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Notes

[Sunday 8 February 2009 - Saturday 14 February 2009]

[Notebook: DB 65 Symmetric U]

[page 106]

Sunday 8 February 2009

To keep the Trinity or leave it out? [of why-quantized] What Augustine and Aquinas are saying is perfectly consistent with both experience and quantum mechanics: Augustine Aquinas 165 Any system observing itself, diversifies itself. The Father begets the [Son] The qubit begets two bits; I reflect upon myself and slowly bring forth all these words, while personally becoming older and more complex. And credit where credit is due. The psychological model has a long history stretching deep into the past in all cultures that have left us a written history. Hacklin

This process in analogous to Peano's adding 1, or Cantor's generation of the next transfinite number. From a network point of view an oscillator is the simplest computation while the reproduction of a person or the generation of the Son may be modelled by the production of a new transfinite number.

Kauffman Kauffman

Monday 9 February 2009

We are thinking of a communication channel as

[page 107]

an algorithm (represented by a Turing machine which transforms the message emitted by the transmitter into the message received by the receiver. For duplex communication, we require the inverse algorithm that goes the other way. Quantum field theory thinks of the communication of forces in terms of the exchange of particles, so we can think that forces have something to do with particles, algorithms and transformations. From this point of view we can think of every particle as a snippet of software that serves as a subroutine in the overall universal process, so explaining why all electrons etc are identical because they are all the same software. Further, we imagine that point particles are those whose software does not require 3-space for its representation. How do we extend this idea to fermion vs boson, ie antisymmetric and symmetric wavefunction, ie using all the possibilities at a given level of complexity.

Yang-Mills Gauge theory - Wikipedia, Yang-Mills theory - Wikipedia, Mass gap - Wikipedia

Dodd page 87: 'So invariance the the Lagrangian under local gauge transformations requires the existence of the photon: the long range electromagnetic field. A physical explanation of its existence may be thought of as communicating the difference space-dependent conventions defining the phase of the electron wave at different points in space.' Dodd, Coughlan

By carrying energy from place to place that suggests that energy can be localized, ie that the point energy of the initial oscillator has been distributed over 3-space while remaining constant (conserved) in time.

Tuesday 10 February 2009

[page 108]

The physics community has long been receiving free drinks on the strength of the scientific and successes of the second world war. From their point of view it seemed reasonable to develop nuclear weapons before Hitler, but the belief that Hitler was developing weapons suggests, in hindsight, the same sort of politically driven intelligence failure that led us into the invasion and destruction of Iraq. Rose, Ricks

Yang-Mills gauge theory and networks.

From the initial oscillator to spacetime.

C, P and T are our fundamental symmetries, or, we might say, the fundamental breakings of symmetry. Streater and Wightman Clearly the initial oscillator, since it is associated with no counter or no complexification is in a sense reversible in time since it has no time, not has any measurable period, ie there is nothing to compare it to. It is, we might say, pure energy with no structure except two states, p and not-p which succeed one another in 'any' order.

The next symmetry, also not requiring space in the conventional sense, is C, the diversification into 'particles' and anti-particles. The defining characteristic of such particles is that when they meet they 'annihilate' into pure energy, which can then break its symmetry once more into different particles.

Next, P requires some notion of space for its conceptualization and it is formalized as Lorentz Transformations with a negative determinant, at least in 3-space (Streater & Wightman).

Dodd: 'Spontaneous symmetry breaking: Obtaining asymmetric solutions (ie massive W bosons) from a symmetric theory (ie

[page 109]

gauge invariant theory) is common in many branches of physics. . . . How has [does?] this come about? The answer lies in the fact that the symmetric state is not the state of minimum energy, and that in the process of evolving toward the minimum energy state, the system has broken its initial symmetry, page 89. Spontaneous symmetry breaking - Wikipedia, Yoichiro Nambu - Wikipedia

Symmetry (as in the symmetric Universe) presents us with a huge array of possibilities which are represented in our model as permutations which, when implements as algorithms, give us more or less effective ways to achieve a given task. These algorithms, we surmise, compete among themselves and from all being winners are winnowed down to the fittest, thus breaking the initial symmetry,

Dodd, page 89: 'We now want to apply these ideas to particle theory to see if a broken symmetry has anything to do with particle mass.'

The C symmetry must have been broken at a time when the whole Universe was so small (or communication so fast) that it was broken throughout the Universe so (as far as we know) there are not whole regions (galaxies, clusters, etc) in the Universe made of anti-matter.

The symmetry represented by U(1) simply represents the initial oscillator with all its manifestations we now call qubits. Qubit - Wikipedia

We can only get stationary patterns of interference (as in the two slit experiment) if we have stationary relationships of phase which in turn require stationary energies. If we conduct the two slit experiment with 'non-monochromatic' particles their different wavelengths give different interference patterns whose sum is spatially symmetric

[page 110]

and so invisible. Conversely, we can use a glorified 'two slit' ie a diffraction grating, to sort a mixture of wavelengths into different energy bins, as is done in spectroscopy.

Is the initial oscillator the Goldstone boson, undetected because it is ubiquitous? Goldstone boson - Wikipedia In the unbroken symmetry there is just the Goldstone boson whose symmetry is broken in to a Goldstone boson (the kinetic energy) and a massive particle, which corresponds to a particle with kinetic energy.

Goldstone bosons and Higgs particles. Higgs boson - Wikipedia

Gravitation + general covariance leads us to continuity at the fundamental level. So we ask 'is gravity quantized? No, because it deals with pure energy it is foolproof and so incapable of error by pure symmetry. Gravitation treats all possibilities equally.

Selection and spontaneous symmetry breaking?

For the initial oscillator, the formula E = h bar omega products hat the quantum of energy is the energy of the Universe.

Dodd page 15: 'Resolution of [the paradoxical appearance of the photon as both a particle and a wave] requires the introduction of a new entity which reduces to both particle and wave in different circumstances. The entity turns out to be a field. . . . ;

All the information in quantum mechanics is carried by phase which is equivalent to action, ie energy x time = frequency x time = the amount of resource devoted to computation since 1 revolution = 1 execution of a Turing machine.

[page 111]

Dodd page 19: 'Heisenberg's approach is the literal manifestation of Wittgenstein's parting philosophical rejoinder, 'concerning that of which we cannot speak, we must pass over in silence'. Wittgenstein, Ludwig Wittgenstein - SEP We can speak (or write equations) only of what we observe, and so observation is to have pride of place in quantum theory.'

