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vol VII: Notes

2014

Notes

[Notebook: DB 78: Catholicism 2.0]

[Sunday 28 December 2014 - Saturday 3 January 2015]

[page 73]

Sunday 28 December 2014

Feynman III 2-8; '. . . disturbance is necessary for the consistency of the viewpoint.' Feynman

Feynman pag 2-2: 'uncertainty comes naturally from the wave picture'. [and from the digital picture].

A story: from wave mechanics to computed dynamics. We observe discrete events whose form (eg electron-ness) appears to be defined with infinite precision, ie it is a quantum or unit.

[page 74]

The determinism suggests the presence of a deterministic machine like a computer executing an algorithm. This suggests that we identify the eigenfunctions of wave mechanics with algorithms or computers, and understand the messages emitted by quantum events to be the outcome of these computations when they are halted, so the eigenvalues of an observable [embodied as particles] are the set of halting eigenvalue computations.

We may think of a communication channel as two pairs of to algorithms, each the inverse of the other, processing strings of symbols from clear to code for transmission and code to clear for reception. Shannon coding can render messages strong against corruption, but not absolutely incorruptible as this takes infinite time for a source whose output rate is finite. The only foolproof method is full duplex: the receiver reads the received message back to the transmitter who acknowledges that the returned message is identical to the original. Claude Shannon

Quantum mechanics embodies the 'echo' method of verification symbolized by the computation of probability P = |ψ|2 = ψψ*, the complex conjugate being interpreted as the return message and the probability of a successful communication being measured by the product of the forward and return messages represented by ψ and ψ* respectively, which could equivalently be written ψ*ψ since ψ** = ψ. The computation of the probability is deterministic, ie the computation of the dot product, although the choice of eigenfunction to execute would appear to be a random event. Here, however, we note the observation that a well coded string has maximum entropy and is indistinguishable from noise, except to the transmitter and receiver of the string.

[page 75]

It may be that at the quantum level the Universe is so simple that Shannon coding is not possible because everything is processed one quantum at action at a time and so the only way to see if a communication is successful is the 'echo' method, and this succeeds between various eigenvectors of the measurement operator and the unknown quantum state being measured at a rate given by the Born law. Born rule - Wikipedia

Measurements are normalized because measurement operators are unitary which means that every measurement has one or another outcome whose probabilities, given by the Born law, add up to 1, so that we can treat a quantum measurement as a communication source whose language is determined by the measurement operator in use.

The notion that the observables are the stationary points in the divine dynamics is gradually gaining weight as it becomes more concrete. The world is held together by logical continuity because it is embedded in the one and consistent God. We understand the stationary points by understanding the dynamics of which they are part. In wave mechanics we see the dynamic process as the superposition of infinite dimensional waves, of which we get an occasional snapshot by making an observation. Now we see that there is nothing special about physics, logic or intelligence, it is all part of the logical continuity of the observable fixed points of the logic being manipulated by creation and annihilation of different species at different points in spacetime.

Can we say the fixed points control the dynamics or the dynamics control the fixed points? Both are true. We design the dynamics by designing the fixed points, since it is generally the dynamic process that we want. We set processes in morion by removing the inhibitions so that potentials can act.

[page 76]

My writing flows when I have a sequence of stationary points to record and a clear road ahead. Then we come to the end of the road where new understanding or new creation is required to continue. In time a new step forward will probably appear. I began this story with faith that God and the World are one. The demonstration by fixed point theory that a world complex in fixed points is nevertheless compatible with the completely simple dynamics of the traditional god has opened my faith to a path to understanding. Now I am beginning to see how this can be all fitted together with the theories of computation and communication which tell us how fixed points logically relate to one another, all built into the Cantor universe which shows how large and complex structures can be made by joining smaller points together, as I am a community of atoms, distinct from but mingled with my environment.

Making the observable world out of the fixed points of the divine dynamics carries echoes of Newton's decision to build his celestial dynamics in a space (god's sensorium) fixed by God. Patrick J Connolly

Everything we observe [is] an act, something prior to space and time which we nevertheless experience as embedded in space and time. Quantum theory requires only time, that is sequential ordering to function (?). Periodic functions step out the process of time. An act occupies space and time, as I do. I am a complex act comprising many smaller quanta of action .S, the total quanta of my life, is mc2 . l /h, where l is my lifetime. This works out to about S = 1053.

Entropy is a count of action [complexion]. An act is a fundamental unit, a state, with no dimension other than orthogonality to the rest of the Universe. What is the Cantor universe, a formal

state space, ie a phase space. A space is the set of all its states. The information carried by a point in the space is equal to the entropy of the space ie the number of points it contains. So log(ℵn!) = ℵn.

