Thank you for your good questions

The definition os the holographic princple I used in the essay is "The

amount of information in any volume of space must be limited by the area of a surface that encompasses it" Stringer and weaker version of the principle exist.

Information is just answers to questions we can ask about the world around us, such as the state of a particle.

Ina unified theory there are not really different fields. They are all different aspects of one field, so the type of information is also unified.

The gravitational field seems special because it is connected to geometry of space-time. All fields interact with gravity to information is all fields is limited by the holographic principle. A black hole must form when informnation density exceeds the holographic bound no matter what form it takes.

P and CP symmetry are broken in nature but CPT symmetry is always valid.

Breaking T symmetry is therefore the same as breaking CP symmetry but this is a very small effect and probably cannot account directly for the arrow of time. Some people might dispute that and we do not know enough to be sure.

However, the bigger point is that space and time themselves are emergent and the second law of thermodynamics cannot make sense at a level more fundamental than the emergence of time.

I hope this answers your questions. If not please ask again.

Dear Philip

Thank you for explanation.

Do you know Who is Warren McCuloch?

Dr. McCulloch's researches uniquely exemplify the modern interdisciplinary approach. During his long and distinguished career in neurology

and related disciplines he has also applied his talents in modern

mathematics, symbolic logic, information theory, cybernetics, medicine, the classics and the history and philosophy of science.

This is one among his many interesting articles.

http://www.vordenker.de/ggphilosophy/mcculloch_what-is-a-number.pdf

Yuri

Philip,

Thank you for your reply.

What is "holographic" in the holographic principle?

Just to be clear, you confirmed that a volume of space with enough signals passing through it could become a black hole.

if this volume has a material in it could this information be sound as well as EM? Could this space be a vacuum?

Jeff

As I go on to explain in the essay the entropy bound means that the information in a volume of space must be described by states on the boundary. This is the sense in which it is holographic, just as a hologram can build a 3D picture from a flat surface.

The information can indeed be included in sound waves but the information in the medium carrying the sound waves will be much more than the information in the sound waves themselves.

Whether it can be a vacuum depends on what you mean by vacuum. If you mean an absence of matter then electromagnetic radiation can travel through a vacuum but sometimes in particle physics we take the vacuum to mean flat space with no matter or radiation of any kind. In this case it contains no information.

Hello Philip, What an excellent essay! Very deep and elemental in nature with a lot of killer maths. I learned from you about Carl von Weizsäcker and his theory "that builds infinite dimensional symmetries using layers of quantisation from information" I have similar idea that in KQID, our Ancestor FAPAMA Qbit can split itself up infinitely without cost to itself and to our Multiverse. However, I concluded that Wheeler did not go far enough that not only "it from bit" but also that "it is bit and bit is it." I did rank highly of your essay, if you have time please look at and rank my essay Child of Qbit in time. Best wishes, Leo KoGuan

    Philip,

    "However, the bigger point is that space and time themselves are emergent and the second law of thermodynamics cannot make sense at a level more fundamental than the emergence of time." By more fundamental do you mean smaller scale of size and larger energies? Quantum Mechanics is statical in its results as is statical mechanics. We can run particle interactions very high energy densities; we currently cannot run something like a stream engine at gamma ray blackbody temperatures. The law of thermal dynamics should hold at the scale of nuclear reactions in the core of stars were temperatures and densities are at this level.

    Jeff

    Dear Philip,

    I completely agree with your overarching point that we need consistency to guide our approach to help us gain further insights into the fundamentals of nature. It struck me, though, that when you gave the examples of Maxwell, Einstein and Dirac, these were in a sense completely different situations from the one that relies on arguments pertaining to black holes to derive new consistency-based insights.

    In each of the historic cases, there was at least a prospect that the assumptions on which the consistency-based arguments rested could eventually be checked by experiment. What prospect do we have for that when it comes to black holes? The power of the consistency-based arguments we derive from these assumptions is only as great as the consistency of the assumptions themselves. It seems to me that if we cannot check our most basic assumptions about black holes experimentally, then there is a real danger that we could have overlooked inconsistencies in them, and will continue do so. This could then lead us to derive false arguments even though they are consistent with the assumptions. Instances like the recent firewall debate only strengthen my suspicion that this may in fact be the case.

    It seems to me that a more reliable way to use consistency as a guiding principle would be to apply it to a situation that has at least a fighting chance to be eventually subjected to experimental test. I agree that it is not easy to find such situations where both GR and QT come into play, but consistency-based arguments based on that kind of a situation would seem that much more compelling.

    As you may know, I am also pursuing an idea based on the notion that spacetime emerges from a lower-dimensional analog, namely that quantum theory tells us that pre-measurement states are spacetime manifestations of lower-dimensional objects and that a "measurement" is really the mechanism by which actual spacetime objects emerge out of these. Several people have told me that this reminds them of the holographic principle, although I am myself remain skeptical of that. It is good, though, that you explore the holographic principle from an angle that others have apparently neglected, as hopefully this will increase the chance the whole issue will be more clearly defined. Why do you think is it the case that over the last 20 years, the application of necklace lie algebras has not been taken up by the string theory community?