A particle is the superposition of many processes operating at different frequencies, that is the execution of a complex algorithm.

Pauli exclusion principle = particle no cloning: simply put if particles are fully identical there is only one of them not two. Identical particles means the same piece of software executing in different instances.

Churchill page 289: 'Few recognized the difference between winning battles and making lasting conquests. Parliament in its youth was eager for war, improvident in preparation and resentful in paying for it. Churchill

page 295 'The revolt, which to the historian is just a sudden flash of revealing light on medieval conditions among the poorer classes, struck with lasting awe the imagination of its contemporaries. It left a hard core of bitterness among the peasantry, and called forth a vigorous and wasteful resistance from authority. Henceforth a fixed desire for the division of ecclesiastical property was conceived.'

page 295: 'The bishops were instructed to arrest all unlicensed preachers, and the Archbishop himself rapidly became the head of a system of Church discipline, and this, with the active

[page 112]

support of the state in the Lancastrian days, eventually enabled the Church to recover from the attack of the laity.

Churchill page 296: 'By his frontal attack on the Church's absolute authority over men in this world, by his implication of the supremacy of the individual conscience and by his challenge to ecclesiastical dogma, Wyclif had called down upon himself the thunderbolts of repression. But his protest had led to the first of the Oxford Movements.' John Wycliffe - Wikipedia

'Fuller the seventeenth century writer, wrote of Wyclif's preachers: "These men were sentinels against an army of enemies until God sent Luther to relieve them".'

The qubit drives the world. Looking at enough of them with random phases, we see U(1), but at the detailed level, each of them goes its own way with a certain frequency. Circle group - Wikipedia

U (1) is Abelian. Not so more complex groups. Abelian group - Wikipedia We can see what is happening in the construction of chiral molecules which have enough structure to be orthogonal to one another no matter how they are placed in space.

1401 De Haeretico Comburendo Henry IV

Michael Atiya: 4 [Clay Millennium] problems at the interface of geometry and analysis. Clay Millennium Prize - Atiyah

. . .

[page 116]

John Tate: [3 Clay Millennium prize problems} Reformulation of Arithmetic and Geometry Clay Millennium Prize - Tate

. . .

[page 117]

Wednesday 11 February 2009

Hamilton's variational principle: Systems evolve so as to minimize L = T - V. For a computer T = rate of processing, V = capacity of memory. Memory is governed by the Pauli exclusion principle, so, as in an atom, if you want more memory you

[page 118]

must have more electron states each having different potential energies mediated by their relationships to the nucleus [and eachother]

Each new correspondent on a network is a 'perturbation' of the network.

Dodd page 28: 'In the quantum version [of Hamilton's principle] as we are dealing with wavefunctions (or more properly fields) which extend throughout space, we do not deal with the total Lagrangian L directly, but with the Lagrangian density L

This assumes that quantum theory takes place 'in' space. We would prefer to think of pace as emerging in some way from quantum mechanics.

'By minimizing L with respect to the wavefunction [of a free electron] and its time and space derivatives, it is possible to derive Dirac's equation of motion of the electron denoted D Psie

delta L Psie = 0 ==> D Psie,

Interaction of photons and electrons:

L0 Psie = L of free electron
L0 A = L of photon
Linteraction ( Psie , A ) = L of interaction

so L = L0 Psie + L0 A + Linteraction ( Psie , A )

'This is the top level specification of the fields being described. . . . The variational principle now describes the propagation of the fields in terms of the creation and destruction of the quanta of the fields and by the wavefunctions of the quanta during their existence

[page 119]

(referred to as propagators in this context).

Feynman diagrams and Feynman rules.

Dodd page 29: 'To calculate the probability P of any physical event . . . it is first necessary to select the initial and final states being observed, denoted |i > and <f | respectively, and then to select all the Feynman diagrams which can connect the two. [All possible network connections]. The mathematical expression for the diagram is then worked out: essentially, the wavefunctions of the quanta are multiplied together to give the quantum mechanical amplitude m for the sub-processes. The amplitude for a number of sub-processes may then be added to give the total amplitude M which is then squared to give the required probability of occurrence.'

This setup is linear because there is no 'self' interaction - photons only interact via electrons and vice versa.

The probability of interactions of photons and electrons is low. 'As each new order of diagram contains a new photon line with two vertices the relative magnitude of successive orders is reduced by e2 /h bar c = 1/137. So only he first few subprocesses need be calculated to achieve an acceptable approximation to the exact answer.

page 30: 'Virtual processes' (unobservable processes) made possible by uncertainty principle.

Renormalization: 'In writing down the Feynman diagrams of the sub-processes we find some whose amplitude (product of wavefunctions) appears to be infinite.'

page 31: In 1949 Feynman, Dyson and Tomonaga showed how the

[page 120]

infinite contribution to the perturbation series can be removed by redefining the electron, photon and electric charge to include quantum corrections. [?] When the real electrons, photons and charges appear, the infinite diagrams are included implicitly and should not be recounted. The mathematical proof of the demonstration is known as 'renormalization'. Renormalization - Wikipedia

All sounds like 'ad hocery' to me arising form the need to deal in continuous mathematics which assumes that the quantum of action can be infinitely subdivided as in the 'path integral' method. We would like to think that all processes involve an integral number of quanta and by enforcing this rule we would get rid of a lot of trouble, but how to do it? The heuristic principle here is that when the world was very young and simple (before it even had space) processes had to be simple and they have taken on their complex appearances by being embedded in the complex machinations of higher levels of the system. [thus eg in everyday computations, simple nand gates are hidden in the rendering of complex images]

Dodd page 32: 'All the calculations in quantum field theory follow from the specification of the correct interaction Lagrangian, which is determined by the conservation laws obeyed by the force under study.'

Minimizing Lagrangian means minimizing processing rate (=T ) while maximizing memory (=V ). What does this mean. All memory = all space = all the things that do not change (relatively speaking) with time = carries potential = potential energy. In standard physics we see potential as being carried by a field in space. How do we understand this in a network model?

Even though it looks complex in the expanded Universe, we are inclined to view gravitation as the fundamental force, since it seems to account for the large scale structure of the Universe

[page 121]

and yet be indifferent to structure, since it sees all structures that have energy, even if these structure are 'dark'. Dark energy - Wikipedia So energy couples to itself (very weakly) and we might say that gravitation itself has no memory and so no structure. When we put it into space (or should we say 'when space uses gravitation' we get the inverse square law and Einstein's curved = dynamic space. We might find the essence of gravitation by looking at Einstein's field equations in zero dimensional space.

