[General] Reply of comments from what a model…

Albrecht Giese genmail at a-giese.de
Thu Dec 10 11:58:59 PST 2015


Hi John,

who should have a 4-momentum? Not clear to me.

Albrecht


Am 10.12.2015 um 08:40 schrieb John Williamson:
> Hi Albrecht,
>
> Yes, did he not say that it would only be in agreement if there was no 
> 4-momentum in them? That they have zero energy-momentum is just the 
> same as saying that they are, effectively, not there at all.
>
> Cheers, John.
> ------------------------------------------------------------------------
> *From:* Albrecht Giese [genmail at a-giese.de]
> *Sent:* Wednesday, December 09, 2015 9:41 PM
> *To:* John Williamson; Nature of Light and Particles - General Discussion
> *Cc:* Mark, Martin van der; Nick Bailey; David Williamson; 
> pete at leathergoth.com
> *Subject:* Re: [General] Reply of comments from what a model…
>
> Dear John,
>
> thank you, and some comments from my part below in the text.
>
> Am 07.12.2015 um 09:32 schrieb John Williamson:
>> Dear Albrecht,
>>
>> Let me help a little: this is off the top of my head - but will give 
>> the right ballpark.
>>
>> The strong interaction (for nucleons) has a coupling constant about a 
>> hundred times bigger than EM. Interaction probabilities need 2 
>> particles so this is about ten thousand times (coupling constant 
>> squared) bigger than EM.
>>
>> This is not a "small effect". Believe me - if they were there for 
>> leptons DESY would have noticed. Even more so we at the EMC (European 
>> Muon Collaboration) would have noticed if they were there for muons. 
>> They are not. You can believe this if you like, but you are wrong.
> The strong force binds the nuclei in the atom and binds the quarks in 
> a nucleus. They have to be bound in a way that they do not touch each 
> other. This is like the atoms in a molecule which are also bound to 
> each other in a way that they do not touch. This is, as we know, 
> achieved by a multipole field. In the molecule it is the van der Waals 
> field based on the electric force. In the nucleus it must be also a 
> multipole field, but based on the strong force. (In nuclear physics 
> this is normally not explained in such a detail but only the result 
> given; this is the typical way in QM).
>
> Such multipole field has a minimum of the potential at a certain 
> distance. This distance defines the distance of the participants. But 
> outside this range the field is still existent; at distance it could 
> decrease by the 1/r^2 law. At least I assume this for my particle 
> model and I see it confirmed by the fact that the Landé factor of the 
> electron has the correct value if I make this assumption.
>
> If now two objects are bound to each other in this way, then the 
> combined field seen from outside has a steeper decrease with r, in the 
> example of my model with 1/r^4 at greater distances. So, if there is 
> an electrical charge in addition, the fall-off at some distance will 
> cause that outside the strong force is in effect weaker than the 
> electrical one.
>>
>> Once again - if there were two bits inside the electron, held 
>> together by whatever forces, we would have seen this. We did not, so 
>> there are not. End of story. The electron, whatever it is, acts as 
>> one thing - at least up to energies up to 400 000 times its mass-energy.
> This is clearly not correct. I have discussed this case with a former 
> research director of DESY. He has spent his entire scientific life 
> with electron scattering experiments and was known for his excellent 
> knowledge of electron experiments all over the world. I could not 
> convince him of my model of a composed and extended electron. But he 
> admitted that there is no experimental evidence which is in conflict 
> with my model. I have explained the reasons in detail here before, so 
> I do not repeat it this time again.
>>
>> There IS something holding the electron charge together though. These 
>> have been, for the last century, designated the "Poincare stresses". 
>> Feynmann talks about these in his lectures. As far as I know, except 
>> for the description in my new papers (the interaction between 
>> electric field and p-vot) and the forces Martin and I have been 
>> calculating with and talking about over the last two decades, these 
>> remain otherwise mysterious. A mystery that endured for most of a 
>> century. In my theory everything is smooth and the whole object is a 
>> single self-confining wave. Just one thing.
