Tuesday, January 25, 2022

Meditation oN exPeriments

  • Edited 2022-01-30 - Experiment notes incorporated, Addendum reduced
  • Edited 2022-01-29 - Found notes added as Addendum

From Denis Diderot, circa 1760:

There are three principal means of acquiring knowledge available to us: observation of nature, reflection, and experimentation. Observation collects facts; reflection combines them; experimentation verifies the result of that combination. Our observation of nature must be diligent, our reflection profound, and our experiments exact. We rarely see these three means combined; and for this reason, creative geniuses are not common.

From J Bellinger, circa 2015-04-01:

A lot of people are good at going to places they’ve been before but few are good at figuring out how to go some place no one has been.

Part of transition from undergrad to grad student is applying. Part of applying is making oneself an attractive candidate. Part of being an attractive candidate is showing promise of good work and talks and papers in support of a principal investigator. Most (all?) doctoral programs expect to support their students for five to seven years, to get good work and talks and papers out of them. Graduate students are expected to graduate without embarrassing the program. Graduates are then expected to be a credit to the program.

Experiment as an Adventure

It is clear the author is not smart enough to be a physics theorist; witness this blog and the main mnp Manual document. Here, I attempt to establish a reason to be an experimentalist by listing experiments I’d like to do or see done. Since professional experimentalists report report irritation with theorists who come up with a new experiment every week, my output of a countable number of experiments is not THAT impressive. Asking questions is certainly easier than answering them!

The author has been identifying interesting experiments for many years. Not doing them. Those experiments fall, unfortunately, in many branches of physics. They fit conveniently neither into any branch of physics nor any one principal investigator’s interests. Instead of a one page summary, this goes on for 1100 lines of markdown, 8 pages of dense typing, 10 pages of pdf. Enjoy. Or ignore.

Table of Contents

The experiments are listed by area of physics.

Some experiments overlap fields. The experiments can be also be categorized by difficulty and cost:

  • new experiments that might cost a fair amount ($$$),
  • new experiments that can be done from a garage ($),
  • review of existing data looking for other phenomena (t) or (+),
  • very expensive experiments ($$$$$),
  • dangerous experiments (*#x̂!) (!^!̂).

The last, of which the author has a few, will not be discussed in public. You’re welcome.

The ($$$$$) experiments are unlikely to be done at the authors request, so will get short shrift here. They can go on a wish list. The experiments ($) that can be done in a garage should perhaps be done in a garage if interested researchers cannot be found. The review experiments, except perhaps for neutrino review, are probably not a basis for a grad school application. Though those experiments would certainly benefit from guidance and review.

So the most relevant experiments for an application (** or ***) are the not very expensive new ones. In addition, the best experiments do not threaten current interpretations. Oh well, blew that one.

Some experiments and areas have an additional judgment in parentheses; the likelihood of success. (-) is unlikely, (x) impossible.

Experimental Attitudes

While it is attractive to see an anomolous result as, given n explanations, plus a pet explanation, the author will be the first to admit that interesting results in an experiment falling outside expectations would NOT prove any particular pet Models even if the experiment were motivated by those Models. In science, I can bet the farm but there is no double or nothing, only clawing back from losses.

Choosing instead the nth: the most interesting, challenging, new, or revolutionary explanation is not a good idea. Though the author has seen that done frequently. More likely is the simplest explanation possible, which may be error, bias, or random variation. Even in low temperature solid state physics, I see that and benefit from a PI who likes the simplest explanations. Attitude picked up over year(s) or group meetings and reviews of papers. Not that I can cite specific dates and examples.

Undergrad physics experience supplies many examples of homework problems in math proofs and developments; when I expected something to cancel I worked extra hard to make sure it did, with an occasional wave of the hands. Many questions asked for proofs of a specific answer, which allows one to look at the expected answer and figure out how to get there. For designing experiments, this can be a useful exercise in asking “what would prove x result” if used with care and honesty about what proves. For performing experiments, having an expected result is a huge mistake. Done all the time, at all levels, but a bad idea.

Experiments in Particles

Left Hand Preference (***)

The author would like to confirm that the left-handed preference seen in the Beta decay of Cobalt-60 experiments by Constance Wu’s team in the 1957 and confirmed with many other experiments since is truly a universal phenomenon. If not already done carefully, making one or preferably more of those experiments compact and traveling to the North Pole, Equator, and Southern Hemisphere sound like a good time to the author.

Why do this? Null hypothesis answer: To confirm that the Standard Model LaGrangian needs the doubling of term count that results from the left-handed preference shown in the 1950’s experiments. Certainly not to disprove the mnp Model’s conjecture that all movement involves internal change and all angular movement or matter involves subtle internal rotation.

Maybe Not Personal

Even if the result IS interesting, that proves nothing in favor of the mnp Model. A universe of other explanations is available if experiment does happen to show that left-hand preference is a local phenomenon. Should explanation be needed, the author suggests that portion of the conceptual universe that sees moving labs as truly undergoing Lorentz transformation will better explain local left-hand preference.

Such an experiment also calls for extraordinary care, almost forensic in detail, to assure that the results are reliable.

I have a strong interest in an unexpected result. Further reason for care. From (2018/11/09 21:55):

I would do Southern hemisphere carefully A) to develop or prove chops with experiment B) to make sure my personal interest, hidden as I may try to keep it, did not interfere with the results. Someone content to validate the left hand preference would run the risk of missing an interesting result but might take shortcuts with verification of direction. We would probably never know, since the experiment is not worth doing THAT many times if left hand preference IS universal. The motivation to be careful should be there, even for an experimenter expecting to confirm the expected left hand preference, since an interesting result would be, well, interesting.

The scientific method does have a definite advantage - surprising results are remembered and valued, if and only if they hold up. If. Retracting articles is not just embarrassing, it is ugly.

Minor Notes on Process

Test spin measurement separately from other experimental setup, with known spins. Have more than one measuring device. Test in areas with materials for which the answer is known. Test the whole setup to verify known results. This is a standard precaution, skipped at peril to the experiment.

Work on measuring everything possible blindly, either by automated equipment or by not knowing the inputs when recording the outputs, with inputs recorded elsewhere or automatically. Calibration might require knowing inputs and okutputs, but then let the randomizations be driven automatically. Best when the inputs be randomly presented, in this case perhaps by not knowing which way the spins are aligned in the sample. Or by not knowing how the testing apparatus is oriented. From (2018/10/15 21:48) make sure sensor can in fact measure both ways, consider putting it upside down or backwards sometimes

Standardize tests for the equipment; we may not need ISO 9001 certification, but want reproducibility. Strive to test the equipment blindly too: have something else produce spins of a random direction and run it through the detectors. Only look later at the magnetic fields that produced or chose the spin after the test data are gathered.

A principle of software design has been that one can strive for “idiot proof” but one may not be able to protect against Machiavelli. Operating systems and networks are finding that many programs need protection against Machiavelli as well. Check software with external tools to make sure changes have not been made. Check materials or inputs with external tools to make sure changes have not been made.

Pay attention to the chain of custody and the handling of materials, devices, software, and data.

Minor Notes on Preparation

Check literature and friends of friends in the southern hemisphere to see if spin preference experiments have actually been done there. Understand the classic experiments, including confirmations. This list may get very long. Start with initial confirmations (from 2018/10/29 17:05) [http://www.fas.org/rlg/021557 Garwin-Lederman-Weinrich.pdf] and [http://puhep1.princeton.edu/~kirkmcd/examples/EP/ambler_pr_106_1361_57.pdf]

Review and understand the classical dynamics techniques for finding reference frames for rotating labs. Look again at The Ambidextrous Universe by Martin Gardiner for its long lucid discussion of parity and the Wu experiment.

(2015-01-29) Background research: Table the velocities and angular velocities of the galaxy, the solar system relative to the galaxy, the earth’s rotation around the sun, the earth’s spinning, and Coriolis effects at various latitudes. Compare diurnal, seasonal, and arm rotation effects for magnitude. Yesterday.

Particle Deceleration ($$$$$ or (!^!̂))

(2015-02-25 1757) Investigating particle deceleration is offered as one of the highly unlikely-to-be-done experiments. The Model suggests that ultra high speed particles may already be a plasma. Can we slow the .9999c particles back to lab frame and find the same particles? If the original particles/protons/lead nuclei still exist, then the suggestion that a plasma has already been achieved at high speeds before a collision can be ruled unlikely.

It is probably very hard and maybe hazardous to slow at the end of a run; just dumping the particles is probably easier than slowing the protons/Pb nuclei.