    All the best,

    Armin

      Jeff, I think that space and time will break down at temperatures and densities around the Plank scale. Theory suggests a Hagdorn temperature for quantum gravity analogous to the one for QCD at much lower temperatures. This is responsible for emergence of space and time. It is a temperature many orders of magnitude higher than those reached in stars or particle accelerators, even in neutron stars and gamma ray bursts. The second law of thermodynamics is safe for anything we are ever likely to observe but conceptually we need to understand how that works.

      Armin, I was coincidentally reading your essay today so I am happy to find your comment here.

      The examples of Maxwell, Einstein, Dirac and Higgs are some of the best examples from history of how logical consistency has been used by theorists. I agree that the circumstances have changed in that further experimental data is lacking for quantum gravity, but that is precisely why consistency is now so important.

      I do think that whatever we conclude will eventually be confirmed by observation but the time scale is goinf to be much larger because it is difficult to reach the energy scales required. Nevertheless there are people looking for possibilities in quantum gravity phenomenology.

      Of course it would be better if some theory could shed light on dark matter or inflation in a way that we could test, but there are people looking at that too. It is not a choice of one or the other. For some reason we seem to be able to make more promising progress on questions that relate to the highest possible energies at this time. Perhaps that will change.

      "Why do you think is it the case that over the last 20 years, the application of necklace lie algebras has not been taken up by the string theory community?"

      This is an interesting question but I think the simple answer is that I have not found a convincing enough case to get them interested. There are so many ideas around that might be important that it is hard to get people interested unless there is something really obvious that makes it look important.

      Sometimes a mathematical idea can hang around for years looking interesting before people find the right way to use it. A good example is twistor theory invented by Penrose years ago. Most people gave up on it but a few kept going. Andrew Hodges developed a complex diagramatic system for physics based on twistors but nobody paid any attention until Witten applied twistors to string theory a few years ago. A group of theorists then started to use it on super Yang-Mills theory. According to Nima Nima Arkani-Hamed they started to develop a new diagramatic approach for this and then noticed that some of their diagrams looked like the ones drawn by Hodges whose theory they could not really understand at that time. So they looked at some of his more complex diagrams and asked what they would mean in their new theory of super yang-mills. Suddenly everything made sense and they were able to move forward much quicker.

      Now they understand it all in terms of invariants of an infinite dimensional Yangian symmetry which had previously been used to understand integral models of spin chains. These things are tantalizingly close to my necklace lie algebras but so far no cigar. It would certainly be amusing if someone wrote down the same definitions as I used twenty years earlier as a solution to the corresponding problem in string theory, but it is more likely that it will be something else

      Philip,

      Thank you for answering my questions. Your answers were well thought out and went in a completely different direction from what I imaged. I was very surprised by the black holes created by crossed information beams. I would have bet against you stating that the second law of thermodynamics survives nearly to the plank scale. I am glad I asked these questions. It looks like your essay is doing well, remember us little people when you win.

      Jeff

      Philip,

      I very much enjoyed reading your essay. Your application of Lie algebras to formulate how spacetime emerges from quantized charges of the symmetry hidden in holography is very intriguing.

      It is also possible to consider the momentum/energy information in a black hole and the lost spacetime information as reciprocal measures of entropy. In this way spacetime emerges from the hidden symmetry of entanglement entropy via the conditional entropy of the local observer.

      Conversely, a compactification of spacetime leads to a dimensional collapse from 4D to 2D (CFT) to 1D in the bulk towards a point singularity. (See my essay "A Complex Conjugate Bit and It".)

      Best wishes,

      Richard Shand

        Hi Philip,

        Terrific to see a way to discretize String Theory. Now if only we could find proof of String Theory... :)

        You wrote:

        1. "The lesson to be taken from holography is that there is a huge hidden symmetry in physics that nobody has yet appreciated."

        What do you think of Bobylev and Vilasi's Projective Invariance as a candidate symmetry? Their paper is not well-known as they published in an obscure journal that soon went under. Luckily, it survives in cyberspace.

        2. "Some observational input on phenomenology of quantum gravity would help but for now everything we can measure is adequately explained by the physics of quantum mechanics, general relativity, thermodynamics, and the standard model of particle physics."

        Quite an optimistic view in the face of multiple foundational cosmological issues regarding Dark Matter, Dark Energy, Inflation, quasar energies, CMB anisotropy, etc! In my essay, Software Cosmos I work out a holonomic model (in the sense of David Bohm and Basil Hiley) that utilizes the Projective Invariance symmetry to address some of these cosmological problems. Hope you get a chance to take a look...

        Hugh

          Hugh thanks for your comments and questions.

          I had not seen the paper of Bobylev and Vilasi. It should be interesting in the context of the systems they describe. The symmetry appears to use 2D Mobius transforms which are part of conformal invariance. This is a very important symmetry in quantum field theories of massless particles. In super yang mills theory there is a dual conformal invariance which conbines with ordinary invariance to give a larger symmetry which can be used to solve the theory in the planar limit and perhaps beyond. In quantum gravity an even larger symmetry is needed to explain holography but projective mathematics surely plays its part.

          I agree that Dark Matter, Inflation etc are big issues that need to be solved but they have not been much help to quantum gravity and I do not mention in my essay.

          I will take a look at your essay to see how you use projective invariance in relation to these problems.