> My impression regarding my electron model (which covers also all 
> leptons and all quarks) is a simple and stable model which covers 
> everything understood today and some facts in addition.
>>
>> Sorry if I gave the impression my talk at Mendel was on the proton 
>> size. It was not. I did talk about my model for quarks and the strong 
>> force though, though that is not in the proceedings paper (attached) 
>> which was on a possible reason for the exclusion principle for fermions.
>>
>> There is something on this on the internet in the talk I gave at 
>> CYBCOM, for which Nick Green provided a link earlier.
> Thanks!
>>
>> Regards, John W.
> Regards
> Albrecht
>
>> ------------------------------------------------------------------------
>> *From:* Albrecht Giese [genmail at a-giese.de]
>> *Sent:* Sunday, December 06, 2015 9:29 PM
>> *To:* John Williamson; Nature of Light and Particles - General Discussion
>> *Cc:* Mark, Martin van der; Nick Bailey; David Williamson; 
>> pete at leathergoth.com
>> *Subject:* Re: [General] Reply of comments from what a model…
>>
>> Hello John,
>>
>> there seems indeed something not understood about the reaction 
>> between nucleons (i.e. quarks) and leptons. I have heard about the 
>> differently measured size of a proton depending on whether it is in 
>> contact with electrons or muons. Thanks that you have reminded me of 
>> this.
>>
>> The case of a muon in the atomic orbit, from which a smaller size of 
>> the proton follows, can be at least qualitatively deduced from the 
>> assumption of a strong force in leptons as given in my model. I 
>> should calculate this quantitatively but need some extra time to do 
>> it. Have it on schedule.
>>
>> There is another influence of the assumption of strong force in 
>> electrons in my model. I have shown in my talk in San Diego that the 
>> simultaneous influence of the electrical force and the strong force 
>> explains classically the Landé factor.
>>
>> You write about a talk which you have given about the topic of the 
>> proton's size at MEDEL2012 and about proceedings of it. Could you do 
>> me the favor and give me a link or some other connection to your 
>> contribution?
>>
>> Regards
>> Albrecht
>>
>>
>> Am 01.12.2015 um 01:35 schrieb John Williamson:
>>>
>>> Hello Albrecht,
>>>
>>> Good for you. I knew about this (peripherally) - but would have been 
>>> worried if there had been a direct measurement of leptons feeling 
>>> the "strong force" - which this is not.
>>>
>>> There are a set of these "anomalies". The most important (and oldest 
>>> to my knowledge) is that measured in spin-spin scattering at the ZGS 
>>> (O'Fallon et al 1977). There is another (the EMC effect) with my own 
>>> name on the papers (I am not central to this work and am one of 
>>> dozens of "authors" on the papers: my role was just to write some of 
>>> the code for electromagnetic (QED) shower simulation and for parts 
>>> of a "QCD" monte-carlo used in some of the analysis).
>>>
>>> There are more recent experiments where the proton "size" differs 
>>> (its cross-section - that is the inter-action rate) depending on 
>>> which lepton you observe it with.
>>>
>>> These are all, in my view, down to a lack of understanding as to 
>>> what the "strong" force is. There are no actual calculations for 
>>> this because the only theory we have (QCD) is non-perturbative. I 
>>> will translate (for mothers) "non perturbative" is shorthand for - 
>>> one cannot calculate anything with it using any known techniques. 
>>> Yes - that bad.
>>>
>>> The underlying anomlies all come fron the proper nature of the 
>>> strong force. THis was part of my invited (keynote) talk at 
>>> MENDEL2012 and there is something on this in the proceedings.
>>>
>>> Regards, John.
>>> ------------------------------------------------------------------------
>>> *From:* Albrecht Giese [genmail at a-giese.de]
>>> *Sent:* Monday, November 30, 2015 8:19 PM
>>> *To:* John Williamson; Nature of Light and Particles - General 
>>> Discussion
>>> *Subject:* Re: [General] Reply of comments from what a model…
>>>
>>> Hello John,
>>>
>>> it took me some time to find references, sorry. And I could not find 
>>> the original paper of DESY about it, but a magazine.