Smashing those particles with a transverse bolus of energy or electrons or muons has probably already been tried, thought about, or rejected. The Model predicts that at very high speeds and ninety degree orientation, the interaction would be surprisingly small. Though subtleties of widening of the particles may allow for a somewhat extended interaction time.

Neutrino Review (+)

Review whether mass traversal is a major contributor to neutrino   (energy and type) change. If experiments measuring solar neutrinos are not comparing to solar neutrinos that have passed through the earth, that’s a major (*** or $$$$) opportunity.

Review whether traversing stronger gravitational fields leads to energy change. This one will be harder and more subtle, since multiple cosmological sources will probably be needed. Finding a standard neutrino source or a star or galaxy type that produces predictable neutrino types and amounts is probably harder than finding astronomy’s standard candles.

Neutrino Experiments ($$ to $$$$)

What is a neutrino? The reports of charge, magnetic moment, handedness, even Majorana effects seem all over the map. Majorana seems to boost blood pressure and increase heart rates in other branches of physics, so I’m skeptical pending experimental verification.

Do hotter detectors offer more variation and so yield higher detection? ($$$) or ($$) if existing detectors can be warmed. This from (2015-02-12) Is directional oscillation of the detector possible, particularly in line with neutrino travel? This might make directional sensing (over time) possible. Of course ($$$$|$) Restated: (2020/09/09) Would heavy atoms vibrating in line with the neutrino path yield even higher detection if 2-d vibrating crystals can be reasonably fabricated? ($$$$$)

Would a long imbalanced magnetic field followed by a long vacuum make neutrinos more detectable? ($$$ and up)

Neutrino/Cosmology/Astronomy Review (+ or $$$$$)

The author has seen physics writers claim neutrinos travel exactly at c, that neutrinos and light from supernovae arrive at the same time. The author has seen physics writers claim neutrinos travel close to c. The author has seen physics writers claim neutrinos, since they have mass, must travel close to c. The author is interested in seeing what experiment shows and understanding without assuming neutrinos behave like all other particles we’ve seen. If neutrinos have mass and travel at c, well, nature is real different.

Do neutrinos traverse black holes? This may be a question for neutrino astronomy, not a field for easy experiments. If astronomy has identified light (and presumably neutrino) producers traversing behind black holes, can a difference in neutrino arrival at Earth be seen? Can neutrino output from pulsars be measured? The author would expect finding supernovae traversing behind black holes while producing neutrinos to be exceedingly rare.

Collision Review (+)

The mnp Model posits strict conservation on charge material, so I suggest some decays and some cross sections will produce different results depending on the intensity of the experiment. Experiments producing more stuff will have higher success rates on those reactions requiring the recruitment of charge material. An example would be muon decay to two electrons and a positron. Not all reactions recruit charge material. For those interactions, the author would expect to see much better agreement between experiments run at different intensities.

If experiments keep track of data during the startup of runs, the author would expect to see interactions that do not need material occurring at the expected rate, but those requiring additional material to show lower cross sections than when the run is operating at full intensity. From (2020/11/08 09:38)

I cannot imagine getting support for this unless the Particle Data Group is concerned about variations between some experimental results but not all. If there IS concern, I would like to be blind to which reactions are problematic.

I propose to categorize reactions in terms of recruitment needed and results freed before looking at the variation in experimental results. Only then is checking different experiments appropriate.

  • Hypothesis: experiments where recruitment is needed have higher cross sections when they are run at higher intensities.
  • Null hypothesis: experiments show the same cross sections for all reactions no matter what intensity they are run at.

Further conjecture: (2022/01/21 14:29) There is an upper bound on effective density of recruitable material particles. Increasing cross section/yield may be asymptotic in intensity or may saturate, so experiments exceeding some intensity may see no increase in cross section. There may be curves we could fit, even from different experiments, based on calculating availability in those experiments.

Hunt for New Particles (+)

This hunt might amount to a PDG Review or might include a deeper dive into promising experiments. The hunt for versions of strange is not expected to receive support. The mnp Model sees down and strange as related, since 1/3 charge quarks are seen as offering 3 possible arrangements of charge while 2/3 charge quarks offer only one. Look for other versions of strange (higher energy but shorter lifetime), then look for other versions of bottom, or bottom + bigger version mesons.

The hunt for neutral particles/quarks larger than up and down but smaller than Z is also unlikely to gain support. The mnp Model sees three possible flavours of smallish neutral particles. A second family is not considered likely below Z (which might be a family as well), and a third family is expected to be larger than tau and top, so unattainable.

Examining the Higgs (from 2019/07.18 22:07) to see if its spin and products are consistent with a meson of bottom-like and anti-bottom-like quarks is not likely to be endearing to particle physicists. Best left unsaid.

Null hypothesis: there is nothing to be found

Particles - Room Temperature Annihilation or Interaction ($$ or (!?!))

Advances in quantum computing and particle storage and optical tweezers may allow single particle interaction experiments. Storing positrons is not any harder than storing electrons and not really much more dangerous. I hope. I suggest considering single electron/positron combination first. Might involve destroying the intersection part of the apparatus, but if enough knowledge can be gained or the apparatus is cheap enough, that may be OK.

Look at the resulting detritus direction. If enough experiments can be done and a preference is seen, controlling for time of day and time of year, that would be interesting. The Model posits that the (apparently) unorganized charge material from the reaction is a form of dark matter, so there may be some (but not a lot of) drag of results toward a rest frame. The Model can see partial coils interacting and being dragged some, so the effect of ceasing to move in the Earth’s rotating frame is not immediate.

Questions destined to irritate experimentalists: Do we keep track of time of day and day of year in high energy experiments? Latitude, Longitude, and orientation? Would an oblate testing chamber with tests at different times of the year make a difference?

Fantasy: Isolate a kaon away from other events to see if decay results are different. From (2020/11/06 19:37)

Casimir Effect Experiments; Courting a Vacuum Catastrophe (+ to $$)

The Casimir Effect has received much work. Calculations and predictions are well developed. Repulsion, usually from fluids, has been found interesting. A chip has been developed to make experiments easier to do while reducing the needs for physically exact positioning. This from a quick reading of the Wikipedia Casimir Effect article, https://en.wikipedia.org/wiki/Casimir_effect.

As an independent focus of study, the Casimir Effect may offer only a low probability of success of finding new materials or levitation techniques or new physics or averting a vacuum catastrophe. As an adjunct, for example by adapting Casimir effect measurements to STM appartus either as an independent study or a way to study surfaces currently studied in (some) different ways, looking at effects of different temperatures or using STM techniques of different bias currents or magnetic fields or varying fields, interesting results may.be available.

If the optics investigation of diffraction in materials, temperatures, and fields yields interesting results, the Casimir effect might become more interesting and easier to add on to those experiments.

  • Model Hypothesis: (2017/11/02 22:22) The Casimir Effect is not vacuum energy but a surface effect of electron coils attracting and in some cases repelling.

  • Hypothesis: Different temperatures and bias fields yield interesting results, not in keeping with calculations.

  • Null hypothesis: No explanation will be found or is needed for the experimental results. No difference from (others) predictions and measurements. No new or exotic materials will be found. The Casimir Effect shows the vaccuum potential is very large.

AstroPhysics

Looking out at regions we cannot visit has been fruitful not just for what we can see for what we can learn from what we see. Cosmology and particle physics have benefited.

Shapiro Effect (+ to $$$$$) (?-)

The Shapiro Effect shows electromagnetism passing close to a massive body slowing. The Model hypothesis is that this slowing is the radiation is taking a longer path, further out from the body, rather than going deeper into a light well. This can be examined if the data on satellite antenna aiming has been collected. (+) If the data has not been gathered I suspect it will not be added to satellite programs just at my request ($$$$).

From (2014-04-04) a Shapiro light ranging test would involve keeping track of location and antennae direction if the antennae are automatically seeking signal optimization. Presumably the transmitters and receivers on satellites are sensitive to direction and auto correct to optimize transmission. (Better than amateur Yagi, anyway.) If the data exists, this experiment becomes a review (+) Easier is to keep track of antennae orientation on Earthbound stations if the antennae are capable of fine tuning. ($$) If VERY fine tuning is needed, highly directional antennae might increase the sensitivity. ($$$)

From (2018/10/15 21:29) the fantasy develops further. If a satellite can aim a collimated beam where it wants and advance or retard the angle, we could do the measurements from Earth with atmosphere and weather as confounding factors. Unless can choose a wavelength not much affected by the atmosphere. Measurement on the ground at various places might be an effort, but perhaps less expense than sending sensors up in a satellite too. If the satellite is on the ecliptic, needs only to aim along the ecliptic. And mis-aim to see what and when the best signal is received. If signal is time varying then timings can be calculated or deduced. The Null Hypothesis is that GR calculations are correct. The mnp Model hypothesis is that there is not as much slowing as expected, but the path is different, first tending in until the beam is tangent to a sphere around the sun and then diverges outward more toward parallel to going away from the sun. The author needs to determine actual factors of gravity for calculations. Experimenters with unlimited funds could also recalculate a lot of transits and compare to measurements and GR predictions. A collimated beam is even better if it cycles through an off or on off pattern. If a fixed period of output is easier, just vary the gaps between transmissions. Ojala.