Monday 29 November 2014
We can only talk about what is observable and speculate about what is invisible. Currently quantum theory posits a world characterized by the deterministic continuous evolution of wave functions which occasionally 'collapse' when they are observed. Because it is continuous motion, we model it with sets whose cardinal is the cardinal of the continuum, which we assume to be 1. The mechanism that makes all these points behave as they do [is mysterious]. Continuous mathematics has been developed over millennia an is thought to be logically sound tat is bound together by logical continua = proofs.

Here we propose a simpler alternative, thst the invisible dynamics is logically rather than geometrically continuous. We do this by assuming that eigenfunctipns are computable functions, so that instead of there being 1 of them there are only 0, that is the number of Turing machines whose algorithm is expressed by a finite ordered set of symbols. Such an algorithm may appear to a casual observer, if it is maximally compressed [by a suitable coding algorithm], as a random sequence of symbols all of which are equiprobable, so maximizing entropy.

If the whole Universe is a computer network, our next task is to see how computer networks create themselves, beginning with nothing from [an] observable point of view (ie the omnino simplex,

[page 78]

continuous) God.

Neuenschwander page 4: ' "Invariant" means a quantity's numerical value is not altered by a coordinate transformation. "Conserved" in contrast, means that within a given coordinate system the quantity doe snot change throughout a process. Neuenschwander

Chaplin, Biography, page 210: 'I did not have to read books to know that the theme of life is conflict and pain.' Not always, there is also harmony and pleasure, which I imagine occupies 90% of my life. Chaplin

'. . . humour . . . ; is the subtle discrepancy we discern in what appears to be normal behaviour.'

Tuesday 30 November 2014

Neuenschwander page 25: Jerry B. Marion: 'In Newtonian mechanics a certain force on a body is considered to produce a definite motion; that is a definite effect is always associated with a certain cause. According to Hamilton's principle, however, the motion of a body ma be considered to result from the attempt of Nature to achieve a certain purpose, namely to minimize the time integral of the difference between kinetic and potential energies.'

Wednesday 31 November 2014
Thursday 1 January 2015

Our human relationships are represented as field of 'force' that guide our behaviour, deciding in a crowded situation who we will dance with, kiss, etc etc. All of tis would seem to be directed by our judgement of whether an interaction will be 'attractive' or not, or maybe productive.

[page 77a]

Neuenschwander page 40: 'The concepts of potential and kinetic energies came along after the concept of force (eg Thomas Young was the first to use the term of "energy" applied to mv2 in 1801-03).

page 46: 'The generalizability of Hamilton's principle to the widest scope of physics , even far beyond mechanics, and its presentation of conservation laws, gives Hamilton's principle a depth and versatility not shared by other mechanical principles.'

Friday 2 January 2015

Albert Camus: Intellectual: 'someone whose mind watches itself '. Bruce Grant

The Lagrangian describes the action. If there is no action, ie the Lagrangian = 0, nothing happens and we have a symmetry, ie a NOP.

The wholeUniverse is one pure act which we see time division multiplexed into the action we see around us, which looks like a massively parallel process but all our local perception of it is time ordered (= serial) communication.

When we say μjμ = 0 we are algebraically adding the flow of action in each dimension to get the total 0, ie the measure of action collapses the structure of spacetime down to a single scalar parameter.

Neuenschwander page 126: "In this chapter we study local gauge invariance. In the analogy it corresponds to rotating the pointer needles by different amounts on different gauges. It may be hard to see how such a transformation can leave anything invariant. But if the gauge needle emits some kind of signal to compensate for its

[page 78a]

rotation, then the coupled system 'gauge + signal' might exhibit some kind of invariance.

Saturday 3 January 2015

Physics uses coordinate systems to study physical systems, but insists that the physics exists independently of the coordinate, so that changing the coordinate system should not change the physics, only the way we look at it. Different coordinate systems may reveal different features of the physics and may hide other features. This notion is supported by the theorem of quantum measurement that tells us that what we see are the eigenvalues of measurement operators, so different operators will reveal different eigenvalues corresponding to the eigenvectors of the operator used. We may think of the observable operator as a reference system. We see a similar sort of behaviour in the senses of different creatures which are sensitive to different features of the environment. In a universe where everything is looking at everything else from its own point of view, can we claim that there is a true point of view that exists independently of observers? Einstein appears to have felt that this is so, but it seems hard to believe in a universe which can be modelled as a layered communication network, since the meaning that a layer may give to the elements of the layer beneath it seems to be pretty much arbitrary. Only at the very lowest level can we expect to find no interpretation effects introduced by the observer, ie we can expect the gravitational structure of the universe to be independent of observers, since gravitation attributes no meaning to actions but sees only their frequency as energy.

