The church of SM physics

  • The attempt at complexity is laudable, but all that work could have been applied to… maybe… a signal or two that theory suggests, in order to support such a theory. But if the preferred path is wandering in the rough filling pails with golf balls when one should find their own ball and play on, then continue on…

  • . But if the preferred path is wandering in the rough filling pails with golf balls when one should find their own ball and play on, then continue on…

    Maybe its time for P to read at least one of the 2o pages of text rather than wandering/blathering on?

    with its own soft....

    that would be respectful..

    https://www.researchgate.net/publication/356972251_A_new_experimental_path_to_nucleosynthesis

  • Here is a diagram to better illustrate my concerns about Wyttenbach's use of his peak-finding algorithm when the detector he is using has a relatively poor resolution (relative, that is, to the spacings of the peaks he is claiming to identify).


    I have taken the background-subtracted spectra shown in Figure 1 from Wyttenbach's manuscript and first (top panel) superimposed a Gaussian distribution scaled to a width of about 10 keV which I suppose is about the minimal resolution for a single spectral peak in Wyttenbach's setup. The bottom panel is similar but shows what would be the expected if one had 2 sets of gamma signals 10 keV apart.



    Main conclusions here are

    1) The wiggles on top of the spectra, apparently regarded as separate peaks by Wyttenbach, go up and down faster that one would expect given the resolution of the detector used,

    2) A single spectral line strong enough to be identified as such by Wyttenbach's peak-finding algorithms could also contribute counts to perhaps 20 or more neighbouring bins (bins are about 0.6 keV wide here). Would the algorithm then identify these as separate peaks?

    3) For situations with multiple genuine gamma signals separated by 10 keV, virtually all spectral bins between the actual signal energies have counts almost as high as the centre peaks. Lots of room for false positives here.


    In his manuscript, Wyttenbach says " ... if you understand gamma spectroscopy then you know that gamma lines usually are very precise and a peek does not spawn [sic] dozens of keV." [Note: I think that "spawn" is a typo and should actually read "span"]. It seems to me that Wyttenbach may be wrong here and that the finite resolution of his detector may indeed result in a peak spanning dozens of keV. I would like to see this problem addressed.

  • I have taken the background-subtracted spectra shown in Figure 1 from Wyttenbach's manuscript and first (top panel) superimposed a Gaussian distribution scaled to a width of about 10 keV

    You mix up a back scattering peek or a high energy peek with a low energy peek. A high energy photon is also back scattered in the detector itself. So your peek in part is a detector artifact. The peeks you think of only occur if we have a very high ( 1'000.. 10'000) count/s. So now you can look up the probability effect of a single line being exactly where it should be if it enters a detector at a random time.


    Sometimes a lower sensitivity is just the best you can have...The other thing is: the Quartz/ceramic tube acts like a filter as only the full energy lines can pass lower energies are highly suppressed.

  • Russ and I calibrated the Theremino GS with several isotopes including Cs137, K40 and Thorium.

    OK. But I assume you mean calibrated for energy scale and I haven't really been concerned about that yet. I have been addressing issues surrounding the minimal resolution of the system.


    If you saved some of the calibration data, the measured Full Width at Half Maximum of the photopeak may yield an empirical estimate of the actual obtained resolution.

  • You mix up a back scattering peek or a high energy peek with a low energy peek. A high energy photon is also back scattered in the detector itself. So your peek in part is a detector artifact. The peeks you think of only occur if we have a very high ( 1'000.. 10'000) count/s. So now you can look up the probability effect of a single line being exactly where it should be if it enters a detector at a random time.

    I'm afraid I don't understand what you are saying here. The best I can make out is that you are saying that part of the spectra at low energies in your Figure 1 are due to various artefacts from scattering of higher energy photons that could not be background subtracted because they did not occur in the background. Is that right? Should I have therefore drawn my peaks like this?


    Or maybe avoided the lowest energies like this?

    I don't see how either of these scenarios would address my concern about how your peak-locating algorithms my falsely identify lines that are spread out by the finite resolution of the system.

  • as far as I am aware

    Probably sintered? similar to Arata's stuff

    probably variable in output which is why different mixes are being explored


    the REEs appear to be the gamechaging addition...there might be ZrO2 simillar to Arata's ,,

    might have been sourced from the history of LENR..R&D

    Mischmetal... Kidwell's work with Gd. definitely the rhodium was worked on at SPAWAR


    Future optimised formulations will be guided by the gamma spec work + calorimetry


    Gd + Sm look promising... I have informed other researchers about that..