This might be turned into a relevant topic of review if satellites have been lost when turning them off when the satellite is a long way away but at 90 degrees from earth with apex at sun? If only a few satellites have been lost, investigating the distribution of positions may not be a large statistically powerful sample.

Relativity (+ or $$$)

Since GPS satellites are moving faster than the surface of the Earth, Special Relativity would suggest they would see Earth clocks moving slower. From (2014-07-15), is there a “simple” experiment of asking the GPS satellites what they see of Earth clocks. Corrections are needed to Earth receivers and have been successfully implemented. Have the GPS satellites been asked the same question? If this has been done, only review is needed (+). If easy to implement, ($$). Since the muon storage experiment shows clocks undergoing angular acceleration do not show any slowing other than due to their speed, clocks in an elevator are NOT slowed by acceleration while those in gravitational fields are, this satellite question is a relevant test.

The author continues to look for experiments of fast reference frame looking back at a slower one. (+) (-)

Galactic Dynamics (+)

(+) (-!) From (2014-10-20 1745) do galaxy arms evolve in predictable manners? Does astronomy show a range of galaxy patterns that suggest evolution or change?

(+) (-) Is there a way to see if loose particles or dark matter slows beyond the MOND limit, perhaps if cosmoligical evidence suggests less mass loss from galaxies than might otherwise be expected?

Dubious Propositions (+ or $$$$$)

Photon Count (+) (x): I need to review results from astronomy to make sure photons are never split, that measurements from different references show different energies only

Brehmstrahlung (+ or $$$$$) (-): Does brehmstrahlung slow particles? Is there a way to see if it even happens in deep space? Only if a Pioneer sees it or can be asked to look.

Solid State Experiments (+ to $$)

From (2021 and 2022): In STM, are we imaging nuclei or electrons? Nuclei. Regarding moving samples with the tip, was pushing things around with an STM tip better when aiming between high points? Would a poorer/broader/multi-point tip work better for pulling or pushing? Regarding tip adjustments, would having an area of lower or higher albedo make picking up or dropping off of a tip, for example, CO easier?

STM approaches and environments would be useful for free electron investigations (below). Casimir Effect investigations (below) and optical investigations (below) would also benefit from scanning tunneling microscopy.

From (2019/07/18 22:13) The vacuum and cold available in condensed matter labs may offer a low expense site for experiment. Or not. NB (2022-01-29) One needs to make sure nothing that will out-gas is introduced. Need to determine the dimensions of what can be introduced with the fiddle arm and how much freedom of location is available. Introducing new wires is hard, it seems. Dropping stuff to the bottom of the chamber is bad form. Having a tool or grasper or two might be interesting. Storage space for five or six 1.5cm square samples does not offer many options. Clearly, the author is not well enough immersed in the lab to have the background to be asking good questions in this Covid era. LoL

Electromagnetism Experiments (+ $ $$)

Many of the experiments listed here may be unnecessary if already done or the results can be predicted clearly enough. The null hypothesis is that all is known about photon/material/material wave function/edge effects. The mnp Model hypothesis is that matter and its wave function is necessary for all interesting redirection of photons. Yet in apparent contradiction, the mnp Model hypothesis suggests electrons can interact with photons.

Photon - Free Electron Interactions (+ to $$$)

In potential overlap with Solid State (cryogenic) or Room Temperature Particle categories, is it possible for a photon/laser beam to be absorbed by a free electron? The undergrad answer is no of course not. The author suggests this is a relativity confirmation test, since free electron absorption would indicate mass actually goes up with momentum increase. This question has been festering for years. The author suspects that in STM no electron would be seen as truly free even when tunneling from tip to sample.

Electrons on negatively charged conductors, on graphene, on semi conductor donor materials, glass, rubber (?) might be almost free, so might be candidates for trying. An electron shower in a laser beam might see the occasional errant electron. Sweeping the light through the shower or the shower across the light?

Measuring where the electron goes, noting what momentum and energy it has, is expected to be difficult. Perhaps almost as difficult as finding a free electron to zap it. The electron confinement techniques currently available may make that almost possible. Measuring momentum transfer to the confining field or worse, showing there is no transfer, might be difficult.

  • Null Hypothesis: Free electrons cannot absorb photons
  • Hypothesis: Free electrons can absorb photons
  • Null Result: We cannot even hit an electron with a photon to find out. No effects whatsoever are seen.

Diffraction and Diffusion - Materials and Methods (+ to $$)

The author would like to understand the parameters (and non-parameters) of diffusion and diffraction. As with all experiments, understanding the physics and literature review come first. Then finding an inexpensive big enough CCD. Old cameras with a 25mm CCD might be candidates, though a much bigger one allows larger experiments or larger fingers.

  • Null hypothesis: All is right with the world. Optics and (maybe) quantum mechanics understands optical phenomena perfectly. Enjoy the learning opportunity.
  • Hypothesis: By changing slit conditions and experimental procedures, interesting results will arise.
  • Model hypothesis: Matter under the influence of electromagentic fields away from radiation itself is necessary to produce the optical phenomena seen.

Review will involve (from 2016/07/11 18:44) categorizing experiments by distribution pattern, coherence, selection mechanism, author cooperation or belief that info is useless, and other criteria to be determined. A database, bibliography, almost an encyclopedia of experiments should result if I do this investigation.

Quantum mechanics and perhaps quantum field theory will be important for this investigation.

What Level of Coherence is Required

From (2016/07/11 18:45) understand coherence.

Delayed choice experiments: From (2013-11-07) review the John Wheeler experiment of shining light across the destination screen. Could we clear the “guide waves” by sending stuff across in between photons. Experimenters pick interval between photons or electrons, when within that interval the clearing can be done, perhaps at a randomized time.

  • Hypothesis: Superposition will not maintain the “guide waves” enough, so sweeping should clear diffraction patterns
  • Null Hypothesis: Sweeping will have no effect

Varied “clearing” spacing: From (2016/06/21 21:37), clearing photons or other field disturbers could be random or spaced - could have different spacing than fhotons going through, so could statistically measure how much effect a recent clearing has.

Varied photon energy: From (2016/06/21 21:39) could we have different wavelength photons go through a coherent field from a cascade of different photons?

Varied photon spacing: From (2016/06/21 21:35) can we get photons out of phase with the previous trapped/measured photons in an experiment? Rephrased (2016/07/11 18:45) can I introduce stutters?

Varied photon aiming: From (2016/07/11 18:36) if electron or photons are aimed at one slit, what is the yield pattern on the other side? How much deviation can be tolerated on the inbound side? Does de-focusing have an effect? What is the effect of the defocus covering both slits? Is there a lag between starting the experiment and collecting results?

Understanding Single Photon Experiments

Do all that see diffusion and diffraction have coherent fields already set up, or are some sending photons or bucky balls with no prior history?

  • Null hypothesis: No prior history is relevant in single photon experiments. Of course.
  • Hypothesis: Well, maybe some history matters.

2014-07-19 single photon experiments seem to occur in the presence of coherent fields from subtracted photons. Somebody (Clark) with clearing between photons finds no interference??

Materials in Diffraction and Diffusion Experiments

If experiment conditions can change the wave function of the electrons in the material making up the slits, so we get higher or lower diffraction? Does cold affect the effective width of the slits? Do electric or magnetic fields imposed on the grating (as a bias as in STM investigations) lead to interesting results?

Do different materials and conductors change the behavior of slits? Can materials be found that hide (or enhance) their presence in diffusion/diffraction experiments?

Changing conditions can include different materials or different material temperatures on each side of a slit, very hot or very cold materials forming the slit. Comparing materials with very active and available electrons on the surface against materials with very little electron availability on the surface. Do superconductors near or just above their temperature of activity act differently?

Momentum Transfer in Diffusion and Diffraction

Does very thin material retain its function as a diffuser? Can thin opaque materials be used to measure momentum transfer, perhaps by noticing increased variation in results if the diffuser is vibrating or moving?