Equivalence
General covariance (subject to the constraint of C infinity gaussian manifold. General covariance - Wikipedia

We divide the initial oscillator into a collection of secondary oscillators distinguished only by the frequencies (energies).

[The fixed point here is the differential equation which admits as solutions all energies summing to ℵ0, which we might say corresponds to the initial singularity]

. . .

In the absence of space angular and linear momentum are both equal to energy.. The origin of space breaks the symmetry of energy into energy and momentum.

God is the most symmetrical being of all. [Omnino simplex Aquinas 20]

We understand symmetry breaking by the generation of new network layers followed by competition among the peers of the new layer for the resources of the previous layer leading to a set of 'fit' systems like the fundamental particles. QED --> Yang mills.

Since the Universe begins as one and remains one, any breaking of symmetry must be accompanied by a 'symmetry restoring' feature which maintains the unity. This implies communication between the pieces of the broken symmetry which physics calls gauge particles. Gauge boson - Wikipedia

Given our idea that gravitation is not quantized we have not so much a gauge particle as a gauge flow, so we conceive of energy flowing around as a non-viscous conserved (incompressible) quantity subject to some differential equations like dE/dt = 0.

Memory, potential, force, distance, energy

Conjugates: 'god' 'prime matter'.

Google.org Google.org

. . .

Before the advent of spacetime, all local symmetries are global symmetries since global = local.

We might look at the symmetry group as a channel through which information may be sent as U(1) is the channel in electromagnetic communication. So Yang-Mills theories of SU(2) etc are more complex channels.

Space and time symmetries, by being broken, enable us to communicate by various serial and parallel channels, such as this writing.

Lower layers of the network are more physical and more abstract. [Abstract knowledge attempts to model these lower layers through the fog of complexity built upon them]

[page 123]

CONSERVATION = MEMORY [software (which is in fact harder than hardware)]

A symmetry group is a closed world of possibilities = CHANNEL

Actual communications are broken global symmetries = local symmetries.

The covariant derivative, by taking into account local symmetries, enables us to connect the changes in local coordinates to the real changes in a particle as it moves through the coordinate mollusc, taking the 'connection coefficients' from place to place into account. Einstein

Dodd: 'The physical laws governing any process are formulated with a particular origin and a particular coordinate system in mind.'

Not so with networks, in which everything is a relationship (channel) between two points, completely defined by the points without reference to any coordinate system. From a network point of view the 'coordinates' are the languages (protocols, algorithms, particles) used to mediate any communication. Ultimately all messages go through the initial singularity, which is completely symmetrical, ie enjoys general covariance, or equivalently, no protocol.

The birth of the qubit = the procession of the Logos, 'simultaneously' produces both potential and kinetic energy. The kinetic energy lies in the oscillation between the two persons, the potential energy from the simple fact of their distance. In the case of the primordial qubit (the initial oscillator), the gauge particle moving between the two concentrations of energy [the 'Holy Spirit'] is itself energy, and we need to dream up a way to couple this to gravitation. [Einstein has done it?]

[page 124]

We do not wish to upset quantum mechanical calculations, but to put them in a wider context.

We see each layer persisting in the layers above it, so we should expect to see the initial singularity (eternal God the Father) everywhere just as we see the initial oscillator (qubit, Father & Son) everywhere. We may interpret the Trinity as a semi-mythological explanation of the emanation of the world from the divinity. Tantra - Wikipedia

The network is 'self-coordinating'.

So we need to introduce a paragraph into why_quantized about general covariance and the expansion of this from the continuously constrained world of general relativity to the 'Turing general covariance' of the world starting from the qubit and the introduction of the quantum of action which is in effect just the initial singularity, the fundamental arithmetic unit.

Oscillation of energy between the two states of a qubit is the same as oscillation of probability, the total probability remaining constant. We can see this as a parity or space inversion, usually described by a continuous rotation.

Linguistic encoding and decoding are equivalent to a covariant derivative.

. . .

[page 125]

The mathematical continuum makes sense if it can be mapped to a logical continuum, so the idea of a line of discrete points is held together by mapping the discrete points to a real line which is physically (= logically) continuous.

Dodd page 44: '. . . the conservation of electrical charge . . . can be represented by requiring the Lagrangian to remain invariant under arbitrary shifts in the phases of the charged particle wave functions appearing in the Lagrangian.

Ie charge is an algorithm which remains the same while processing all the different messages represented by different phases.

The L is something static that can be written down and so represent an algorithm that can process many different inputs and is symmetric with respect to the inputs. So English speakers are symmetric with respect to the language, since they can process all inputs equally. This symmetry is partly broken when one speaker uses words the other does not know and completely broken when they use two different languages (considered orthogonal to one another).

The layering of the permutation network may be considered in terms of groups and subgroups.

With a computer, we only observe the input (say keyboard) and the output (say screen). All the other operations of the machine are transparent (= virtual)

[page 126]

Dodd page 46: Muon behaves exactly like a heavy electron and decays into an electron in 2 x 10-6 s, so it is not found in ordinary matter.

Can we see a meson as an inefficiently coded electron, achieving the same end with a lot more cycles (energy) [and so selectively disadvantaged].

A language must be symmetrical so that it can express many different ideas with equal facility, ie flatness.

Say it again. A communication channel, ie an algorithm, must be open to all messages obeying the protocol, ie flat or symmetric. So a Turing machine can multiply, add, divide, etc any two rational numbers as long as none of the inputs or outputs exceed 'machine infinity'.

Thursday 12 February 2009

Lagrangian is composed of additive elements. We might assume that L (initial oscillator) = 0, ie the kinetic energy of the Universe is equal to its potential energy, which is equal to the zero energy of the initial oscillator, which does not exist in the sense that it communicates with nothing outside itself. Fact? Fantasy? Meaningless? Convincing? Testable? Consistent?

Interference of two indistinguishable electrons, N 448:262, 233 Neder et al

INTERFERE - RESONATE

[page 127]

't Hooft N448:271 't Hooft Reconciliation of Quantum Mechanics and Special Relativity completed in the Standard model.

't Hooft page 271: '. . . [gauge theories] had been proposed by Chen Ning Yang and Robert Mills who were inspired by the fact that the two basic forces of nature that were well understood, gravity and electromagnetism, were both based on the principle of gauge invariance: that is that symmetry transformations can be performed in one region of spacetime without affecting what happens in another.'

Or does it mean that every local change in explained by a message to or from elsewhere?