>>>
>>> The indication of the strong force to leptons is a more indirect 
>>> conclusion. In 1997 two teams at the HERA storage ring at DESY found 
>>> an unexpected excess of events in quark-positron interactions. These 
>>> events were unexpected as the Standard Model excludes an interaction 
>>> of quarks with leptons on the basis of the strong force. It was then 
>>> made the ad hoc assumption that an unknown particle may exist with 
>>> name leptoquark. Such particle is not excluded by the Standard 
>>> Model, and it is assumed to react with leptons and with quarks. The 
>>> following search for leptoquarks at DESY and at other labs was 
>>> without success. So the direct interaction between quarks and 
>>> leptons by the strong force will remain as a solution.
>>>
>>> I can give the following references for this:
>>> 1.)  Scientific American, March 24, 1997  about the detection of 
>>> additional events
>>> 2.) "Search for contact interactions, large extra dimensions and 
>>> finite quark radius in /ep /collisions at HERA", ZEUS Collaboration, 
>>> Physics Letters B 591 (2004) 23-41   as an example for the search 
>>> for leptoquarks.
>>>
>>> But I would like to emphasize again that the assumption for the 
>>> strong force in e.g. the electron makes it possible to deduce the 
>>> inertial mass of this particle (as also of others). I do not know 
>>> any other approach which provides an origin of inertia deduced from 
>>> basics.
>>>
>>> Regards
>>> Albrecht
>>>
>>>
>>> Am 27.11.2015 um 03:46 schrieb John Williamson:
>>>> Hello Albrecht,
>>>>
>>>> So the strong force has been observed to act on electrons at DESY? 
>>>> Very interesting. Do you have a reference for that?
>>>>
>>>> Regards, John.
>>>> ------------------------------------------------------------------------
>>>> *From:* General 
>>>> [general-bounces+john.williamson=glasgow.ac.uk at lists.natureoflightandparticles.org] 
>>>> on behalf of Albrecht Giese [genmail at a-giese.de]
>>>> *Sent:* Thursday, November 26, 2015 4:53 PM
>>>> *To:* Richard Gauthier
>>>> *Cc:* Nature of Light and Particles - General Discussion
>>>> *Subject:* Re: [General] Reply of comments from what a model…
>>>>
>>>> Hallo Richard,
>>>>
>>>> thank you for your alternative proposal. Unfortunately there are 
>>>> some points of misunderstanding with respect to my model. And also 
>>>> some other physical arguments I like to point to - in your text.
>>>>
>>>> Am 23.11.2015 um 19:43 schrieb Richard Gauthier:
>>>>> Hello Albrecht,
>>>>>
>>>>>     I’m glad that you say that developing a 2-particle model of 
>>>>> the electron was not your main interest. I think it will be useful 
>>>>> to see what parts of your model may be saved, and what parts may 
>>>>> have to go, to get a working model in progress for the electron 
>>>>> which most of us here might agree on. First, since there is no 
>>>>> generally accepted evidence of a nuclear strong force relation to 
>>>>> electrons, let’s drop that proposal for holding your 2 circulating 
>>>>> charged massless particles in orbit, at least for now.
>>>> Here I object. 1) The strong force in the electron was seen at DESY 
>>>> experiments in the 1990s. 2) Without referring to the strong force, 
>>>> the calculation of the mass of the electron has incorrect results 
>>>> by a factor of several hundred. This was found out by physicists in 
>>>> the 1940s, e.g. by Helmut Hönl. (I can send you his paper if you 
>>>> are interested, however in German.)
>>>>> Second, since there’s no evidence for a two-particle structure of 
>>>>> the electron from any scattering or other experiments, let’s also 
>>>>> consider dropping that proposal for now. Your insistence that a 
>>>>> 2-particle model is required for conservation of momentum at the 
>>>>> sub-electron level does not seem sufficient to accept this part of 
>>>>> your 2-particle model. We don’t even know experimentally that 
>>>>> conservation of momentum exists at the sub-electron level, do we? 
>>>>> Just an article of faith?