Diffusion and Diffraction Without Presence of Matter (+ for now) (b46-no-matter)

Can a curtain of free-ish electrons in or near a slit lead to differences? Reflection? Random redirection of the photons? Redirection of the electrons? Increased velocity of the electrons? This touches on the free electron-photon interaction pursuit above.

Does diffraction, diffusion, creation or radiation require matter or can it be accomplished by pure electric, magnetic, or electromagnetic means? This may require looking at high energy particle collisions and perhaps high energy cosmological events. For now, this is an experiment review topic with low probabilities of success.

Antennae (+ to $$$)

Do antennae at different temperatures, materials, bias charges or magnetic bias fields, behave as described by the quantum mechanics of the surfaces or do they behave differently. Is material (metal) skin depth relevant to antenna behavior?

  • Null hypothesis: Between quantum mechanics and electromagnetics, nothing remains to be learned.
  • Hyper-null hypothesis: Investigating these issues will provide no interesting techniques for small scale radiation or STM experiments or small scale technology.

Evanescent Fields Left by Photon Passage (+ to $$$ or x)

Can we measure the evanescent fields created by a single photon?

  • Null Hypothesis: photons leave no trace. There is no such thing as evanescent fields.
  • Model Hypothesis: photons create evanescent electromagnetic fields that do not have a net effect on the random field potential that exists in the vicinity of matter and are not conventionally measurable and not conventionally seen as energy.

Can I invent a way to see those electromagnetic fields? Is subsequent passage of photons affected in subtle ways? Certainly, I do not expect support for this endeavor.

Vacuum Recruitment (+ to $$$)

From (2016/08/10 13:47) Can a varying magnetic or electromagnetic field without matter lead to diffraction and/or diffusion?

From (2016/09/26 13:14) Is the presence of matter necessary for photon generation?

  • Null hypothesis: Quantum field theory rules.

Relativistic Optical Experiments {+ and $$$$$$$)

No experiments are likely to be available between armchair musings and impossible measurements. Thought experiments, such as diffraction experiment in a high speed frame or a relativistic double slit experiment at varying angles, can only be tested by finding some cosmological phenomena. Unlikely!

Preparation Required for Optical Experiments

The author would need enough preparation in quantum mechanics and quantum field theory to start predicting results. The author would need to collect background literature and a bibliography. The author would need to continue getting exposure to materials. Show, not just say.

Optical Experiments Conclusion

These questions are not all separate. For example, they may combine in understanding the behavior of half silvered mirrors. from (2014-03-21) could the changing EM fields that go through the half silvered mirror conjure a photon at a different phase or sign and only dissipate or cancel another further down the line in the multi-stage experiments?

Null hypothesis: again, let me restate, we know everything we need about diffusion, diffraction, and spin. More is not to be discovered. The investigation should have lead to a lot of learning. Enjoy.

Experimental Design (+)

Studying experimental design is expected of an experimentalist. Some of the author’s proposed investigations require more than the usual level of care, making an almost forensic approach and understanding of experimental design appropriate.

Figuring out ways to measure while blind to the results. Automatic collection is of course the gold standard. Varying the inputs without the researcher’s knowledge, only to reveal the inputs during analysis.

For example, with the room temperature decay or single collision experiments, the measuring apparatus, if an opaque hemisphere and small enough, can be rotated by a random amount by the controller, then the results viewed to make sure the device is operating properly. Only when the random rotation is taken out can we look at the directional results over a large collection of measurements.

The posts and appendices in the mnp Manual proposing a Registry for Design and Data and a Journal of Negative Results have not yielded change in the field of physics, but show my ongoing interests in experimental and communication methods. This post/chapter can be seen as a personal Registry of Design.

Academic work can be divided into three or four areas: note taking, results gathering and analysis, and publishing. Investigation of the transfer of notes to publishing has been interesting but not earthshaking. The author’s program Scribe for formatting reports (from the teletype/hard copy days) has certainly not gone anywhere. The experiment (2022-01-24) transition to composing with Markdown which will be translated to Latex and HTML is ongoing. This post/chapter will be the first. Investigations of Electronic Lab Notebooks continues. None of this is a subject for graduate school. The tools are interesting and hopefully help foster the creation of new science.

Presentation: I was asked how to display results on a screen. On (2015-03-02) I wrote down an answer: color, pattern, change over time (careful to not be annoying), size length/area/volume, greater shading for depth?? shape (round line triangle square offers GH code for number [of -sides-] where round is 1 and a line segment is 2, a triangle 3, if we don’t go to infinity on polygons. Management by exception allows sound: tone,timbre,chord, and/or vowel. When is sound used? On an event, failure, when mouse over (games used to do that a lot!). Sound bite: there was a time when the University of Michigan computing center, if the last job completed successfully and there was not another waiting, would play Hail to the Victors. Time to check the next card deck.

Display of 3-d tensors on a 2-d screen will be revisited. I promise. Similar is the display of probability density functions in 2-d over time or over changing conditions such as temperature. For some changes, presenting a movie perhaps at different paces, with a slider bar whose color represents temperature. Of if the image of probabilities is a scalar, changing the color of the entire image with temperature may be telling. Color can be used to gain attention, sometimes to the detriment of the science. Shout out to PJ for that!

Choosing instrumentation, beyond small computers, analog digital converters, and thermocouples, is not something I have a lot of experience with yet. I do remember, back in the early 80’s, being asked how to computer square roots quickly on a high speed logic board. They were using MUCH faster calculators than I was with my Z-80 4MHz processor with software floating point, but needed even faster results. I heard myself ask “What are you doing with the square root. Comparing it?” The yes answer prompted “Then square what you are comparing to.” I never heard back from that large project, but the take home message is

Think about what you need to measure and what you need to calculate. Algorithms can offer faster or better results than more hard work.

Observation will be better, for example, if Machiavelli er the observer does not know when, for example, fields were supplied to the slit but is just measuring the level of diffusion, the results will be better. In quantum level experiments, we may need sample photons at times to check runs, even if that means reducing the number of successful runs. Observing and recording the results even for those “sampled” or “ruined” runs is a useful test of the observation if the observer does not know about the inputs. At an extreme, if thwarting Machiavelli is important, a known photon may need to be sent along in place of the unknown sampled out. Sending a false sample to a testing lab can be a useful technique; if the DNA lab always returns the desired match, they may not be following good testing procedures though business will be good for a while.

The difficulties measuring the speed of neutrinos back in 2011 inspired many thoughts on observation blinding. If a delay of 0 to 9 (nanoseconds?) is called for, start at the 56th digit of pi and use those numbers. Or send those numbers to a device AND have a collegue send (and record) numbers to be added to the first stream of numbers, so that neither sees the value submitted to the device.

Analysis itself can be somewhat blinded if taken in steps, without knowing where the input data came from or which experiment it refers to or which direction or orientation the suite of measurements was taken in. The computer science concept of unit testing or proof is useful. Again, algorithms and procedures can offer better or more reliable results.

Statistics are useful (from 2019/09/01 09:59) but biostatistician GM points out if a study does not have intra-ocular impact, it is not that significant. To translate to the vernacular, if it doesn’t hit you between the eyes it isn’t meaningful. Still, in some experiments, understanding the calculation and meaning of power will be useful, as will an understanding of Bayes inference and the role of false negative and positive. So the author is called to learn more statistics to augment that gathered from (mostly) experience with biostatistics.

Beyond Physics

The sketch of “How to Create a Terrestrial Flying Disk” requires materials science, computer science, and aerodynamics, but not much new physics so is “Interesting. But weird.” Other than creating such a device for the sake of creation and bragging rights and perhaps using it as a reliable high altitude helicopter, there do not seem to be pressing reasons to press on.

End Words

(2018-11-14) Taking the Graduate Record Exam (GRE) to start a five year clock for preparing, taking the Physics GRE, and applying to graduate school has had a number of consequences. One of the questions raised by the "who do you want us to report these results to" is "what program are you applying to?"

Preparation Story

Humor: I imagine a munchkin asking "what kind of physics are you?" "You mean what kind of physicist?" "No, what kind of physics?" "Well, if you give me the ten choices, I’ll have to say "physics." "Oh, so you are physics physics." "Since I can’t say all of the above or most of the above, yes" "Can’t you make up your mind?"

And to that question, the answer will be/is useful to me, but perhaps not to a graduate program. What kind of physics am I? Maybe theoretical physics some day, perhaps even mathematical. Hah. After over two years of undergraduate physics courses, that looks far less likely. For graduate school, putting together an experiment seems a better path. But what would be best or available?