Hoddeson et al Rise of the Standard Model Hoddeson

Asymptotic freedom: the strength of reactions reduced at short distances, (instead of blowing up to infinity?)

'Bjorken scaling' Wu-Ki Tung

't Hooft page 272: '. . . theorists had concluded that no quantum field theory would be suitable for the strong force - until the asymptotic freedom of Yank-Mills fields was uncovered.

'This [1970s] model describes the closely related Yang-Mills systems for he three major forces . . . one Higgs field and several matter fields. These matter fields were Dirac fields, describing the four known leptons and the three known quarks (up, down and strange) all of which has half a unit of spin. According to this theory, the Dirac particles cannot interact directly with one another but only by exchanging energy quanta of the Yang-Mills field. The interactions between Yang-Mills and

[page 128]

matter fields are identical for all particle types; only the Higgs fields couples differently to the different matter fields. And only in this was is differentiation brought between the various kinds of particles according to this new insight.'

Discovery of more quarks and leptons gave us the 'standard model'.

't Hooft: page 273: 'Adding neutrino mass terms to the standard model, was, however, only a minor repair and not totally unexpected, although it did add more parameters to the model. The earlier version had 20 fundamentally freely adjustable parameters in it; now the number would need to be increased to at least 26.'

And this for 24 fundamental particles: 12 bosons and 12 fermions. [?] Elementary particle - Wikipedia

page 273: 'By the 1980s it was understood that quantum field theories are perfect frameworks for the detailed modelling of all known particles. Indeed, if we require theories with only a limited number of elementary degrees of freedom, and thus a finite number of freely adjustable parameters, then it must be assumed that all forces are renormalizable. But, for all strong forces, the more stringent conditions of asymptotic freedom is required. The only theories with these desired properties are theories in which Dirac particles interact exclusively with Yang-Mills fields and (where needed) Higgs fields. This is now regarded as the answer to that problem of more than half a century ago - how to reconcile quantum mechanics with special relativity.'

The fact of consistent universal structure points to memory, which in turn points to the 'eternal' initial singularity.

Lederman N 4488:310 Lederman Book 1993 The God Particle Lederman 1

[page 129]

Does the Higgs really give mass to everything?

Lederman page 312: 'By necessity we are now comfortable with the hypothesis that all standard model particles have zero radius and so no [spatial] substructure. [Although they have enough structure to have different identities = quantum numbers].'

This suggests that they are outside space in the same way as the internet is apparently outside space. As I browse files and talk to people around the world, their spatial distances and orientations are irrelevant to me. All I need to know is their [logical] address (which can be mapped to a physical computer somewhere) and their 'content'.

Neder et al 448:333 'For a single particle the interference is between the amplitudes of the particle's wave functions, whereas the interference between two particles is a direct result of quantum exchange statistics. ' Neder et al

What we mean when we say that a particle has mass is that it has a very short range (as a force mediating 'virtual' particle) because it can only borrow a quantum of energy for so long before ut has to give it back and cease to exist. This assumes m = E/c 2.

Many theologians (not me) claim that their source is outside the Universe.

The development of the standard model has not been easy and many of the problems have arisen from the perceived need to take all calculations to the continuum limit. Our task here is to reconcile the discrete network

[page 130]

picture with the continuous picture, and the natural starting point appears to be gravitation, which (although it is not part of the standard model) appears to be naturally continuous. Einstein's key insight when developing the theory of relativity was that coordinates systems (at least as understood by his contemporaries) were not part of nature, but simply convenient forms of addressing the elements of a system under study. What matters in nature is the relationships of the elements to one another. Their relationship to a coordinate system is merely a way of clearly expressing their relationships to one another. This insight is captured by the term 'general covariance' which means that no matter how we choose the coordinates, nature goes its own way. The fixed points in the natural system are events and we may use different coordinate systems to label natural events in any way we like subject to one constraint only, that the transformations between different coordinate systems be smooth and continuous, that is diffeomorphisms, a constraint naturally captured by tensor analysis. Diffeomorphism - Wikipedia Tensor - Wikipedia

Tensors through the mechanism of covariant derivatives and connection coefficients automatically compensate for changing bases, so a tensor equation true in one coordinate system is true in all coordinate systems connected to the first by a diffeomorphism.

The network approach goes one step further, doing away with external coordinate systems altogether, requiring only distinct addresses with no fixed spatial relationships whatever to do their business. All that is needed to send a message is the address of the recipient and the message, and the address is something local to the recipient, rather than global.

[page 131]

By doing away with an ordered coordinate system, communication systems must search their address books to find recipients, but if addresses are hierarchically ordered, the process can be fast.

Standard model does not exist in geometric space but in address space.

Gravitation is in a way the simplest gauge theory because it works in real familiar imaginable space and time. Einstein's insight was to use Gauss and Riemann's ideas to provide an intrinsic addressing system for cosmic dynamics It is also simple because it is blind to all but energy which behaves like a single global conserved flow, just like money, with the added feature that like money, energy attracts energy. The gravitational gauge is energy.

KINETIC energy is ATTRACTIVE
POTENTIAL energy is REPULSIVE, so systems try to move away from areas of high potential, like the top of the swing of a pendulum. One is repelled by the tops of hills and attracted by the valleys, but energy is nevertheless conserved. So the high potential of the initial singularity repels the Universe into expansion, yet as soon as it begins to expand the resulting kinetic energy is attractive.

CURVATURE = POTENTIAL

Curvature restricts communication, flatness encourages it, so we travel more easily over flat surfaces than hilly ones.

[page 132]

Friday 13 February 2009

Quantum gauge theories were inspired by the classical gauge theories, Maxwell's electrodynamics and Einstein's gravitation. Both may be understood using the simplest gauge model of all, the classical harmonic oscillator, embodied in a simple pendulum or weight on a spring. This in turn comes back to Newton's gauge equation F = ma which is enunciated in Newton's three laws which are a more detailed statement of the ancient idea no effect without a cause, where cause is translated force. To this Newton gave mathematical expression.

All of this can be understood in terms of the interplay of potential and kinetic energy mediated by force. In total, energy is conserved, but it may flow from potential to kinetic and back again through the intermediary of a force. Causality tells us that force is acting when we see a change of movement of energy. force is a message.

This concept received its highest classical expression in the general theory of relativity, where gravitation is seen as the intermediary between the shape of space (a potential) and the movement of bodies within it, expressed in Einstein's equations, which deal with a continuum of conserved energy.