>>>> This may be a point of personal judgement, but in my view the 
>>>> conservation if momentum is a fundamental law in physics, maybe the 
>>>> most fundamental law. It follows logically from the symmetry of 
>>>> space (refer to Emmy Noether, who has set some logical basics for QM).
>>>>>
>>>>>     So what is left of your model? You claim that your two 
>>>>> particles are massless and travel at light speed.  But you don’t 
>>>>> say that they are also without energy, do you? If there are two 
>>>>> massless particles, they will still each have to have 0.511/2  MeV 
>>>>> of energy if the electron’s total resting energy 0.511 MeV is 
>>>>> divided equally between them.
>>>> I have explained this in a former comment. The two "basic" 
>>>> particles do not have any energy by themselves. The energy is 
>>>> caused by the motion of the basic particles in the situation of a 
>>>> bind. Mass is anyway a dynamic property of matter as it is even 
>>>> seen by present main stream physics.
>>>>> One kind of particle that has no rest mass but has energy and 
>>>>> travels at light speed is a photon.
>>>> This assumption is not true as explained above.
>>>>> (Let’s forget about gluons here for now since there is no accepted 
>>>>> evidence for a strong nuclear force on electrons). So each of your 
>>>>> two particles (if there are still two for some other reason 
>>>>> besides conservation of momentum, and a need for an attractive 
>>>>> force between them to overcome their electric repulsion) could be 
>>>>> a charged photon (circulating charge is necessary to get a 
>>>>> magnetic moment for the model) with energy 0.511/2 MeV, which has 
>>>>> energy but no rest mass. OK.
>>>> Not true!
>>>>> But each of these two charged photons, each of energy 0.511/2 MeV 
>>>>> = mc^2/2 will have a wavelength of 2 Compton wavelengths = 2 h/mc 
>>>>> . If 1 wavelength of each photon is turned into a single closed 
>>>>> loop, the each loop would have a radius 2hbar/mc, which is twice 
>>>>> the radius hbar/mc of your proposed electron model. To make each 
>>>>> of these photons move circularly in a way that each of their 
>>>>> wavelengths gives a radius of hbar/mc as in your model, each 
>>>>> photon would have to move in a double loop. So there will be two 
>>>>> photons each of energy 0.511/2  moving in a double loop in this 
>>>>> model. This is getting complicated.
>>>> The Compton wavelength has a different origin. It comes from 
>>>> scattering of photons at an electron (example). The Compton 
>>>> wavelength is then the maximum change of the wavelength of the 
>>>> photon in such process. - This wavelength is in this way not any 
>>>> geometrical extension of the electron. Yes, we find this value in 
>>>> some calculations, but we should be cautious to use it for the 
>>>> determination of dimension.
>>>>>
>>>>>    Let’s drop one of the two photons for simplicity (Occam’s razor 
>>>>> put to good use) so that the other photon will have the full 
>>>>> electron energy 0.511 MeV .
>>>> What is the origin of this energy in the photon? And which 
>>>> mechanism causes actually the energy of this photon? A photon can 
>>>> in general have any energy, doesn't it?
>>>>> This photon will now have a wavelength 1 Compton wavelength. If 
>>>>> this 1 Compton wavelength charged photon moves in a single loop it 
>>>>> will create an electron with magnetic moment 1 Bohr magneton and a 
>>>>> spin of 1 hbar. That’s good for the experimental magnetic moment 
>>>>> of the electron (slightly more than 1 Bohr magneton)  but bad for 
>>>>> its experimental spin (which you tried to reduce to 1/2 hbar in 
>>>>> your model by a delayed force argument). If the photon moves in a 
>>>>> double loop it will be good for the spin (which now is exactly 1/2 
>>>>> hbar) but bad for the magnetic moment (now 1/2 Bohr magneton).
>>>> Why does the double loop reduce the spin? Why the Bohr magneton? 
>>>> The magnetic moment depends on the area in the loop. How large is 
>>>> this area in this case?
>>>>
>>>> The magnetic moment is larger than the Bohr magneton. In my model 
>>>> this is the contribution of the (small) electrical charges in view 
>>>> of the (large) strong charges.
