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Oct
18

Tagged in: SRI Remote Viewing Experiments, Russell Targ, precognition, Nick Herbert, Dean Radin, Central Intelligence Agency

It's easy to argue both sides with statistics. Remember the stats proving smoking was good for u from tobacco companies years ago. I wonder how Dean et-al will respond to Nick's challenge here? Remember Russ Targ's CIA SRI claims on precognitive remote viewing, e.g. Red Chinese nuke test 4 days in advance Of course that's not a good statistical sample.

I don't find Robin's hypothesis convincing, but I am not an expert in statistical design of psychological experiments with living subjects. Also there have been analogous objections to the drug tests and medical investigations that rely on statistics.

Sent from my iPhone in London, Mayfair near the American Embassy.

On Oct 18, 2012, at 6:34 PM, nick herbert <quanta@cruzio.com> wrote:*I've looked over this paper meta-analyzing the "presentiment experiment" and am shocked that such a careful analysis completely ignores one very plausible explanation **for this seeming retrocausal effect--namely Robin's anticipatory expectation informally expressed at http://forums.randi.org/showthread.php?t=123256 but as far as I can tell **never published. Radin claims to have excluded Robin's hypothesis for some of his experiments but I know of no formal replication of Radin's claim. Robin's Hypothesis is a **reasonable and entirely natural possible explanation for the presentiment effect and as such needs to be rigorously excluded before accepting presentiment as a fact. **The case for human presentiment is only as strong as the efforts made by its proponents to rigorously falsify it. The apparent failure to seriously test (or even consider--as in the MTU article) **Robin's anticipatory expectation hypothesis greatly diminishes my faith in presentiment as a real physical effect.**Nick Herbert**http://quantumtantra.blogspot.com*

Aug
13

Tagged in: Quantum Theory, Nick Herbert, David Bohm, Basil Hiley

On Aug 11, 2012, at 1:41 AM, Basil Hiley <b.hiley@bbk.ac.uk> wrote:

On 27 Jul 2012, at 07:00, nick herbert wrote:

On Jul 26, 2012, at 9:50 AM, nick herbert <quanta@cruzio.com> wrote:

1. The oft-cited remark that non-relativistic Bohmian mechanics gives the same result
as conventional QM for all conceivable experiments is plain wrong. The two theories
possess radically different ontologies which lead to radically different consequences.

BH: How can it be wrong? It uses exactly the same mathematics, without the addition or subtraction of any new mathematical structure. Its predicted expectation values found in all experiments are identical to those found from the conventional rules. If you want to criticise it, why not simply say "It adds no new experimental predictions, so why bother with it?" Then you can get into arguments about which interpretation is better in your opinion. Then it is a matter of opinion not experimental science.

JS: However, Antony Valentini's extension does add new predictions consistent with my own independent investigations and also Brian Josephson's which already has observational evidence in its favor (Libet, Radin, Bierman, Puthoff-Targ, Bem)

NH: What exists in QM is a wavefunction, spread out in configuration space
(and this wavefunction is "real" according to PBR). For a given quantum state
all systems represented by that state have the same ontology.

BH: The ontology gives meaning to the notion of a "quantum state". What does it mean to say "For a given quantum state all systems represented by that state have the same ontology"?

NH: What exists in BM is an actual particle which for S-states has the remarkable property
that v=0. In BM all systems represented by the same state are different--their difference (in the
S-state case) being the differing positions of the static electron. A Bohmian S-state
consists of an ensemble of stationary electrons each in a different position whose
position pattern is given by psi squared.

It is this v=0 property of BM S-wave electrons that is used to create counterexamples to the
contention that BM and QM give the same predictions.

1. Muonic Hydrogen. Like t! he electron the muon in the BM picture is stationary. Hence the muon
lifetime in BM is the just the natural lifetime. However in QM the muon has a velocity distribution
so the lifetime is lengthened by relativity. BM and QM predict different lifetimes for the muonic atom. One may object

that I have introduced relativity into a non-rel situation. However the QM and BM states are still non-rel.

The lifetime of the muon can be seen as a measuring device probing the ontology of the muonic hydrogen.

The probe uses a relativity effect to measure a non-rel configuration.

BH: I recall having already answered this criticism some time ago. Time dilation is a relativistic phenomenon so you must use the relativistic Dirac theory in this case.

JS:: Yes, Nick's error here is obvious. He appeals to the wrong equation for the problem. It's a Red Herring.

BH: In the past there I have been entirely happy with the treatment of the Bohm model of the Dirac equation that we have given. However Bob Callaghan and myself have now obtained a new complete treatment of the Dirac equation with which I am completely happy. It uses the Clifford algebra in a fundamental way as it must to link with the known successful spinor structure. See Hiley and Callaghan: Clifford Algebras and the Dirac-Bohm Quantum Hamilton-Jacobi Equation. Foundations of Physics, 42 (2012) 192-208.