The foundation of universal structure is the abstract bifurcation of the initial singularity into a potential and a motion. We identify the potential with memory and the motion with processing, and the principle of causality becomes no

[page 133]

memory changed without process. Ie the communication is the gauge measuring the change of potential.

Maxwell Maxwell

As in mathematics, the discretum comes before the continuum. Since the invention of the continuum it has come to dominate mathematics and hidden much of what the discrete has to tell us. This only began to find its way back into the light of day with the work of Cantor, Frege and co, who saw that even the arguments about the continuum were discrete and logical.

The fate of the Standard Model now hangs upon the Large Hadron Collider. Will is reveal the Higgs boson? Will it reveal new physics?

I smoke to gain insight and hope that in later life, if I lie dying of smoke induced cancer, that I will be able to look back on what I have seen and communicated to the world [and feel] that it was worth it. I hope Einstein felt this.

We may look upon a differential equation as a fixed point of an infinity of dynamic solutions like the vibration of a string and its overtones which would be countably infinite if not suppressed by the stiffness of the string

FLOW - FLUX - FLUXIONS Method of Fluxions - Wikipedia

Change + cause of change = 0. Once we can appreciate the cause of a change, it is as though nothing has

[page 134]

happened.

Saturday 14 February 2009
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Further reading

Books

Click on the "Amazon" link below each book entry to see details of a book (and possibly buy it!)