>>>>
>>>> And which mechanism causes the double loop? It cannot come from 
>>>> itself. A circuit is a simple structure which does not need many 
>>>> influences. A double loop is more and needs a cause.
>>>>> So there’s still a problem with the model’s magnetic moment. But 
>>>>> this double-looping charged photon model now has gained the 
>>>>> zitterbewegung frequency of the Dirac electron which is desirable 
>>>>> for an electron model which hopes to model the Dirac electron. And 
>>>>> it also has 720 degree symmetry which the Dirac electron has 
>>>>> (while your original 2-particle model has a rotational symmetry of 
>>>>> 180 degrees, since each particle would take the place of the other 
>>>>> after a half-circle rotation).
>>>> In my model the zitterbewegung frequency is the circulation 
>>>> frequency of the basic particles. The rotational symmetry is not 
>>>> 180 but 360 degrees as the strong field of the basic particles is 
>>>> not equal, but one basic particle changes the other one by 
>>>> electrical influence. This works analogue to the case of the van 
>>>> der Waals force.
>>>>>
>>>>>     What do you think of this new model so far?
>>>> Did I explain it sufficiently?
>>>>>
>>>>> Richard
>>>> Albrecht
>>>>>
>>>>>> On Nov 22, 2015, at 9:43 AM, Albrecht Giese <genmail at a-giese.de> 
>>>>>> wrote:
>>>>>>
>>>>>> Hello Richard,
>>>>>>
>>>>>> I never have persistently tried to develop a 2-particle model. 
>>>>>> What I have persistently tried was to find a good explanation for 
>>>>>> relativistic dilation. And there I found a solution which has 
>>>>>> satisfied me. All the rest including the 2 particles in my model 
>>>>>> where logical consequences where I did not see alternatives. If 
>>>>>> there should be a model which is an alternative in one or the 
>>>>>> other aspect, I will be happy to see it.
>>>>>>
>>>>>> Am 22.11.2015 um 00:13 schrieb Richard Gauthier:
>>>>>>> Hello Albrecht,
>>>>>>>
>>>>>>> I admire your persistence in trying to save your doomed (in my 
>>>>>>> opinion) 2-particle electron model.
>>>>>> Why 2 particles in the model? I say it again:
>>>>>>
>>>>>> 1) to maintain the conservation of momentum in the view of 
>>>>>> oscillations
>>>>>> 2) to have a mechanism for inertia (which has very precise 
>>>>>> results, otherwise non-existent in present physics)
>>>>>>
>>>>>> I will be happy to see alternatives for both points. Up to now I 
>>>>>> have not seen any.
>>>>>>> Do you understand how unreasonable and irrational it appears for 
>>>>>>> you to write:   "Then I had to determine the field constant S 
>>>>>>> which is normally provided by experiments. But quantum mechanics 
>>>>>>> is so unprecise regarding the numeric value of the strong force 
>>>>>>> that there is no number available in the data tables. Here I 
>>>>>>> found that I could use the Bohr magneton to determine the 
>>>>>>> constant. (Which turned out to be S = hbar*c, merely a 
>>>>>>> constant).” ?
>>>>>> I have once asked one of the leading theorists at DESY for a 
>>>>>> better quantitative explanation or determination of the strong 
>>>>>> force. His answer: Sorry, the strong force is not good enough 
>>>>>> understood so that I cannot give you better information.
>>>>>>> How could the number S  that you could not find in “unprecise” 
>>>>>>> tables about the strong force possibly be the same number that 
>>>>>>> can be found precisely from the electron’s Bohr magneton 
>>>>>>> ehbar/2m and which you claim is S = hbar*c ? This is an 
>>>>>>> unbelievable, desperate stretch of imagination and "grasping at 
>>>>>>> straws", in my opinion.