In the Beginning

Six experiments dominated my early preparation for grad school. Stated in null hypothesis mode:

  • Particle physics: Verify that the Wu experiment or similar spin experiments show left handed preference in the Southern Hemisphere and at the equator.

  • Particle physics: Verify that collision and decay experiments do not have small quarks bigger than strange and shorter lived.

  • Particle physics: Verify that there is no evidence from collision and decay experiments for neutral particles/quarks larger than up and down but smaller than Z and that there are not two more larger shorter lived flavours and there are not multiple families. (THAT was a hard hypothesis to put in null form!)

  • Optics: Show that the material of a diffusion screen and the quantum behavior of the material around the slit(s) have no effect. Verify temperature independence and if possible frame independence.

  • Condensed Matter: Verify the Casimir Effect results and fill in gaps.

  • Relativity: Verify that aiming parameters for satellite radar from the far side of the sun and from away from the sun are exactly as General Relativity would predict.

Not so many months later (2018/11/07 08:50) the priority list was five, again in null hypothesis mode: left hand preference is universal, general relativity predicts the path of aimed beams from satellites, there are no small neutral particles, there is not a third form of up slightly more massive than strange and shorter lived neutrinos cannot be captured with the help of asymmetrical magnetic fields.

Why This and Why Now?

I was advised that with my background I could not get into grad school, so I might as well post about interesting experiments. Seeing them done by others would certainly not diminish my vanishingly small chances of getting into graduate school. A few of years of classes and expanding understanding of physics have added to the experiment list. And to understand how some might be easy, but some exceedingly difficult. Long enough for my respect for experimentalists to go up.

I am more interested in being clear about my interests and the mnp Model than I am in persuading. The wags suggest that is a good idea, since I will NOT be persuasive.

Conclusion

How this school endeavor is going to finish is not clear.

One of the benefits of putting the compilation of experiments together is the opportunity to gather all the thoughts from the various electronic files (not really deserving the title electronic lab notebook, this) and to think about them, categorize them, and see what patterns they form. Major pruning to make the list useful remains.

Thanks to the Giants.

Return Addresses:

Addendum - Extra Experiment Thoughts Found (2022 01 28)

While writing post 46, Meditations oN exPeriment, I had the feeling I was missing something. I covered all the experimental topics desired, but often wrote extemporaneously about issues I had thought about previously. Yesterday, I found 5 pages, 114 entries individual, 70 entries when multiple contemporaneous thoughts on the same topic joined each other. These thoughts were in the original materials but not the extracted notes on experiment I had used to write post 46. The result is three dense pages of markdown display, approximately five pages of pdf.

A background note on methods: I collect thoughts while reading or writing at the computer using a command line script that adds date and time to the thoughts. Every few years or when resuming blogging, I save the original, sort the thoughts by topic, save that with a date range and use topics as needed. I have now created, for this correction, a script (called thoughtprocess abbreviated tp if you must know) for processing the thought file(s). After processing, using a spreadsheet to sort by topic or subtopic is much easier and producing markdown tables simpler. More important, the process should be more reliable. Doing that in public may not be such a good idea; if I choose what to write about and what ideas are worth writing about, a lot of pruning makes for less publishing work.

Not every idea is a good one. With this update to post 46, Meditations oN exPeriment, much of the temporary Addendum has been incorporated. Much has been relegated to comments that pandoc will not include in the html or tex translations. Some has been relegated to the trash. You ARE welcome.

Sunday, January 23, 2022

Registering Experimental Designs and Data Encouraged

Abstract

Saving designs before experiment and data before analysis and publishing and then (lightweight) publishing of negative or inconclusive results, are encouraged. A proposal for a lightweight registry of experimental designs and data may be more effort than it is worth, given current tools for timestamping and electronic lab notebooks.

Tenth Anniversary

On the approach of the tenth anniversary of the idea to register experimental designs without disclosing those designs publicly, the author is pulling that registry idea out into the light of a blog with single digit readership by updating the one page proposal, Appendix G from 2012, to account for the “new” internet. The registry is seen as an extremely lightweight method of recording the existence of files. Those files remain with the user and can later be shared privately or publicly at the user's discretion.

The proposal will be placed directly in the Appendix mnp Model's Journal of Negative Results in the main mnp Manual: An Architecture for the Fine-Grained Structure of Everything since the existence of free timestamp servers and well reviewed free electronic lab notebooks makes this proposal less attractive. One minor advantage of the proposal is that a creator can send a number or a line of data rather than a cryptic file to a receiver, though in all cases the original file will eventually need to be sent if verification is important.

For reference, here is the revised proposal for a registry of methods and data.

Lightweight Registry Proposal - Deprecated

Initially intended to be a registry of experimental designs in physics with no requirement to publish the designs themselves, the concept could be applied more widely. Proving that one did a body of work by a certain date is useful for academia in general, to prove prior experimental design but also to prove that a body of data was gathered by a time and maybe to prove drafts were done by a certain time. Registering lab notebooks occasionally at least puts a “seal” on the work, though dates and times between submissions are not “proven” by the contents of the notebook.

Outside academia, copyright in general is an effort to establish authorship and time. Establishing time of ideas for patents and prior art is relevant to some, including academia. The author's imagination is neither unlimited nor fast, so further ideas are welcome.

So proposed here is a fast lightweight method of proving a timeline for data that might be kept private or made public.

Prior Art

The need to prove that something existed at a certain time was handled in the past by mailing it to oneself in a stamped envelope so that the post office would postmark the package (thanks, E). One had one chance to open the package to prove the contents, after that the contents were out of the bag. The advent of photocopiers meant one could also use the materials before opening.

Notaries could be paid to put stamps on documents and record when that stamp was applied. This was a fairly heavy investment and depended on users keeping the documents unchanged. Without sealing the documents inside a container (see the previous paragraph), this might not be considered reliable.

Current Art

An industry buzzword is RFS 3161 compliant timestamping. The commercial services take information (as suggested here) and create a hash of the information and the servers credentials and send that file back as a timestamp token, which is stored by the creator of the information. No need to store the timestamp remotely. Other services store the original document remotely and create the timestamp remotely. Some free timestamp services exist, though finding them and verifying them can take time. And using them can require programming.

Not itself a lightweight solution.

Certainly the author is not introducing a completely new concept.

Putting anything on the internet is considered by many to be permanent. Photo owners who let their account lapse sometimes discover otherwise. Depending on reference frame, portions of the internet may become beyond the event horizon. Time of publication is an issue. Establishing that something was published at a certain time seems problematic. The author wishes material put on the internet DID have a date visible, that search results had a creation or substantive edit date. He has had the experience of reading material and documentation only to discover that it was written years ago about prior versions. Or written for completely different audiences, as when tax information addresses “you” but applies only to business owners.

If a blog post is considered proof that it was created on a certain date, blogging can be used. If the dates are not maintained or can be adjusted, this is not so reliable.

Creating a project on github maintains the commit date (thanks E and 2018 notebook entry) for all to see. The project name and author is publicly known, as is the contents. Github might not be amenable to keeping millions of projects whose single file consists of length, CRC32, and SHA-512 for free. Naming conventions might be established. Or not. All project names are unique to that author, so conflicts are not an issue.

NFT's, if the author could ever understand them, probably do not contain a date resistant to spoofing or counterfeiting.

Even heavier or more expensive solutions include:

ISO 9001 general quality control requirements can include keeping track of documents and dates. Costs.

The US Food and Drug Administration (FDA) has requirements for tracking work. Probably very heavyweight, given the profits and human safety issues involved.

Timestamp Servers

Direct timestamp services exist on the internet. Timestamp servers take a cryptographic hash of an existing file and return an encrypted file containing basically proof that that hash was submitted at a certain time to a trusted server. Many cost. Some are free. Most require programming.

Free Timestamp Servers

A list of free timestamp programs can be found in https://gist.github.com/Manouchehri/fd754e402d98430243455713efada710 . The list was last updated six months prior to January 2022 review. The discussion can reveal changed experiences and new servers found by others. Some servers are limited to 100 per month or 5 per day or 10 per day or 20 in 20 minutes or non-commercial use only. Finding and using a timestamp server requires either knowledge or a program, some of which make creating timestamps invisible.

Electronic Lab Notebooks

Electronic Lab Notebooks exist. Most cost. The idea has existed since the 1950's. Implementations started to be feasible twenty or thirty years ago. Most Electronic Lab Notebooks have improved (or been impemented) in the last ten years. Searching those three words turns up many reviews and sources. Reviews may include 40 products in the list. Many are industry specific. Many are large. Even searches adding the word free turn up reviews of mostly fee based services. For example, SciNote is accepted by the FDA, NIH, and European Commission, includes inventory tracking, standard operating procedures management, and project management. Most do much more than just provide timestamps for information.