Coordinate system - language. As language expands it develops the ability to record more subtle features of human experience and at the same time propagates these experience, increasing their frequency.

[page 79]

Noether Wikipedia: 'Noether's first theorem states that any differentiable symmetry of the action of a physical system has a corresponding conservation law.' Noether's theorem - Wikipedia

Conservation of momentum is a consequence of Newton's third law: action and reaction are equal and opposite. We might se this as an example of duplex communication where we represent the forward and reverse processes (echoes) of a message to be φ and φ*. The probability of the communication succeeding is the product of the forward and reverse probability amplitudes, P = |φ|2 = φφ*.

A large proportion of the mathematical machinery of physics is concerned with the transformation f coordinate systems while preserving the integrity of the physical systems they describe. The aim is to obtain a coordinate free insight into what is happening, ie determine the relationships of elements of the universe to one another without being led astray by coordinates.

The tour de force in this enterprise is the general theory of relativity which identifies the reality and te coordinate system using the metric to translate between actual distances and coordinate distances.

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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!)

Chaplin, Charles, My Autobiography, Simon & Schuster 1978 Amazon Editorial Reviews Book Description Charles Chaplin was born in London in 1889 to actor parents. His career in films started in 1914 with a string of single-reelers for Keystone Comedy Film Company. Success was immediate, and nine years later, to get better terms, he helped form United Artists. Chaplin's life was full of controversy, from his memorable arguments with the government about taxes to his marriage late in life to Oona O'Neill, daughter of playwright Eugene and two generations his junior. By her he sired an extensive brood. She in turn cared for him devotedly through the remainder of his long life (he died on Christmas Day, 1977). "From a destitute childhood in Victorian London to fame without frontiers...one of the success extravaganzas of the century." (Publisher's Source) 
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Crankshaw, Edward, Krushchev, Collins 1966 'Most of the material for my . . . book was gathered over a long period and in a number of countries, above all, of course, the Soviet Union. I cannot thank by name the many who have helped me, and those who still live in Russia and Eastern Europe would not be pleased if I did so. I am grateful to them all the same. It would be pleasant, if, twelve years after Stalin's death, I could acknowledge assistance from 'official' Russians; but from these, as always during the past 25 years, -- save for on startling gesture from Krushchev himself -- there has been nothing but obstruction.'back
Feynman, Richard P, and Robert B Leighton, Matthew Sands, The Feynman Lectures on Physics (volume 3) : Quantum Mechanics, Addison Wesley 1970 Foreword: 'This set of lectures tries to elucidate from the beginning those features of quantum mechanics which are the most basic and the most general. ... In each instance the ideas are introduced together with a detailed discussion of some specific examples - to try to make the physical ideas as real as possible.' Matthew Sands 
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Feynman, Richard P, and Albert P Hibbs, Quantum Mechanics and Path Integrals, McGraw Hill 1965 Preface: 'The fundamental physical and mathematical concepts which underlie the path integral approach were first developed by R P Feynman in the course of his graduate studies at Princeton, ... . These early inquiries were involved with the problem of the infinte self-energy of the electron. In working on that problem, a "least action" principle was discovered [which] could deal succesfully with the infinity arising in the application of classical electrodynamics.' As described in this book. Feynam, inspired by Dirac, went on the develop this insight into a fruitful source of solutions to many quantum mechanical problems.  
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Neuenschwander, Dwight E, Emmy Noether's Wonderful Theorem, Johns Hopkins University Press 2011 Jacket: A beautiful piece of mathematics, Noether's therem touches on every aspect of physics. Emmy Noether proved her theorem in 1915 and published it in 1918. This profound concept demonstrates the connection between conservation laws and symmetries. For instance, the theorem shows that a system invariant under translations of time, space or rotation will obey the laws of conservation of energy, linear momentum or angular momentum respectively. This exciting result offers a rich unifying principle for all of physics.' 
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  back
Zee, Anthony, Quantum Field Theory in a Nutshell, Princeton University Press 2003 Amazon book description: 'An esteemed researcher and acclaimed popular author takes up the challenge of providing a clear, relatively brief, and fully up-to-date introduction to one of the most vital but notoriously difficult subjects in theoretical physics. A quantum field theory text for the twenty-first century, this book makes the essential tool of modern theoretical physics available to any student who has completed a course on quantum mechanics and is eager to go on. Quantum field theory was invented to deal simultaneously with special relativity and quantum mechanics, the two greatest discoveries of early twentieth-century physics, but it has become increasingly important to many areas of physics. These days, physicists turn to quantum field theory to describe a multitude of phenomena. Stressing critical ideas and insights, Zee uses numerous examples to lead students to a true conceptual understanding of quantum field theory--what it means and what it can do. He covers an unusually diverse range of topics, including various contemporary developments,while guiding readers through thoughtfully designed problems. In contrast to previous texts, Zee incorporates gravity from the outset and discusses the innovative use of quantum field theory in modern condensed matter theory. Without a solid understanding of quantum field theory, no student can claim to have mastered contemporary theoretical physics. Offering a remarkably accessible conceptual introduction, this text will be widely welcomed and used.  
