduced by1/Mp^2
I consider the weak force to be carried by weak bosons, so thatthe geometric strength of gravity should be reduced by 1/MW^2
That gives the result:
FINALLY, CONSIDER RENORMALIZATION RUNNING FOR THE COLOR FORCE:
That gives the result:
The use of compact volumes is itself a calculational device,because it would be more nearly correct, instead of
to use
However, since the strongest (gravitation) geometric forcestrength is to be normalized to 1, the only thing that matters isRATIOS, and the compact volumes (finite and easy to look up in thebook by Hua) have the same ratios as the noncompact invariantmeasures.
In fact, I should go on to say that continuous spacetime and gaugeforce geometric objects are themselves also calculational devices,and
that it would be even more nearly correct to do the calculationswith respect to a discrete generalized hyperdiamond Feynmancheckerboard.
In my view, it flows naturally from the void by introducing abinary choice (Yin-Yang) which creates the generalized hyperfiniteII1 von Neumann algebra factor made up of 8-dim Clifford algebracomponents (think of a generalization of the Aleph of Borges, oran infinitely large simplex ).
Other people who have a less Taoist/IFA viewpoint than I are freeto say whatever they want to say about each step. Some ( like me )might say that each step is inevitable, while others might say thateach step is a separate "postulate".
WHICHEVER VIEW ANYONE TAKES, THE MODEL IS CLEAR, WELL-DEFINED,CONSISTENT, AND REALISTIC, which is far beyond any other physicsmodel that has yet been presented, so it bothers me that it is sowidely ostracized ( possibly one reason being that I refuse todisavow the mystical origins of my intuitions used in constructingthe model ).
This simplified expository overview is based on July 2006 e-maildiscussion with Ark Jadczyk.
0 - I start with the emergence from the void of a binary choice,like Yin-Yang, which naturally gives a real Clifford algebra, so thatphysics is described by a very large real Clifford algebra (ageneralized hyperfinite II1 von Neumann factor).
Then:
1 - due to real Clifford periodicity it is reducible to Cl(8)tensor product factors (in this message I will ignore sometechnicalities like signature), so Cl(8) describes physicslocally.
2 - Cl(8) vector spacetime is octonionic, and Spin(8) bivector isthe Lie algebra of the physics gauge group, with a Lagrangian (forthis message just looking at spacetime and spinor fermions andignoring gauge bosons etc)
3 - At low (where we are) energies a specific quaternionicsubmanifold freezes out, splitting the 8-dim spacetime into a 4-dimphysical spacetime plus a 4-dim internal symmetry space and creatingsecond and third generation fermions that live (at least in part) inthe 4-dim internal symmetry space and correspond respectively topairs and triples of octonion basis elements.
4 - ignoring for this exposition details about the 4-dim internalsymmetry space, and ignoring conformal stuff (Higgs etc), andconsidering for now only first generation fermions, the 4-dimspacetime Lagrangian spinor fermion part is:
Look at the basic Lagrangian spinor fermion part:
In the conventional picture, the spinor fermion term is of theform m S S* where m is the fermion mass and S and S* represent thegiven fermion. Although the mass m is derived from the Higgsmechanism, the Higgs coupling constants are, in the conventionalpicture, ad hoc parameters, so that effectively the mass term is, inthe conventional picuture, an ad hoc inclusion.
but
to construct the integral such that the mass m emerges naturallyfrom the geometry of the spinor fermions.
To do that, make the spinor fermion mass term have the volume ofthe Shilov boundary corresponding to the symmetric space with LOCALsymmetry of the Spin(8) gauge group with respect to which the firstgeneration spinor fermions are seen as +half-spinor and -half-spinorspaces.
Note that due to triality, Spin(8) can act on those 8-dimensionalhalf-spinor spaces similarly to the way it acts on 8-dimensionalvector spacetime prior to dimensional reduction.