Free Electronic Lab Notebooks

For electronic lab notebooks, two references might be useful. A review article relevant to academic research from Nature Protocols (2022-01-14): Higgins, S.G., Nogiwa-Valdez, A.A. & Stevens, M.M. Considerations for implementing electronic laboratory notebooks in an academic research environment. Nature Protocol (2022). https://doi.org/10.1038/s41596-021-00645-8 runs ten pages in two columns. The short story: implementing ELN's is hard and requires knowing the lab's needs. ELN's offer advantages of searching, archiving, and sharing but have a learning curve.

A free, open source electronic lab notebook is eLabFTW https://www.elabftw.net It can be run locally or hosted by organizations centrally or remotely on the web. Installation normally uses Docker, so is moderately complicated or moderately easy depending on ones experience. To run locally, half a day for setup by a moderately savvy user is one estimate. The existence of such notebooks and timestamp services allows the author to put this Lightweight Registry for Experimental Design and Data on hold.

Deciding to use an electronic notebook after researching options and requirements takes some time. Using electronic lab notebooks might be useful for many.

Advantages of a Registry of Methods and Data

Without creating any stigma, having a registry for methods and data might make submitting to a Journal of Negative Results easier. If the methods are already packaged and the data can be packaged for delivery to responsible reviewers, then only a summary of results may be needed for submittal to a JNR.

Introduction to the concept of Journal of Negative Result

Regarding a public Journal of Negative Results, which attempts to create a repository for failed experiments and ideas, there have been many efforts. Motivations for a Journal of Negative Results include the oft cited 2005 paper by Ionnadis in PLOS Medicine which has a medical focus and suggests most published findings are false. At least that synopsis gains attention. It also suggests that negative studies in some fields, if published, might appropriately lead to abandonment of the field. Again, note the medical focus. Citation: Ioannidis JPA (2005) Why Most Published Research Findings Are False. PLoS Med 2(8): e124. https://doi.org/10.1371/journal.pmed.0020124 August 30, 2005.

Mentioned in https://www.aje.com/en/arc/negative-results-dark-matter-research/ are

The dark matter article notes that negative findings, in the rare event of being published, are less likely to be cited http://www.plosone.org/article/info:doi/10.1371/journal.pone.0054583 . The author suggests a lack of citation may not be a measure of utility; researchers benefiting from negative results by avoiding an area or even a field may not cite, but still benefit by redirecting their energies. Measuring those intangible benefits is not easy. The article raises the question “Would you take the time to write up negative results if there were a simple template and some credit for your efforts?”

Motivations for a Journal of Negative Results include The often cited 2005 paper by Ionnadis in PLOS Medicine which suggests most published findings are false. At least that synopsis gains attention. Citation: Ioannidis JPA (2005) Why Most Published Research Findings Are False. PLoS Med 2(8): e124. https://doi.org/10.1371/journal.pmed.0020124

Registry Proposal Details - Deprecated

Now that the reasons to create a registry are seen as transitory, the proposal itself is included here but not fully rounded out.

Data to Store

Perhaps timezone, but don't worry about spoofing. Perhaps URL, but do not worry about spoofing or VPN's.

Data Required

Hope to work without cookies. Hope to work without having the website re-written or spoofed.

Design Parameter

For a designer whose experience includes

  • working on the Camp Fire response, which burned an area bigger than the Bay Area,
  • using 16K DRAM chips from manufacturers claiming the rare errors were from cosmic rays
  • upgrading to hard drives with 10 Megabytes of storage
  • graduating from (shared) dial up to ADSL
  • moving from ADSL to fiber only recently

the author retains an acute awareness of storage space, storage reliability, bandwidth, minimal resource demands, privacy, user effort, and user learning/knowledge requirements.

One concern, of course, is the user reaction “do I really have to learn something new?” Another, similar to modern reaction to email, “That looks really old.” “Like last year.” “Why do you use green rather than blue? It's ugly.”

Storing the data is the easiest part of this proposal. Keeping it secure is more work. Retrieving it is yet more work. Making the user interface pleasant is work. Making it secure and resistant to denials of service and tampering is a lot of work.

Limitations on Use

To limit the denial of service by a/some users creating a lot of entries: Set a limit on number of submissions per day? Use captcha or something similar to assure human use. Though the author finds that irritating.

If we really do not want commercial or vanity use, restrict users outside .edu addresses.

Responsibilities of the User

Primary is keep an exact copy of the file from which the record / time stamp / identity stamp was created. This applied to copyright applications since the advent of copyright, so will not be unfamiliar. Still, the author has at times struggled to keep archival copies locally or not so locally and keep them findable. Storing encrypted files on the net is fine. The user still must retain the key and assure the encrypted file remains accessible.

Personal Notes on Keeping Notebook

Keeping directories constant has been virtually impossible; single files are more manageable. The author has found it hard not to go back to electronic records of thoughts and do spell check without changing the substance. If I were really concerned, I'd know where the original was kept and what its name was. As an old time user of computers, I DO have a lot of backup copies. Just finding the version I want is tough and of course the contents COULD be spooked or changed.

Responsibilities of the Keeper

Keep the information as append only, do not go back to change previous entries, just allow additions. Backup the data in multiple manners, save the encryption key for those backups, have a succession plan, try to avoid Hollywood scenes of kidnapping or rubber hose steganography, Succession plans: does the community take over decisions, do we worry about privatization of the data. If backup is kept off-line (or on) bit-rot

Challenge

The start of bulletin board systems was accompanied by science fiction that worried about nefarious use of encrypted communication. There are so many ways to communicate, in the open and in “private” that I will not worry about that.

Naming

A catchy name is needed for new (or old) concepts hoping for acceptance. Meme's welcome.

  • Container
  • time capsule
  • cache
  • vault
  • registry
  • notary...
  • store
  • registry
  • repository
  • What stored
  • plans
  • myplans
  • experimental time capsule
  • experiment registry
  • my notary proposal (note the favored mnp acronym)
  • notebook repository
  • lab notebook snapshots
  • file
  • methods
  • Combined terms
  • methods cache
  • experimental methods
  • journal of pending results
  • registry of experimental design and data (redd)
  • Bare terms trying to be memes
  • knox no locks
  • I did it
  • I got it
  • Proof
  • 200 Proof
  • prior art
  • been there
  • done that
  • remember when
  • back then
  • my history
  • keeper of the flame
  • whats your plan

We want to go viral if we want lots of attention and use. More relevant for advertising or other money making ventures. And a dot com name, not a dot org name.

Academia, not so much.

Meditations on the Statistical Physics of Information Storage

The details of the proposal for a Lightweight Registry remind the author of the interesting proof from Introduction to Statistical Physics. That proof suggested that information storage need involve no energy. But retrieval does involve energy. And changing existing storage also requires energy to clear, to read and revise if necessary.

In like manner, a lightweight record keeper need keep no state or extra information. When limitations like number of requests per day or time between requests are placed, the programming energy costs go up, sometimes a lot if security is involved. Keeping cookies is work, and may require permission from the user, depending on reference frame. Again, increasing transaction energy and cost.

The original proposal from 2012 is included here. Since it too is outdated, it is mostly shown in lighter text.

If researchers in a field were to file their methodologies and predictions prior to experiment with a registry, the subsequent results should have more power and respect in that field.

Required submission: length and more checksums (and proof that a human is submitting)

Optional submissions: Topic, Title, Author, Contact Info, Date, Keywords, Text. Any information can be kept “private” for a period of time chosen by the submitter.

The subsequent papers on that experiment would quote a submission number and length and checksums and provide the document that matches. This would allow readers to know the methodologies and predictions at the time of submission to FR Journal (jfr.com is taken).

The registry would take no view on the reliability of the checksums or the information submitted, only that the submission was made with the data provided. The users would decide how much to trust. For example, if it is subsequently found that a 1M file with a CRC32 and an SHA-256 is easily modified while maintaining length and sums, then the value of the submitted information would go down.

The data would be stored off-line after a (short?) while, rather than being maintained only on-line. Verifying old submisions might cost and be a minor profit source. Or bringing an old submission up for public view for a while might cost.

The Future Results Journal may be more relevant in fields with more and smaller experiments and in fields where variation is greater such as medicine, sociology, economics, biology, environmental science.

The initial idea stems from seeing medical research performed “to significance.” Which has significant negative results.