DOI: 10.1007/s10701-011-9558-z and in more detail in The Clifford Algebra Approach to Quantum Mechanics B: The Dirac Particle and its relation to the Bohm Approach, (2010) aXriv: 1011.4033.

Our work shows that the Bohm charge velocity of the electron is, in fact, given by v= Psi alpha Psi, where alpha is the Dirac 4x4 matrix, which is related to the Dirac gamma matrices. (See Bohm and Hiley The Undivided Universe, p. 272 for our original treatment which is confirmed by our latest work.) If you now look at the wave function of the ground state of the Dirac hydrogen atom which you can find in Bjorken and Drell p. 55 you will find the electron is moving in the ground state. What is interesting is that when you take this expression and go to the non-relativistic limit you find the velocity is zero, exactly the result that the Schrödinger equation gives. Remember the energy levels calculated from the Schrödinger hydrogen atom are only approximations to those calculated using the Dirac hydrogen atom.

Do you have a reference to the paper that measures the lifetime of the muon in muonic hydrogen? I can't find a good reference to a clean experiment which shows exactly how to measure the time dilation you mention. I have recently written up the details of the calculation that I have outlined above but I would like to add a better reference to the actual measurement.

2. Electron Capture decay. Certain radioactive elements (Beryllium 7, for instance) possess an excess
positive charge and do not have enough energy to decay by positron emission. Instead they capture the
S-state electron which transforms a nuclear proton into a neutron and neutrino (inverse beta decay).
Electron Capture (EC) is a very delicate probe of the ontology of the S-state electron. QM ontology
(all electrons the same) predicts a smooth exponential decay. After many half-lifes all the Be7 is gone.

BM ontology predicts a very different outcome: exponential decay for all electrons located inside the nucleus;

infinite li! fe for stationary Bohmian electrons located outside the nucleus.

BH: You must read past the simple Bohm model introduced in chapter three of our book, "The Undivided Universe". The first ten chapters contain a discussion of the non-relativistic Bohm model. There we show that if you want to apply the theory to problems where the particles interact either with other particle or with fields like the electro-magnetic field, you must introduce an appropriate interaction Hamiltonian. In section 5.3 to 5.5 we show how to deal with a very simple example of two-particle interactions. These sections were written simply to illustrate how the mathematics work and how you can explain the results using the Bohm interpretation. NB the interpretation is only applied after we have solved the Schrödinger equation containing the interaction Hamiltonian. You can't solve these equations exactly so you have to use perturbation theory. Remember the maths is the same as for the standard interpretation. It is the interpretation that is different.

What happens if the interaction Hamiltonian involves the electromagnetic potentials? To discuss interaction with the electromagnetic field you must go to a relativistic theory. This means you must use the Dirac equation. Chapter 12 of our book begins to show you how to do this. The work of Bob Callaghan and myself mentioned above takes this further. What we have done is to discuss the free Dirac electron for simplicity. We simply wanted to show how it worked without introducing more realistic interaction Hamiltonians.

Now let me try to answer your question as to how we deal with electron capture. In order to describe this capture, we have to introduce the appropriate interaction Hamiltonian. What is the appropriate interaction Hamiltonian in this case? To find this we have to go to a review article like "Orbital electron capture by the nucleus" [Rev. Mod Phys. 49 (1977) 77-221]. You will see that the interaction Hamiltonian is a weak electron current-hadron current interaction. You must now put that into the Dirac equation and calculate away. Well the calculations are all done in the Rev. Mod. Phys. paper and all we need to do is to interpret the results according to the Bohm model.

Where your analysis goes wrong is that you assume (1) the non-relativistic theory and (2) there is no interaction between the nucleus and the electron. You can do that to a first approximation to explain the principle of the Bohm model to, say, a first year undergraduate, but you must not say that's all there is. It is not a true reflection of the processes that are involved! There is an interaction between the nucleon and the electron and you must take this into account even in the Bohm model if you want to understand the physics.

If your message is simply to say that the naive Bohm model based on the Schrödinger is inadequate to deal with these problems then I totally agree with you. Bohm and I have always recognised that the '52 work was just a first step. Let me quote from his Causality and Chance book p. 118

“It must be emphasized, however, that these criticisms are in no way directed at the logical consistency of the model, or at its ability to explain the essential characteristics of the quantum domain. Rather they are based on broader criteria, which suggest that many features of the model are implausible and, more generally, that the interpretation proposed in section 4 [of the ‘52 paper] does not go deep enough.”

I thought that in our book, "The Undivided Universe", we made it clear that chapter 3 was a first step. All the remaining chapters were to show how the model was to be developed to meet many different actual situations found in nature. Finally in chapter 15, we outlined what was going to be developed in a second volume, which would probe a much deeper structure but unfortunately Bohm died just as we were finishing the first book.

NH: If these two counter-examples to the QM/BM experimental identity conjecture have been discussed in the literature,

I! am unaware of it. But they should be.