Then, take the the spinor fermion volume to be the Shilov boundarycorresponding to the same symmetric space on which Spin(8) acts as alocal gauge group that is used to construct 8-dimensional vectorspacetime:
- the symmetric space Spin(10) / Spin(8)xU(1)
- corresponds to a bounded domain of type IV8
- whose Shilov boundary is RP^1 x S^7
Since all the first generation fermions see the spacetime overwhich the integral is taken in the same way ( unlike what happens forthe force strength calculation ), theonly geometric volume factor relevant for calculating firstgeneration fermion mass ratios is in the spinor fermion volumeterm.
Consider a first-generation massive lepton (or antilepton,i.e., electron or positron). For definiteness, consider an electron E(a similar line of reasoning applies to the positron).
Since the electron cannot be related to any other massive Diracfermion,
Consider a first-generation quark (or antiquark). Fordefiniteness, consider a red down quark I (a similar line ofreasoning applies to the others of the first generation).
Therefore first-generation quarks or antiquarks can by gluons,weak bosons, or decay occupy the entire volume of the Shilov boundaryRP1 x S7, which volume is pi^5 / 3, so
Consider graviton interactions with first-generationfermions. Since MacDowell-Mansouri gravitation comes from 10Spin(5) gauge bosons, 8 of which are charged (carrying color orelectric charge) as shown in the root Spin(5) root vector diagram
* * * o o Spin(5) root vector diagram * * *
in which the 6 root vectors * correspond to color carrying gaugebosons act similarly to the action of the 6 color-charged SU(3)gluons shown in the SU(3) root vector diagram
* * * SU(3) root vector diagram * * *
The 2 charged Spin(5) gravitons denoted by o carry electriccharge. However, even though the electron carries electric charge,the electric charge carrying Spin(5) gravitons can only change theelectron into a ( tree-level ) massless neutrino, so the Spin(5)gravitons do not enhance the electron volume factor, whichremains
Since the quark carries color charge, Spin(5) graviton action onits color charge multiplies its volume V(quark) by 6, giving
The 2 Spin(5) gravitons carrying electric charge only cannotchange quarks into leptons, so they do not enhance the quark volumefactor, so we have (where md is down quark mass, mu is up quark mass,and me is electron mass)
The proton mass is calculated as the sum of the constituent massesof its constituent quarks
which is close to the experimental value of 938.27 MeV.
In the first generation, each quark corresponds to a singleoctonion basis element and the up and down quark constituent massesare the same:
First Generation - 8 singletons - mu / md = 1
Second and third generation calculations are generally morecomplicated and will not be dealt with in this simplified overview,except to say that combinatorics indicates that in higher generationsthe up-type quarks are heavier than the down-type quarks. The thirdgeneration case, in which the fermions correspond to triples ofoctonions, is simple enough to be used here as an illustration of thecombinatoric effect:
8^3 = 512 triples
mt / mb = 483 / 21 = 161 / 7 = 23
The use of compact volumes is itself a calculational device,because it would be more nearly correct, instead of
to use
However, since the fermion masses all are derived from and relatedto the Higgs VEV ( which could be considered to be given ) the onlything that matters is RATIOS, and the compact volumes (finite andeasy to look up in the book by Hua) have the same ratios as thenoncompact invariant measures.
In fact, I should go on to say that continuous spacetime and gaugeforce geometric objects are themselves also calculational devices,and
that it would be even more nearly correct to do the calculationswith respect to a discrete generalized hyperdiamond Feynmancheckerboard.
In my view, it flows naturally from the void by introducing abinary choice (Yin-Yang) which creates the generalized hyperfiniteII1 von Neumann algebra factor made up of 8-dim Clifford algebracomponents ( think of a generalization of the Aleph of Borges, oran infiniitely large simplex ).
Other people who have a less Taoist/IFA viewpoint than I are freeto say whatever they want to say about each step. Some ( like me )might say that each step is inevitable, while others might say thateach step is a separate "postulate".
WHICHEVER VIEW ANYONE TAKES, THE MODEL IS CLEAR, WELL-DEFINED,CONSISTENT, AND REALISTIC, which is far beyond any other physicsmodel that has yet been presented, so it bothers me that it is sowidely ostracized ( possibly one reason being that I refuse todisavow the mystical origins of my intuitions used in constructingthe model ).