Monday, January 17, 2022

Musings oN Particles

Herein, a few demonstrations of thinking in the mnp and Constituent Models. This blog grows out of ongoing revisions to Appendix B of the main mnp Model document, An Architecture for the Fine-Grained Structure of Everything. One paragraph on Beta + decay of fluorine18 grew into pages on quarks and the exchange of charge material seen as basic to weak and strong exchanges.

Quark Charges

Quark charges seem to be exactly -2/3, -1/3, 1/3, and 2/3 of the elementary charge of the electron/positron e+. Perhaps with puzzling corrections where the gluons seem to have a bit of charge in some types of experiment. The mnp Model can explain those ephemera as a result of the quarks contending for charge material. The mnp Model uses the basic experimental result to suggest that, mathematically and geometrically, those charges can be formed by combinations of +1/6 and -1/6 and that the quantum of charge is actually 1/6 of the elementary charge. In the mnp Model, these sixths are seen as filament loops. In the (or a) Constituent Model, the charge structure remains as just sixths with greater affinities for like charges and less for opposite charges, but quantized nonetheless.

Up is five positive plus one negative unit of (the new) quantized charge. Down is two positive and four negative.

Having a consistent size of charge structure for quarks has structural purity. The sixths of a charge picture allows positrons and electrons be “degenerate” quarks, which is attractive conceptually.

Current physics vocabulary does not seem to have a term for the smallest measured items with charge, so the author is casting about for alternatives. Lepton includes neutrinos but not quarks. Quarks include only fractional charges. New terms might be particulate, particulite, kwark, fepton, six-pack, six as a noun. No good word starting with f comes to mind. Fwark seems forced; the pun on fork might entertain some versed in software development but will dismay many others. For now, the author will use italic six as a noun. And call it \mnplepton in the latex source.

This picture of sixths also allows a three positive plus three negative “quark” that would be stable until it encounters another quark, when it would probably trade three of one charge or the other to convert the encountered quark into its charge opposite and produce a positron or electron.

This neutral six has not been seen in experiment, unless the Z is a candidate. Since it is more mixed in charge structure, the mass/size of the six's is expected to decrease from z to down to up to electrons and positrons.

This document will appropriate the letters n and p for the negative and positive quanta. Those are loops that strand as six in the mnp Model and just sixths in the Constituent Model. Apologies to particle physics for the overlap among the 26 letters. So the table of the charge structure of six's would be:

Quantized ChargesNet ChargeParticle Name
0n 6p+1positron
1n 5p+2/3up
2n 4p+1/3anti-down
3n 3p0z
4n 2p-1/3down
5n 1p-2/3anti-up
6n 0p-1electron
Charge Structure of Basic six Units

The n and p notation is also used in discussing and diagramming the lay (layout) of filaments in strands. Since this document uses loop and figment indicators much more than neutrons and protons this admittedly overlaps Particle Physics use of n and p. Again, apologies. This sixth of the elementary charge idea has been around a long time, at least since Post 12 (2012-10-26) - Many New Possibilities for the Charge Structure of Matter

Neutrons Emitting Electrons

The mnp Model posits that charge material is neither created nor destroyed, though it may be hidden at times. Neutron decay needs the charge material of an additional six. From 11/04/11 (a palindromic date if we ignore the century), neutron decay wants one down quark to convert to an up, so in filament notation, the neutron pppppn nnnnpp nnnnpp becomes the proton pppppn pppppn nnnnpp. Maybe a more readable way to write that is the neutron ppp ppn/nnn npp/nnn npp or 5p 1n/2p 4n/2p 4n becomes the proton ppp ppn/ppp ppn/nnn npp or 5p 1n/5p 1n/2p 4n. A solitary neutron would need filaments nnn ppp to change to a proton and create an nnn nnn which is an electron. The spaces are used like the thousands separator in currency notation and do not indicate that six's have a three and three structure. If nnn nnn and ppp ppp are recruit-able with a big enough photon in a high energy decay/collision experiment, then nnn ppp should be available too.

Starting with

        p p
       p   p
        p N             p p
                       n   p
    p P     P p         n n
   n   n   n   n
    n n     n n
One of the two down will attract an n from the z (which holds its filaments less tightly) in exchange for the p not in contention.
        p p
       p   p
        p N             p p
                       p   p
    p P     P n         n n
   n   n   n   n
    n n     n n
That down (which has changed to an anti up) then attracts another n in exchange for the P in contention, which is no longer in contention but an integral part of the new up. The remaining n in the new up becomes a victim of contention as the new up tries to take the P in contention from the remaining down. This leaves the incoming z as an up with its N in contention, behaving and looking exactly like an up in a nucleon.
        p p
       p   p
        p N             p p
                       p   p
    p P     n n         N p
   n   n   n   n
    n n     n n
which is bound to the original up and one of the original down as a proton, leaving the electron free.
   p p       p p
  p   p     p   p
   p N       N p

        p P            n n
       n   n          n   n
        n n            n n

The mnp Model suggests that a neutron in deep, empty or cold space cannot decay unless it encounters such filament loops. Whether the six figment loop of 0 net charge item called a z (the seventh and only neutral six in the Models) actually exists is open for debate. The LEP experiment at CERN did not find such a particle.

The author does not expect single filament loops to be available in just the right numbers for recruitment, though that is a possible explanation if experiment never finds z's as nnn ppp six's or particles. Single unaffiliated filament loops may well be present away from galaxies and might be part of dark matter.

Musings About 18F9 Decay in the mnp Model

Charge material conservation and figment and filament recruitment are central to the mnp Model. As an illustration, consider 18F9 becoming 18O8, for which two modes are possible. The more common is direct positron emission, the less common electron capture.

18F9 Beta Plus Decay

To give off a positron and convert a proton into a neutron, the mnp Model attempts a mechanism as follows, in keeping with the charge material conservation principle of the Model.

For reference, up is, in sixths notation, ppp ppn. Down is nnn npp. The proton is ppp ppn/nnn ppn/ppp ppn where the two up quarks are trying to recruit the same p filament coil from the down. If the two up were trying to recruit different p filaments from the down, the reaction would complete like most weak interactions in about 10-8 seconds yielding 2 positrons and an electron.

The neutron is nnn ppn/ppp ppn/nnn ppn. The competition here can be seen as both down trying to recruit the n filament coil from the up. Or as the up is trying to recruit a p loop from each of the down. For a proton to decay to a neutron and a positron, additional charge material is needed. Picture the original proton in filament picture notation, with 12p and 6n:

      n n
     n   n
      p P

  p p     p p
 p   N   N   p
  p p     p p
This needs to become, in beta+ decay, a neutron and a positron, with 9 n, 9p, and a 6 p positron:
      p p          p p
     p   p        p   p
      p N          p p

  p P     P p
 n   n   n   n
  n n     n n
An additional 3n and 3p is needed. If the proton is relatively exposed in the unstable fluorine-18 nucleus, so it is not protected by the other nucleons, and it encounters a neutral z, the hypothesized 3n 3p six.
      n n          n n
     n   n        n   p
      p P          p p

  p p     p p
 p   N   N   p
  p p     p p
The strongest attraction for rearrangement comes from the two up, which have 5 p's to attract a sixth though both are already distracted by competition for one of the P's in the down. The six z might be considered a donor by the two up's, which would likely attract different filaments of the z.
      n n       n n
     n   n     n   p
      p P       P p

      p p       p N
     p   N     p   p
      p p       p p
Since the z is not attracting its three p's as much as the up is attracting p's, one of the up will win a p from the z, which z then becomes a down. Since the remaining up is trying to gain a P from the now down which has been the z, we have the picture of a neutron with a freed positron:
  n n     n n
 n   n   n   n
  p P     P p

      p N          p p
     p   p        p   p
      p p          p p

18F9 Electron Capture

The electron capture picture starts here. This picture has been harder to develop. For an up to become a down when an electron is captured, many images of the change are possible.

From conservation of charge material, proton 5p1n 5p1n 4n2p plus an electron 6n to yield a neutron 4n2p 4n2p 5pn1 starts with a total 12p and 12n and appears to end with 3p3n. If charge material is conserved, it appears that 3p3n has disappeared. The mnp Model answer would be that a z has been created. Still, changing the quarks is not easy.

For a down quark, it would need to lose one n and gain a p. But the result needs not just the existing down but a second. For an up quark to become a z involves losing two p to gain n. The closest relative to the electron is the down quark, which would entail losing 2 n and gaining 2 p. A direct exchange of 2 strands between electron and an up would seem to be called for. Explaining that is a challenge, though randomize and see what is stable emerge is one approach.

The hardest part of an electron capture explanation is starting the breakup of the electron.