>>>>>> When I have realized that my model deduces the Bohr magneton, I 
>>>>>> have used the measurements available in that context to determine 
>>>>>> my field constant. (I could also go the other way: I can use the 
>>>>>> Planck / Einstein relation E = h * f and the Einstein-relation E 
>>>>>> = m*c^2 to determine the constant S from the internal frequency 
>>>>>> in my model. Same result. But I like the other way better. BTW: 
>>>>>> Do you know any other model which deduces these relations rather 
>>>>>> than using them as given?)
>>>>>>>
>>>>>>> Here is the meaning of “grasping at straws” from 
>>>>>>> http://idioms.thefreedictionary.com/grasp+at+straws :
>>>>>>>
>>>>>>>
>>>>>>>     grasp at straws
>>>>>>>
>>>>>>> Also,*clutch at 
>>>>>>> straws*.Makeadesperateattemptatsavingoneself.Forexample,/He had 
>>>>>>> lost the argument, but he kept grasping at straws, naming 
>>>>>>> numerous previous cases that had little to do with this 
>>>>>>> one/.Thismetaphoricexpressionalludestoadrowningperson 
>>>>>>> tryingtosavehimselfbygrabbingatflimsyreeds.Firstrecordedin1534,thetermwas 
>>>>>>> usedfigurativelybythelate1600s.
>>>>>>>
>>>>>>> I am not at all opposed to using desperate measures to find or 
>>>>>>> save a hypothesis that is very important to you. Max Planck 
>>>>>>> described his efforts to fit the black body radiation equation 
>>>>>>> using quantized energies of hypothetical oscillators as an "act 
>>>>>>> of desperation”.  So you are of course free to keep desperately 
>>>>>>> trying to save your 2-particle electron hypothesis. I personally 
>>>>>>> think that your many talents in physics could be better spent in 
>>>>>>> other ways, for example in revising your electron model to make 
>>>>>>> it more consistent with experimental facts.
>>>>>> Do you know any other electron model which is so much consistent 
>>>>>> with experimental facts (e.g. size and mass) as this one (without 
>>>>>> needing the usual mystifications of quantum mechanics)?
>>>>>>>  By the way, van der Waals forces do not "bind atoms to form a 
>>>>>>> molecule". They are attractive or repulsive forces between 
>>>>>>> molecules or between parts of a molecule. According to Wikipedia:
>>>>>>>
>>>>>>> " the *van der Waals forces* (or *van der Waals' interaction*), 
>>>>>>> named after Dutch 
>>>>>>> <https://en.wikipedia.org/wiki/Netherlands>scientist 
>>>>>>> <https://en.wikipedia.org/wiki/Scientist>Johannes Diderik van 
>>>>>>> der Waals 
>>>>>>> <https://en.wikipedia.org/wiki/Johannes_Diderik_van_der_Waals>, 
>>>>>>> is the sum of the attractive or repulsive forces between 
>>>>>>> molecules <https://en.wikipedia.org/wiki/Molecule> (or between 
>>>>>>> parts of the same molecule) other than those due to covalent 
>>>>>>> bonds <https://en.wikipedia.org/wiki/Covalent_bond>, or the 
>>>>>>> electrostatic interaction 
>>>>>>> <https://en.wikipedia.org/wiki/Electrostatic_interaction> of 
>>>>>>> ions <https://en.wikipedia.org/wiki/Ion> with one another, with 
>>>>>>> neutral molecules, or with charged molecules.^[1] 
>>>>>>> <https://en.wikipedia.org/wiki/Van_der_Waals_force#cite_note-1> 
>>>>>>>  The resulting van der Waals forces can be attractive or 
>>>>>>> repulsive.^[2] 
>>>>>>> <https://en.wikipedia.org/wiki/Van_der_Waals_force#cite_note-Van_OssAbsolom1980-2> 
>>>>>>>
>>>>>> Yes, my arrangement of charges of the strong force causes as well 
>>>>>> a combination of attractive and repulsive forces and is doing the 
>>>>>> same like in the van der Waals case. That was my reason to refer 
>>>>>> to them.
>>>>>>
>>>>>> Best regards
>>>>>> Albrecht
>>>>>>>
>>>>>>> with best regards,
>>>>>>>     Richard
>>>>>>>
>>>>>>>
>>
>
>
>
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