BH: You are quite right, these points should be discussed in the literature. Unfortunately I have been too involved in developing the ideas outlined in chapter 15 and that means going deeper into what I think really underlies quantum phenomena. You will find some of this work in the latest publications of mine which are accessible on the net. A good place to find a comprehensive review of my latest efforts is in my paper Process, Distinction, Groupoids and Clifford Algebras: an Alternative View of the Quantum Formalism, in New Structures for Physics, ed Coecke, B., Lecture Notes in Physics, vol. 813, pp. 705-750, Springer (2011). Unfortunately I don't think it is available on the net at present but if you are interested I can send you a copy.

Thank you for your interest in our work.

Basil.

Nick Herbert

Jul
27

Tagged in: Nick Herbert, David Bohm

Nick, that is a Red Herring. The bare Bohm model you cite never claims to be a complete theory. Indeed, I suspect the problem you raise below was one of the reasons Vigier introduced the quantum noise - sub-quantal Brownian motion terms. Decay of unstable real particles is a zero point vacuum fluctuation effect not found in bare non-relativistic quantum mechanics.

For example, the bare Dirac equation does not give the Lamb shift and the magnetic moment of the electron correctly - you need QED radiative correction. Same idea here for bare Bohm theory. It's only the zero order starting point so to speak.

In any case, Basil will correct me if my memory here is mistaken?

On Jul 26, 2012, at 12:42 PM, nick herbert <quanta@cruzio.com> wrote:*If these two BM examples have been treated**in the literature I am not aware of it.**You are more knowledgable than I.**Please cite references.**Note that ordinary QM treats these two problems **quite simply without recourse to zero-point fluctuations.*

Jack: No, I don't think so. You must couple the atomic electron Hamiltonian to a random EM field ~** j**.**A**zpf mimicking virtual photons to compute decays if you don't use QED.

In other words, if you simply start with

H0 = p^2/2m + e^2/r

where m is the muon mass & r is the relative coordinate

you cannot calculate the decay of the muon in orthodox QM without adding some Hint to H0. So it comes down to the same thing in essence no matter which interpretation you use.

Nick: *I am interested in reading Vigier's BM description **of these two experiments to see if his method**does indeed, as you are apparently claiming, **give the same results as non-relativistic QM.*

On Jul 26, 2012, at 11:55 AM, JACK SARFATTI wrote:*On Jul 26, 2012, at 9:50 AM, nick herbert <quanta@cruzio.com> wrote:**1. The oft-cited remark that non-relativistic Bohmian mechanics gives the same result **as conventional QM for all conceivable experiments is plain wrong. The two theories **possess radically different ontologies which lead to radically different consequences.**What exists in QM is a wavefunction, spread out in configuration space **(and this wavefunction is "real" according to PBR). For a given quantum state **all systems represented by that state have the same ontology.**What exists in BM is an actual particle which for S-states has the remarkable property **that v=0. In BM all systems represented by the same state are different--their difference (in the **S-state case) being the differing positions of the static electron. A Bohmian S-state **consists of an ensemble of stationary electrons each in a different position whose **position pattern is given by psi squared.**It is this v=0 property of BM S-wave electrons that is used to create counterexamples to the **contention that BM and QM give the same predictions.**1. Muonic Hydrogen. Like the electron the muon in the BM picture is stationary. Hence the muon **lifetime in BM is the just the natural lifetime. However in QM the muon has a velocity distribution **so the lifetime is lengthened by relativity. BM and QM predict different lifetimes for the muonic atom. One may object** that I have introduced relativity into a non-rel situation. However the QM and BM states are still non-rel The lifetime of the muon can be seen as a measuring device probing the ontology of the muonic hydrogen.** The probe uses a relativity effect to measure a non-rel configuration.*

Nick, you have neglected coupling to the zero point vacuum fluctuations that trigger when the unstable particle decays. The unstable real particle gets a kick from a virtual particle giving it a velocity. I think this is done explicitly in Vigier's sub-quantum stochastic Brownian motion addition to the bare NR QM Bohm model you cite. So when you do that everything works. Similarly below.*2. Electron Capture decay. Certain radioactive elements (Beryllium 7, for instance) possess an excess **positive charge and do not have enough energy to decay by positron emission. Instead they capture the **S-state electron which transforms a nuclear proton into a neutron and neutrino (inverse beta decay). **Electron Capture (EC) is a very delicate probe of the ontology of the S-state electron. QM ontology **(all electrons the same) predicts a smooth exponential decay. After many half-lifes all the Be7 is gone.**BM ontology predicts a very different outcome: exponential decay for all electrons located inside the nucleus;**infinite life for stationary Bohmian electrons located outside the nucleus.**If these two counter-examples to the QM/BM experimental identity conjecture have been discussed in the literature, **I am unaware of it. But they should be.**Nick Herbert**KISS MY BARE ART*