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Papers
Heisenberg, Werner, "Quantum Mechanical Re-interpretation of Kinematic and Mechanical Relations", Zeitschrift fur Physik, , 33, 1925, page 879-893. tEnglish translation in B L van der Waerden, Sources of Quantum Mechanics, Dover Publications, New York, 1968, pp 261-276. 'It has become the practice to characterize [the] failure of the quantum-theoretical rules as a deviation from classical mechanics, since the rules themselves were essentially derived from classical mechanics. This characterization has, however, little meaning when one realises that the Einstein-Bohr frequency condition (which is valid in all cases) already represents such a complete departure from classical mechanics, ... that even for the simplest quantum-theoretical problems the validity of classical mechanics simply cannot be maintained. In this situation it seems sensible to discard all hope of observing hitherto unobservable quantities, such as the position and period of the electron, and to concede that the partial agreement of the quantum rules with experience is more or less fortuitous. Instead it seems more reasonable to try to establish a theoretical quantum mechanics, analogous to classical mechanics, but in which only relations between observable quantities occur.' (van der Waerden pp 262-263.). back
Links
Actuarial science - Wikipedia, Actuarial science - Wikipedia, the free encyclopedia, 'Actuarial science is the discipline that applies mathematical and statistical methods to assess risk in the insurance and finance industries. Actuaries are professionals who are qualified in this field through education and experience. In many countries, actuaries must demonstrate their competence by passing a series of rigorous professional examinations. Actuarial science includes a number of interrelating subjects, including probability, mathematics, statistics, finance, economics, financial economics, and computer programming.' back
Born rule - Wikipedia, Born rule - Wikipedia, the free encyclopedia, 'The Born rule (also called the Born law, Born's rule, or Born's law) is a law of quantum mechanics which gives the probability that a measurement on a quantum system will yield a given result. It is named after its originator, the physicist Max Born. The Born rule is one of the key principles of the Copenhagen interpretation of quantum mechanics. There have been many attempts to derive the Born rule from the other assumptions of quantum mechanics, with inconclusive results. . . . The Born rule states that if an observable corresponding to a Hermitian operator A with discrete spectrum is measured in a system with normalized wave function (see Bra-ket notation), then the measured result will be one of the eigenvalues λ of A, and the probability of measuring a given eigenvalue λi will equal <psi,|Pi|psi> where Pi is the projection onto the eigenspace of A corresponding to λi'. back
Bruce Grant, Leaders must choose the right indset for 21st century Asia Pacific, 'I have been wondering lately why, after a lifetime of watching political leaders, national and international, I do not trust Tony Abbott, even when I agree with what he is saying or doing, while I trust Barack Obama, even when I don't like what he is saying or doing.' back
Claude Shannon, Communication in the Presence of Noise, 'A method is developed for representing any communication system geometrically. Messages and the corresponding signals are points in two “function spaces,” and the modulation process is a mapping of one space into the other. Using this representation, a number of results in communication theory are deduced concerning expansion and compression of bandwidth and the threshold effect. Formulas are found for the maximum rate of transmission of binary digits over a system when the signal is perturbed by various types of noise. Some of the properties of “ideal” systems which transmit at this maximum rate are discussed. The equivalent number of binary digits per second for certain information sources is calculated.' back
Noether's theorem - Wikipedia, Noether's theorem - Wikipedia, the free encyclopedia, 'Noether's (first) theorem states that any differentiable symmetry of the action of a physical system has a corresponding conservation law. The theorem was proved by German mathematician Emmy Noether in 1915 and published in 1918.[1] The action of a physical system is the integral over time of a Lagrangian function (which may or may not be an integral over space of a Lagrangian density function), from which the system's behavior can be determined by the principle of least action.' back
Patrick J Connolly, Newton and God's Sensorium, Abstract: ' In the Queries to the Latin version of the Opticks Newton claims that space is God’s sensorium. Although these passages are well-known, few commentators have offered interpretations of what Newton might have meant by these cryptic remarks. As is well known, Leibniz was quick to pounce on these passages as evidence that Newton held untenable or nonsensical views in metaphysics and theology. Subsequent commentators have largely agreed. This paper has two goals. The first is to offer a clear interpretation of Newton’s claim about space and God’s sensorium by situating those claims within Newton’s philosophical thought. The second is to show how my interpretation rescues Newton from Leibniz’s critiques. . . . ' back

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