Augustine, Saint, and Edmond Hill (Introduction, translation and notes), and John E Rotelle (editor), The Trinity, New City Press 1991 Written 399 - 419: De Trinitate is a radical restatement, defence and development of the Christian doctrine of the Trinity. Augistine's book has served as a foundation for most subsequent work, particularly that of Thomas Aquinas.  
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Bergson, Henri, and Arthur Mitchell (translator), Creative Evolution, Rowman & Littlefield 1983 Amazon Book Description: 'Creative Evolution, originally published in 1911 by Henry Holt and Company, is the work which catapulted Bergson from obscurity into world-wide fame. A study of the philosophical implications of biological evolutionary theory, the impact of this book reached far beyond biology and seemed to many to herald a new age in philosophy and the sciences.' 
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Churchill, Winston S, A History of the English Speaking People (Volume 1), Cassell Reference 2002 Amazon Product Description 'Volume I tells the story of Britain from pre-history to the Battle of Bosworth - the last of the battles of the Wars of the Roses in 1485 - and describes the strife and turmoil in the making of a nation. When this volume begins, tribal law was supreme; when it ends, Brtiain had become a nation and stood on the threshold of those adventures overseas which were to make an empire. Along the way we encounter a plethora of closely observed characters - William the Conqueror, Alfred the Great, Richard the Lionheart, Joan of Arc - and Churchill analyses the beginnings of Parliament, the Church and the monarchy with an eye as sharp as his legenday wit.' 
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Coughlan, G D, and J E Dodd and B M Gripaios, The Ideas of Particle Physics: An Introduction for Scientists, Cambridge University Press 2006 Amazon Product Description 'The third edition of this well-received book is a readable introduction to the world of particle physics. It bridges the gap between traditional textbooks on the subject and popular accounts that assume little or no background knowledge. Carefully revised and updated, this new edition covers all of the important concepts in our modern understanding of particle physics. The theoretical development of the subject is traced from the foundations of quantum mechanics and relativity through to the most recent particle discoveries and the formulation of modern string theory. It includes a full description of the prospects for the Large Hadron Collider at CERN, which will allow many key ideas to be tested. The book is intended for anyone with a background in the physical sciences who wishes to learn more about particle physics. It is also valuable to students of physics wishing to gain an introductory overview of the subject.' 
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Dodd, J E, and G D Coughlan, The Ideas of Particle Physics: An Introduction for Scientists, Cambridge UP 1991 Jacket: 'This book is intended to bridge the gap between traditional textbooks on particle physics and the popular accounts of the subject ... Although entirely self contained, it assumes a greater familiarity with the basic physics concepts than is usually the case in popular texts. This then allows a fuller discussion of more modern developments.' 
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Einstein, Albert, and Robert W Lawson (translator) Roger Penrose (Introduction), Robert Geroch (Commentary), David C Cassidy (Historical Essay) , Relativity: The Special and General Theory, Pi Press 2005 Preface: 'The present book is intended, as far as possible, to give an exact insight into the theory of relativity to those readers who, from a general scientific and philosophical point of view, are interested in the theory, but who are not conversant with the mathematical apparatus of theoretical physics. ... The author has spared himself no pains in his endeavour to present the main ideas in the simplest and most intelligible form, and on the whole, in the sequence and connection in which they actually originated.' page 3  
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Feldman, , Joel S, and Thomas R Hurd, Lon Rosen, Jill D Wright, QED: A Proof of Renormalizability, Springer Verlag 1988  
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Hacklin, J, and Clement Huart, Raymonde Linossir, H de Wilman-Grabowska, Charles-Henri Marchal, Henri Maspero, Serge Eliseev and Paul-Louis Couchoud (Introduction), Asiatic Mythology: A Detailed Description and Explanation of the Mythologies of all the Great Nations of Asia, Crown Publishers Crescent Books Jacket: Asiatic Mythology was a great pioner work when it was first published [1932] and it has been ever since. . . . The Introduction says, "To penetrate to the heart of a civilization we ought to begin with a knowledge of its gods." Asiatic Mythology does indeed penetrate to the heart of civilizations that are drawing nearer to us than ever before. Therefore the book is today more significant and valuable than ever.' back
Hoddeson, Lillian, and Laurie Brown, Michael Riodan & Max Dresden (editors), The Rise of the Standard Model, Cambridge University Press 1997 Review '... a beautifully produced collection of essays by most of the leading scientists involved - including no fewer than eight Nobel laureates - and several eminent historians ... both practitioners and knowledgeable bystanders can draw inspiration from these reflections on what may turn out to have been the golden age of particle physics.' Graham Farmelo, New Scientist 'The volume is informative and useful to historians of physics.' Helge Kragh, Centaurus '... this book is ... worthwhile , timely and valuable.' R. Barlow, European Journal of Physics  
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Kauffman, Stuart, At Home in the Universe: The Search for Laws of Complexity, Oxford University Press 1995 Preface: 'As I will argue in this book, natural selection is important, but it has not laboured alone to craft the fine architectures of the biosphere . . . The order of the biological world, I have come to believe . . . arises naturally and spontaneously because of the principles of self organisation - laws of complexity that we are just beginning to uncover and understand.'  
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Lederman 1, Leon, and Dick Teresi, The God Particle: If the Universe is the Answer, What is the question, Mariner Books 2006 '. . . Part history, part autobiography, part polemic, with sideswipes on mystics onthe way, the book is a strange hotch-potch held together more by Lederman's outsize personality than any logic. . . . ' Roland Pease Nature 362, 302 (25 Mar 1993) 
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Maxwell, James Clerk, Treatise on Electricity and Magnetism (vol 1), OUP 1998 First published 1873 
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Maxwell, James Clerk, Treatise on Electricity and Magnetism (vol 2), OUP 1998 First published 1873 
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Ricks, Thomas E, Fiasco, The American Military Adventure in Iraq, 2003 - 2005, Penguin (Non-Classics) 2007 Amazon.com Review 'Fiasco is a more strongly worded title than you might expect a seasoned military reporter such as Thomas E. Ricks to use, accustomed as he is to the even-handed style of daily newspaper journalism. But Ricks, the Pentagon correspondent for the Washington Post . . . has written a thorough and devastating history of the war in Iraq from the planning stages through the continued insurgency in early 2006, and he does not shy away from naming those he finds responsible. His tragic story is divided in two. The first part--the runup to the war and the invasion in 2003--is familiar from books like Cobra II and Plan of Attack, although Ricks uses his many military sources to portray an officer class that was far more skeptical of the war beforehand than generally reported. But the heart of his book is the second half, beginning in August 2003, when, as he writes, the war really began, with the bombing of the Jordanian embassy and the emergence of the insurgency. His strongest critique is that the U.S. military failed to anticipate--and then failed to recognize--the insurgency, and tried to fight it with conventional methods that only fanned its flames. What makes his portrait particularly damning are the dozens of military sources--most of them on record--who join in his critique, and the thousands of pages of internal documents he uses to make his case for a war poorly planned and bravely but blindly fought. . . . ' Tom Nissley 
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Ricks, Thomas E, The Gamble: General David Petraeus and the American Military Adventure in Iraq, 2006-2008, Penguin Press 2009 Amazon product description: 'The Gamble offers news breaking information, revealing behind-the-scenes disagreements between top commanders. We learn that almost every single officer in the chain of command fought the surge. Many of Petraeus’s closest advisers went to Iraq extremely pessimistic, doubting that the surge would have any effect, and his own boss was so skeptical that he dispatched an admiral to Baghdad in the summer of 2007 to come up with a strategy to replace Petraeus’s. That same boss later flew to Iraq to try to talk Petraeus out of his planned congressional testimony. The Gamble examines the congressional hearings through the eyes of Petraeus and Ambassador Ryan Crocker, and their views of the questions posed by the 2008 presidential candidates. For Petraeus, prevailing in Iraq means extending the war. Thomas E. Ricks concludes that the war is likely to last another five to ten years—and that that outcome is a best case scenario. His stunning conclusion, stated in the last line of the book, is that “the events for which the Iraq war will be remembered by us and by the world have not yet happened."' 