    The gamma spec approach looks promising..

    used sporadically ...in prior LENR R&D without intricate analysis


    Hagelstein came up with interesting gamma to phonon conversion results(the low end of the chain)

    but his sensor was cheap ZnS fragile and speciallised for alpha not gamma..(an X123)

    https://dspace.mit.edu/bitstream/handle/1721.1/121824/1104134989-MIT.pdf?sequence=1&isAllowed=y


    for R&D gamma to gamma 'conversion' from 10Mevs down to5 kevs.... 500ev or so(the high end)

    a good gamma spec +sophisticated analysis is useful..

  • The reason I am dubious is that, as far as I am aware, no one on site knows how the fuel pellets in the experiments were prepared.

    Even I don't know it...So as a scientist I don't like it too.


    But we now plan much cleverer experiments and it's all about knowledge and modelling where we are the only ones that know how to do it...

  • Even I don't know it...So as a scientist I don't like it too.

    I am very glad to hear that you don't like the present situation either. You have spent years of your life analyzing data and writing a manuscript based on results that, right now, are irreproducible. Your entire project is therefore undercut from the very beginning and that is too bad.



    But we now plan much cleverer experiments and it's all about knowledge and modelling where we are the only ones that know how to do it...

    No it isn't. It isn't "all about knowledge and modelling". It is also about this fuel actually working in a repeatable way. But that is not happening. Almost 4 years on and not even Russ George's collaborators know how to reproduce his results.

  • Gd + Sm look promising. I have informed other researchers about that..

    About one year ago I suggested to researchers who were

    repilcating Mizuno's Ni/Pd reactor that they

    try samarium on their nickel mesh....

    this was just based on the minimal data in Wyttenbach's earlier paper .September,2019

    https://www.researchgate.net/publication/336107679_Nuclear_Particle_Physics_version_20_SO4_physics_Main_achievements


    This is my email

    On Mon, Nov 30, 2020 at 4:01 PM robert bryant ............. wrote:

    Quote
    God Bless your Research Robert Bryant Sydney

    This was the reply..

    Quote
    Hi Fantabulous mail and heartfelt thanks for your mail/suggestions and time. I understood the gist and we are working on it. In fact, our lab is functioning continuously and we got good results during Corona time itself. We never closed our lab as we have a small yet dedicated team to work irrespective of sundays/festivals.... But of course we are struggling with the funding part as all funding has deviated to Covid -19 issues from the Government. I will study a lil and get back to you

    SVP et al worked pretty quickly with minimal rupees and no gammaspec.

    In October 2020, Ramarao reported 71W xs for 300W input with Pd/Ni.

    In June 2021 , Ramarao reported 137W xs for 300W input with Pd/Ni/Sm.

    The recent publication of Wyttenbach's "atomecology' paper

    probably means that REEs cannot be locked up forever with a patent

    by..SPAWAR,IH, and the like..although no doubt they will try.

    The sooner this becomes public knowledge in the wider world... the better

    http://ikkem.com/iccf23/speakervideo/1a-IN03-Ramarao.mp4


  • Once more this is a delta spectrum modified by the Theremino parameters for nearby bucket contributions.

    I would still like to know how the background-subtracted spectra shown in Figure 1 of your ResearchGate manuscript have been modified "for nearby bucket contributions". I think that when you publicly post figures like this you need to explain them well enough so that your readers can understand what has been done.


    What is the modification you mention?

  • What is the modification you mention?

    These are standard spectra with default setting and definitely not shown to identify single lines as it is said in the text...



    May be once you should explain us why you are going on asking your questions despite everything is answered in the text? Either you do research and have the details or you are just reader of science news that gets a part of the information.


    As said. The reason I publish some facts is to avoid others do general patenting.

  • These are standard spectra with default setting and definitely not shown to identify single lines as it is said in the text...

    I have downloaded Theremino_MCA v7.3**. In this version there are many parameter settings where histogram files saved using the "export" menu button precisely reflect what is shown on the screen. For other settings (for instance when the IIR filter is engaged) this 1-to-1 relationship is lost.


    Since in Figures 1 and 2 you choose to show these spectra in a way that somehow do not bear a 1-to-1 relationship with the data you actually carry out calculations on, I think you need to tell people how they differ. This is important. I have noted, for instance, that the spectra at 280C and 350C shown in Figure 1 are far too similar ... at the low bin occupancies you have these spectra should differ randomly 4-5 times more than seen in the Figure. Why? Is it artefact? This is unanswered.


    Why not redo Figures 1 and 2 using data directly from the histogram files? It is trivial. And your figures need to be redone anyway because they are so blurry and hard to read.


    **Note: I originally said v4.0. That was wrong. Sorry for the confusion

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