The original situation in filament picture notation where capital letters indicate the filaments involved in contention shows a proton (up up down) and an energetic electron:

      n n          n n
     n   n        n   n
      p P          n n

  p p     p p
 p   N   N   p
  p p     p p
The total input is a proton, with 12p, 6n and a 6n electron. Picture the expected result, a neutron and a positron, with 9 n, 9p, with the disappering 3 p and 3n as a z.
      p p          p p
     p   p        p   n
      p N          n n

  p P     P p
 n   n   n   n
  n n     n n

Perhaps the simplest explanation: an electron is in proximity and with the compatible spin when a positron is created in Beta + decay and the two annihilate to become not one but two z's. Those z's must be of a size to absorb a reasonable amount of energy.

For a direct explanation, the electron needs to be or become energetic enough that its coils are opened up to a similar radius as the quark with which it will start exchanging.

Maybe the down wrestles an n from the electron to yield two anti up and the two up still contending for the P in the original down.

   n n     n n
  n   n   n   n
   n P     p n

  p p     p p
 p   N   N   p
  p p     p p
Then the new electron turned anti up tries to get an N from one or both of the up, since those N's are already accessible.
  n n     n n
 n   n   n   n
  n P     P n

  p p     p p
 p   N   N   p
  p p     p p
This contention appears nominally symmetrical. That might pull one of the anti up into close proximity with a down so that the coils can more closely align. If some portion of those coils arrange to a stranding of 3p 3n of the non-contending filaments, the coils will expand to a higher radius and separate from the other. Leaving briefly
  n n     n      p n
 n   n   n      p   n
  n P     P      p n

  p p     p
 p   N   N
  p p     p

The two 3 strands are still involved/intertwined with each other, so the N or P might drop out of contention. To go toward the observed result, the N would drop out and somehow the anti up gets a p from the nascent six. The author is not willing to end with either QED or the simple details are left to the reader. This is not satisfying. Worse ideas can be found in the JNR Appendix to the main mnp document.

18F9 Electron Capture - A Better Explanation

Direct explanation, number two, is just that the electron is compatible in energy and spin to one of the up, intertwines, and some of the coils reach 3p 3n and expand to separate from the other 6 strands. The temporary result can be pictured

  n n     n      p n
 n   n   n      p   n
  p P     n      p n

  p p     p
 p   N   N
  p p     p
the resulting six is a down, which is not interested in losing an N but in gaining one by latching onto the N already in contention, trying to give up a P.
  n n             p n
 n   n           p   n
  p P    n n      p n
        P   n
  p p    p n
 p   N
  p p

The nucleon stays intact. Voilà. With only one major appeal to magic. A slightly more satisfying explanation for electron capture. At least as a demonstration exercise in thinking about charge conservation and in recruitment toward stability, Not a total loss as a thought experiment. One hopes.

This emphasis on charge material conservation leads the author to suggest that the cross-section values for various interactions are not single numbers when the reaction depends on something outside or additional to the particles involved in the reaction. Some reactions like neutron decay may not happen in deep space, with little around. Vacuums in proximity to mass are not empty; energy in the form of recruitable m 's is available. Dark matter may be mostly recruitable, so some regions around galaxies are not empty either. And yet, the author finds himself, once again, suggesting alternates to the established physics. With no expectation of being persuasive.

Gamma Particles

From 11/05/11, another palindrommic date, Gamma particles from electron-positron destruction are seen as not just fhotons made up of \m-figments the way fhotons are pictured in the mnp Model. They are not even particles with a given size. They definitely are mostly energy, the m figments as energy released by the reaction. They also contain \ni and \p figments traveling at the speed of light. Those charge material figments are currently seen (2022) as staying organized in the quantized filament loops that provided the structure for the original particles. The mnp Model does not see the loops as being broken up by high energy reactions.

All n, p, and loop filaments n and p lack the ability to travel the very long distances that real fhotons have. Charge material will scatter faster.

If coils DO break up in high energy collisions, the individual figments will be hard to recruit into loops and thus would be seen as adding to dark matter in the current universe. Since the mnp Model sees black holes as retaining only figment count, momentum, and quantized charge material loops, this would also lead to loss of a significant portion of the only information retained in black holes. So perhaps the author's preference for the persistence of figment loops has an inherent bias toward existence.

The mnp and Constituent Models see weak interactions as the exchange of quantized charge materials between particles leading to different particles and the strong force as quarks attempting to exchange charge material but being prevented by the contention of another quark for the same quantized charge material.

Monday, January 10, 2022

A Tale of Two Models

The mnp Model may be presented either as a specific structural model with three entities and three effects that combine and operate as the universe or as a general conceptual model comprised of constituents moving at c. So instead of a single linear exposition, the author is faced with two (nay, more) choices. This dilemma has been faced before. Based on Dickens' model, here is one draft of a start with the original included for reference. On first reading, choose a column.

mnp/Constituent ModelsDickens
Adaptation:Original:
A Tale of Two ModelsA Tale of Two Cities
I. The EpochI. The Period
It was the best of times,It was the best of times,
it was the worst of times,it was the worst of times,
it was the age of wisdom,it was the age of wisdom,
it was the age of foolishness,it was the age of foolishness,
it was the epoch of belief,it was the epoch of belief,
it was the epoch of incredulity,it was the epoch of incredulity,
it was the season of Understanding,it was the season of Light,
it was the season of Dark Energy,it was the season of Darkness,
it was the spring of hope,it was the spring of hope,
it was the winter of despair,it was the winter of despair,

we had everything before us, we had nothing before us, we were all going direct to Understanding, we were all going direct to Confusion

we had everything before us, we had nothing before us, we were all going direct to Heaven, we were all going direct the other way

— in short, the period was so far like the present period, that some of its noisiest authorities insisted on the Models being rejected, for good or for evil, as the height of folly, vanity, and foolishness with a priori no chance of success.

— in short, the period was so far like the present period, that some of its noisiest authorities insisted on its being received, for good or for evil, in the superlative degree of comparison only.

There were established journals and authorities on the thrones of science.

There were a king with a large jaw and a queen with a plain face, on the throne of England; there were a king with a large jaw and a queen with a fair face, on the throne of France.

In all Disciplines it was clearer than crystal to the lords of the Discipline preserves of wisdom and knowledge, that things in general were settled for ever.

In both countries it was clearer than crystal to the lords of the State preserves of loaves and fishes, that things in general were settled for ever.

Or not.

Thank you, Charles Dickens. Original here: http://www.gutenberg.org/ebooks/98

In many ways, the present period is not so different from the year of the Current Era one thousand seven hundred and seventy-five. Or it is. Different.

So the mnp/Constituent Model exposition will be a Tale of shuttling back and forth between Two Models with a common origin but separated by a channel of specificity. This Tale is offered in quest of understanding and of an alternate to the current and Standard Models.

The current models have been preserved one hundred eighty, one hundred fifty four, one hundred forty five, one hundred thirty four, one hundred sixteen, one hundred thirteen, one hundred two, ninety three, ninety two, ninety one, and fifty one years, depending on which Current Model one chooses, by diligent experiment and explosive development of useful product. Preserved also by acceptance of the contradictions and unknowns with the promise one makes in science to revisit mysteries and other rough edges. (2)

The two new Models ARE based on the exposed bedrock of physics. The speed of light, c, is a constant. Experiments and the universe Exist (E). The general Model can be considered the Continental Model, since it has some mathematical connection to the rest of physics. It has been christened the Constituent Model. The more specific Model may be considered the island Model, since it appears untethered to any existing theory. It has been christened the mnp Model, for the three basic entities mediators, negatives and positives seen as making up matter, energy, and fields. The mnp Model adds an understanding of the third foundation/leg of modern physics, the Planck constant h.

The quest for novel understanding will be interesting. The tale unfolds...

Local Addendum - Current Model Dates

Pick your metric:

AreaTopic/ScientistYear
Statistical MechanicsBernoulli1738
Maxwell 1859
Boltzman 1864
Statistical Mechanics proper1870's
Statistical Mechanics as a term by American mathematical physicist J Willard Gibbs 1884
Boltzmann's collected Lectures on Gas Theory 1896
Gibbs Elementary Principles of Statistical Mechanics, which formalized the basis of statistical mechanics and which was found to be very general1902
Electro MagnetismMaxwell's equations1864
Maxwell's Treatise on Electricity and Magnetism1873
RelativitySpecial Relativity 1905
General Relativity 1916
Quantum Mechanicsin matrix form by Heisenberg Born and Jordan 1925
in wave form by Heisenberg Pauli and Dirac 1926
as the Heisenberg Uncertainty Principle and the Copenhagen Interpretation (Schrödinger)1927
The Standard Model1967