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Rose, Paul Lawrence, Heisenberg and the Nazi Atomic Bomb 1939-1945: A Study in German Culture, University of California Press 1998 Amazon Editorial Review From Booklist 'Of the controversies surrounding the dawn of the atomic age, ranking near the top is the matter of Werner Heisenberg and his team's failure to put a bomb in Hitler's hands. Two principal explanations exist. One view, presented in Thomas Powers' Heisenberg's War (1993), is that Heisenberg hindered research, and, in any event, was not ordered to go all out for the bomb; Rose adopts the opposing contention that Heisenberg failed not because of moral compunctions but because he miscalculated the moderator required by a plutonium-producing reactor and the critical mass for a U235 bomb. That Rose spitefully condemns Powers' popular book as "entirely bogus" indicates the passion he brings to arraigning Heisenberg and his historical defense; and on bomb technology, the strictly technical side, Rose bests Powers. However, his attempted clinching of the argument by digressions into German patriotism and Heisenberg's mindset is too speculative to be convincing. Deeply researched scholarship for serious students.' Gilbert Taylor 
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Streater, Raymond F, and Arthur S Wightman, PCT, Spin, Statistics and All That, Princeton University Press 2005 Amazon product description: ' PCT, Spin and Statistics, and All That is the classic summary of and introduction to the achievements of Axiomatic Quantum Field Theory. This theory gives precise mathematical responses to questions like: What is a quantized field? What are the physically indispensable attributes of a quantized field? Furthermore, Axiomatic Field Theory shows that a number of physically important predictions of quantum field theory are mathematical consequences of the axioms. Here Raymond Streater and Arthur Wightman treat only results that can be rigorously proved, and these are presented in an elegant style that makes them available to a broad range of physics and theoretical mathematics.' 
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Wittgenstein, Ludwig, and David Francis Pears, Brian McGuinness, Bertrand Russell , Tractatus Logico-Philosophicus, Routledge 2001 'This as a most imortant book containing original ideas on a large range of topics, forming a coherent system, which, whether or not it be, as the author claims, in its essentials the final solution of the problems dealt with, is of extraordinary interest and deserves the attention of all philosophers.' Frank Ramsey, 'Critical Notice of L Wittgenstein's Tractatus Logico-Philosophicus', Mind, XXXII, no 128 (October 1923) pp 465-78.  
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Papers
Lederman, Leon, "The God particle et al.", Nature, 448, 7151, 17 July 2007, page 310-312. 'The birth of particle physics -- that is high energy physics -- can be dated to about 1950, offspring of the marriage between nuclear physics and the study of cosmic rays. It exploited techniques and technology from both disciplines, and its objective was to identify the primordial particles of nature -- those from which all matter is made -- and codify the laws of physics that oversee their propperties and social behaviours.'. back
Neder, I, N Ofek, Y Chung, M Heiblum, D Mahalu & V Umansky, "Interference between two indistinguishable electrons from independent sources", Nature, 448, 7151, 19 July 2007, page 333 - 337. 'Very much like the ubiquitous quantum interference of a single particle with itself, quantum interference of two independent, but indistinguishable, particles is also possible. For a single particle, the interference is between the amplitudes of the particle's wavefunctions, whereas the interference between two particles is a direct result of quantum exchange statistics. Such interference is observed only in the joint probability of finding the particles in two separated detectors, after they were injected from two spatially separated and independent sources. Experimental realizations of two-particle interferometers have been proposed; in these proposals it was shown that such correlations are a direct signature of quantum entanglement between the spatial degrees of freedom of the two particles ('orbital entanglement'), even though they do not interact with each other. In optics, experiments using indistinguishable pairs of photons encountered difficulties in generating pairs of independent photons and synchronizing their arrival times; thus they have concentrated on detecting bunching of photons (bosons) by coincidence measurements. Similar experiments with electrons are rather scarce. Cross-correlation measurements between partitioned currents, emanating from one source, yielded similar information to that obtained from auto-correlation (shot noise) measurements. The proposal of ref. 3 is an electronic analogue to the historical Hanbury Brown and Twiss experiment with classical light. It is based on the electronic Mach–Zehnder interferometer that uses edge channels in the quantum Hall effect regime. Here we implement such an interferometer. We partitioned two independent and mutually incoherent electron beams into two trajectories, so that the combined four trajectories enclosed an Aharonov–Bohm flux. Although individual currents and their fluctuations (shot noise measured by auto-correlation) were found to be independent of the Aharonov–Bohm flux, the cross-correlation between current fluctuations at two opposite points across the device exhibited strong Aharonov–Bohm oscillations, suggesting orbital entanglement between the two electron beams.. back
't Hooft, Gerard, "The making of the standard model", Nature, 448, 7151, 19 July 2007, page 271 - 273. 'The standard model of particle physics is more than a model. It is a detailed thoery that encompasses nearly all that is known about the subatomic particles and forces in a concise set of principles and equations.. back
Links
Aquinas 165 Summa I, 28, 1: Are there real relations in God? 'Reply to Objection 4. Relations which result from the mental operation alone in the objects understood are logical relations only, inasmuch as reason observes them as existing between two objects perceived by the mind. Those relations, however, which follow the operation of the intellect, and which exist between the word intellectually proceeding and the source whence it proceeds, are not logical relations only, but are real relations; inasmuch as the intellect and the reason are real things, and are really related to that which proceeds from them intelligibly; as a corporeal thing is related to that which proceeds from it corporeally. Thus paternity and filiation are real relations in God.' back
Aquinas 20 Summa I, 3, 7: Whether God is altogether simple? 'I answer that, The absolute simplicity of God may be shown in many ways. First, from the previous articles of this question. For there is neither composition of quantitative parts in God, since He is not a body; nor composition of matter and form; nor does His nature differ from His "suppositum"; nor His essence from His existence; neither is there in Him composition of genus and difference, nor of subject and accident. Therefore, it is clear that God is nowise composite, but is altogether simple. . . . ' back
Aquinas 20 Summa: I 3 7: Whether God is altogether simple? 'I answer that, The absolute simplicity of God may be shown in many ways. First, from the previous articles of this question. For there is neither composition of quantitative parts in God, since He is not a body; nor composition of matter and form; nor does His nature differ from His "suppositum"; nor His essence from His existence; neither is there in Him composition of genus and difference, nor of subject and accident. Therefore, it is clear that God is nowise composite, but is altogether simple. . . . ' back
Circle group - Wikipedia Circle group - Wikipedia, the free encyclopedia 'In mathematics, the circle group, denoted by T (or in blackboard bold by ), is the multiplicative group of all complex numbers with absolute value 1, i.e., the unit circle in the complex plane.' back
Clay Millenium Prize - Atiyah Michael Atiyah Lecture back
Clay Millenium Prize - Tate Lecture by John Tate back
Dark energy - Wikipedia Dark energy - Wikipedia, the free encyclopedia 'In physical cosmology & Astronomy, dark energy is a hypothetical form of energy that permeates all of space and tends to increase the rate of expansion of the Universe. Dark energy is the most popular way to explain recent observations that the Universe appears to be expanding at an accelerating rate. In the standard model of cosmology, dark energy currently accounts for 74% of the total mass-energy of the Universe.' back
Diffeomorphism - Wikipedia Diffeomorphism - Wikipedia, the free encyclopedia 'In mathematics, a diffeomorphism is an isomorphism of smooth manifolds. It is an invertible function that maps one differentiable manifold to another, such that both the function and its inverse are smooth. . . . They are Cr diffeomorphic if there is an r times continuously differentiable bijective function between them whose inverse is also r times continuously differentiable. back
Elementary particle - Wikipedia Elementary particle - Wikipedia, the free encyclopedia 'In particle physics, an elementary particle or fundamental particle is a particle not known to have substructure; that is, it is not known to be made up of smaller particles. If an elementary particle truly has no substructure, then it is one of the basic building blocks of the Universe from which all other particles are made. In the Standard Model, the quarks, leptons, and gauge bosons are elementary particles.' back
Gauge boson - Wikipedia Gauge boson - Wikipedia, the free encyclopedia 'In particle physics, gauge bosons are bosonic particles that act as carriers of the fundamental forces of nature.[1][2] More specifically, elementary particles whose interactions are described by gauge theory exert forces on each other by the exchange of gauge bosons, usually as virtual particles.' back
Gauge theory - Wikipedia Gauge theory - Wikipedia, the free encyclopedia 'In physics, gauge theory is a quantum field theory where the Lagrangian is invariant under certain transformations. The transformations (called local gauge transformations) form a Lie group which is referred to as the symmetry group or the gauge group of the theory. For each group parameter there is a corresponding vector field called gauge field which helps to make the Lagrangian gauge invariant. The quanta of the gauge field are called gauge bosons. If the symmetry group is non-commutative, the gauge theory is referred to as non-abelian or Yang-Mills theory.' back
Goldstone boson - Wikipedia Goldstone boson - Wikipedia, the free encyclopedia 'In particle and condensed matter physics, Goldstone bosons (also known as Nambu-Goldstone bosons) are bosons that appear in models with spontaneously broken symmetry.' back
Google.org Google names Larry Brilliant as Executive Director of Google.org 'Mountain View, CA - February 22, 2006 - Google Inc. (NASDAQ: GOOG) today announced the appointment of Dr. Larry Brilliant as Executive Director of Google.org, which administers Google's philanthropic activities. In this role he will work with the company's co-founders Larry Page and Sergey Brin to define the mission and strategic goals of Google's philanthropy. Dr. Brilliant is a founder and director of The Seva Foundation, a Policy Advisory Council Member at the University of California, Berkeley School of Public Health, and a member of the Strategic Advisory Group of Kleiner-Perkin's Pandemic and Bio-Defense Fund.' back
Google.org Searching for solutions 'Google.org aspires to use the power of information and technology to address the global challenges of our age: climate change, poverty and emerging disease. In collaboration with experienced partners working in each of these fields, we will invest our resources and tap the strengths of Google's employees and global operations to advance our initiatives.' back
Henry IV De Haeretico Comburenda Statutes of the Realm, 2:12S-28: 2 Henry IV: ' . . . and they the same persons and every of them, after such sentence promulgate shall receive, and them before the people in an high place cause to be burnt, that such punishment may strike fear into the minds of others, . . . ' back
Higgs boson - Wikipedia Higgs boson - Wikipedia, the free encyclopedia 'In particle physics, the Higgs boson is a massive scalar elementary particle predicted to exist by the Standard Model. The Higgs boson is the only Standard Model particle that has not yet been observed. Experimental detection of the Higgs boson would help to explain how massless elementary particles can cause matter to have mass. More specifically, the Higgs boson would explain the difference between the massless photon, which mediates electromagnetism, and the relatively massive W and Z bosons, which mediate the weak force. If the Higgs boson exists, it would be an integral and pervasive component of the material world.' back
John Wycliffe - Wikipedia John Wycliffe - Wikipedia, the free encyclopedia 'Chair Jaimin John Wycliffe . . . also spelled Wyclif, Wycliff, Wiclef, Wicliffe, or Wickliffe) (mid-1320s – 31 December 1384) was an English theologian, lay preacher[1], translator and reformist.' back
Ludwig Wittgenstein - SEP Ludwig Wittgenstein (Standord Encyclopedia of Phlosophy) 'Considered by some to be the greatest philosopher of the 20th century, Ludwig Wittgenstein played a central, if controversial, role in 20th-century analytic philosophy. He continues to influence current philosophical thought in topics as diverse as logic and language, perception and intention, ethics and religion, aesthetics and culture.' back
Mass gap - Wikipedia Mass gap - Wikipedia, the free encyclopedia 'In quantum field theory, the mass gap is the difference in energy between the vacuum and the next lowest energy state. The energy of the vacuum is zero by definition, and assuming that all energy states can be thought of as particles in plane-waves, the mass gap is the mass of the lightest particle. Since exact energy eigenstates are infinitely spread out and are therefore usually excluded from a formal mathematical description, a more pedantic definition is that the mass gap is the greatest lower bound of the energy of any state which is orthogonal to the vacuum.' back
Method of Fluxions - Wikipedia Method of Fluxions - Wikipedia, the free encyclopedia 'Method of Fluxions is a book by Isaac Newton. The book was completed in 1671, and published in 1736. Fluxions is Newton's term for differential calculus (fluents was his term for integral calculus). He originally developed the method at Woolsthorpe Manor during the closing of Cambridge during the Great Plague of London from 1665 to 1667, but did not choose to make his findings known (similarly, his findings which eventually became the Philosophiae Naturalis Principia Mathematica were developed at this time and hidden from the world in Newton's notes for many years).' back
Qubit - Wikipedia Qubit - Wikipedia, the free encyclopedia 'A quantum bit, or qubit . . . is a unit of quantum information. That information is described by a state vector in a two-level quantum mechanical system which is formally equivalent to a two-dimensional vector space over the complex numbers. Benjamin Schumacher discovered a way of interpreting quantum states as information. He came up with a way of compressing the information in a state, and storing the information on a smaller number of states. This is now known as Schumacher compression. In the acknowledgments of his paper (Phys. Rev. A 51, 2738), Schumacher states that the term qubit was invented in jest, during his conversations with Bill Wootters.' back
Renormalization - Wikipedia Renormalization - Wikipedia, the free encyclopedia 'In quantum field theory, the statistical mechanics of fields, and the theory of self-similar geometric structures, renormalization refers to a collection of techniques used to take a continuum limit.' back
Spontaneous symmetry breaking - Wikipedia Spontaneous symmetry breaking - Wikipedia, the free encyclopedia 'Spontaneous symmetry breaking in physics takes place when a system that is symmetric with respect to some symmetry group goes into a vacuum state that is not symmetric. At this point the system no longer appears to behave in a symmetric manner. It is a phenomenon that naturally occurs in many situations. The symmetry group can be discrete, such as the space group of a crystal, or continuous (i.e. a Lie group), such as the rotational symmetry of space.' back
Tensor - Wikipedia Tensor - Wikipedia, the free encyclopedia 'A tensor is an object which extends the notion of scalar, vector, and matrix. The term has slightly different meanings in mathematics and physics. In the mathematical fields of multilinear algebra and differential geometry, a tensor is a multilinear function. In physics and engineering, the same term usually means what a mathematician would call a tensor field: an association of a different (mathematical) tensor with each point of a geometric space, varying continuously with position.. back
Wu-Ki Tung Bjorken scaling - Scholarpedia 'Bjorken Scaling refers to an important simplifying feature (scaling) of a large class of dimensionless physical quantities in elementary particles, notably the structure functions in deep inelastic scattering, that implies observed strongly interacting particles (hadrons) are made of point-like constituents. It was first proposed by James Bjorken in 1968. This idea, along with the contemporaneous concept of partons by Feynman, and the subsequent experimental discovery of (approximate) scaling behavior, inspired the formulation of Quantum Chromodynamics (QCD), the modern fundamental theory of strong interactions, in 1974. Bjorken scaling is, however, not exact; it is mildly broken. The QCD theory can predict the logarithmic scale-breaking behavior of the relevant physical quantities; and these predictions have been fully confirmed by modern high energy experiments.' back
Yang-Mills theory - Wikipedia Yang-Mills theory - Wikipedia, the free encyclopedia 'Yang-Mills theory is a gauge theory of quantum field theory based on the SU(N) group. It was formulated by Yang and Mills in 1954[1] in an effort to extend the original concept of gauge theory for an Abelian group, as was quantum electrodynamics, to the case of a nonabelian group with the intention to get an explanation for strong interactions. This initial idea was not a success as the quanta of the Yang-Mills field must be massless in order to mantain gauge invariance but such massless particles should have had long range effects that are not seen in experiments. So, the idea was put aside till the start of 1960 when the concept of breaking of symmetry in massless theories, initially due to Jeffrey Goldstone, Yoichiro Nambu and Giovanni Jona-Lasinio, with particles acquiring mass in this way, was put forward.' back
Yoichiro Nambu - Wikipedia Yoichiro Nambu - Wikipedia, the free encyclopedia 'Yoichiro Nambu . . . born January 18, 1921) is a Japanese-born American physicist, currently a professor at the University of Chicago. Known for his contributions to the field of theoretical physics, he was awarded the Nobel Prize in Physics in 2008 for the discovery of the mechanism of spontaneous broken symmetry in subatomic physics.' back

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