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Introduction
Since
its discovery(1), the "missing momentum" in nucleus-nucleus collision
provoked much experimental and theoretical work, but the real situation
is still not clear. This is because it is not "apparent", as some researchers
have suggested, but rather represents a real loss in nucleus-nucleus collisions.
Furthermore, this loss of momentum is a characteristic of both central
and peripheral projectile impacts on the target. As the projectile velocity
generally is large, and the velocity of the fragments produced by compound
nucleus disintegration is also large, special relativity equations are
used to calculate their momenta and energies. They are also used to calculate
the energies of the RaE(2) electrons emitted, 238U(3)(4) decay, muon decay(5),
and similar decay phenomena, annihilation phenomena, and anomalous mean
pass. It is well known that experimental values found cannot be explained
by the special relativity equations even though, in some cases, they can
be explained by the participating neutrino. However, in nucleus-nucleus
collision, nucleon annihilation, and anomalous mean pass, neutrinos cannot
be used, or at least, their use has not as yet been attempted.
Nucleus-nucleus
collision is important not only to understand the phenomenon itself, but
also because experiments reveal a surprising failure to conserve momentum.
This result is not a surprise, however, when applying the autodynamics
paradigm.
Autodynamics
We
are trying to demonstrate that the "missing momentum" in nucleus-nucleus
collision is real, i. e., it is not due to undetected particles, as in
the original definition(6). The arguments given in reference (7), page
615, regarding the undetected neutrons and justifying the loss of linear
momentum transfer, are irrelevant even though the detector used can only
detect charged particles, because if the phenomenon is symmetrical, the
momenta will cancel automatically. If the phenomena are not symmetrical,
the large number of the experimental results gives an LMT lower than 90
% of projectile momentum. When the LMT is small, the undetected particles
argument is still irrelevant. The difference between the experimental
values and the calculated ones is due to two things: the use of special
relativity equations to calculate the particles' momenta, and a special
*signature*. The difficulty in applying special relativity equations arises
because they can only be used when the particle energies are externally
provided(8). We normally apply special relativity kinetic energy equation
to the wrong cases! When the particles receive the energies from decay,
the momentum is less than when they receive energy from the external medium.
In these decay cases autodynamics equations apply(5). To see the Addendum.
In
fact, the momentum sum of the compound nucleus residues has nothing to
do with projectile momentum. This is very easy to see in Table I of reference
(9), because when the projectile momentum increases 3.75 times, the LMT
only increases from 230 to 265, producing a decreasing ratio in LMT-projectile
momentum, from 0.83 to 0.48. When the folding angles are close to 180o
the LMT are small, and when the former decreases, the LMT increases. There
is an inverse ratio between the fission fragments' folding angle and the
LMT. The larger the folding angle, the lower the LMT.
A
few different cases will be given as calculated examples. The autodynamics
equations used to calculate are(2,8):
Ec = moc^2 [1 - (1- B^2)^1/2]
m = mo (1- B^2)^1/2
p = mo (1- B^2)^1/2 v
Where
Ec = Kinetic Energy, m = mass, p = momentum, B = v/c, v = particle velocity,
c = light velocity.
It
will be supposed that the collision between projectile and the bombarded
nucleus is central, and compound nucleus fission is symmetrical with respect
to its center of mass with relativity and autodynamics momenta conservation.
The values given in Table I show the small difference, in the center of
mass, between special relativity's (SMR) and autodynamics' (SMA) momenta,
only 2 %, meanwhile the difference between the LMTA and LMTR is 12 % (PLMTAR=88
%) on the laboratory system. This results in a special *signature* for
nucleus-nucleus collision. This special signature is given by the fact
that fission is characterized by two heavy fragments (mass between 70
and 170 MU) flying away with large angles, forming a "folding angle" close
to 180 degrees, and also light nuclei, and especially, the very light
particles such as alpha, tritium, deuteron, neutron and/or proton, generally
at small angles, where the autodynamics momentum, compared to special
relativity's momentum is smaller, contributing more to an LMT difference.
There is an inverse relation between folding angle and partial or total
LMT due to the fact that an important part of the LMT is given by P|R
(Ref. (6) Fig, 4 and 5) and this "is mainly determined by the folding
angle TAB=TA + TB between the two coincident fission fragments", ref.
(6) page 1931 2o column. Considering full LMT the situation is the same,
ref. (16) Fig. 7.
In
Table II there are not either symmetrical energies or fission fragments
of equal mass (A=80, B=120). The LMT is considerably smaller because the
folding angle increased by 10 degrees, and the ratio autodynamics/relativity
decreased to 78 %, even though this case is favorable with respect to
Table I, because the light particles' energies are greater.
When
the LMTA is equal to projectile momentum the special relativity calculated
values (LMTR) are at 108 % of the projectile momentum. This value is very
close to the maximum value reported, about 120 %, even though the probability
of finding this value is very small, and normally, the LMT is smaller
than the projectile momentum. (Ref. 16, Fig. 12; Ref. 7, Fig. 2; Ref.
9, Fig. 7 and 8; Ref. 17, Fig. 3).
But
if in Tab. I we make EA, EB, equal to 113 MeV (kinetic energy 1/2) and
angles A=102o and B=258o, the "critical"(6) folding angle is 173.4o (FAR)
and the LMTRA is equal to 74.8 %. If in an example like this we look for
values to find an LMTA equal to projectile momentum (autodynamics momentum
conservation) the LMTR will increase to Õ 125 %.
It
is surprising that to our knowledge, not one author comments on this compound
nucleus fission energy. It is accepted by everyone that there is an excitation
energy in the compound nucleus, and it seems that the fission residue
energies after compound nucleus decay are bigger than the projectile energy.
If this is the case, where do the fission residue energies come from?
Of course, part of the energy is given by the projectile energy, but the
complementary part must be provided by compound nucleus mass decay.
The Chain Reaction
In
reference (9) the authors propose to use the technique to produce a heavy
nucleus. It is possible to form a new and important conclusion regarding
the phenomena: it seems, looking at the experimental literature, that
in each fusion-fission reaction the compound nucleus fission energy is
bigger than the projectile energy. If this is the case, it should be possible
to produce a chain reaction using an inexpensive element like Pb(10) mixed
with other inexpensive elements to form a compound material with the capacity
to maintain the chain reaction. Of course, this could be a long road,
but the scientific possibility is a real one.
In
Table I we probably gave to each fission product a kinetic energy that
is too large, reference (6) page 1933-1934-1935, reference (11) page 2188,
reference (9) page 2529, reference (12) page 1948 (Here C energy peaks
around 215 MeV), reference (13) page 418, but when the kinetic energy
values are reduced to 1/2, the LMT proportion is approximately the same
even though its value is bigger.
If
in this example, we reduce the fission fragment and all residue energies
to 1/2 of their original ones (ET=1600 MeV), the final total energy is
2.54 times bigger than the projectile energy. If we reduce those energies
to 1/4, the final total energy is 1.27 times bigger than the projectile
one. But in the last case especially, the calculated statistical value
is too small with respect to the residues' emission probability. For example,
there is only a small quantity of carbon under a value of 100 MeV, and
no boron under 50 MeV (Fig. 6 of Ref. (6)) and 1/2 or 1/4 of its original
value is 100 and 50 MeV, respectively. In the beryllium case the original
energy is 125 MeV, and 1/2 and 1/4 of this value is 62.5 and 31.75 MeV,
a region where there are only small quantities of Be, if in fact there
is any at all.
A
realistic value could be 1/3 of the original energy, and in this case,
the ratio is 1.7 times bigger than projectile energy. If this is the case,
to satisfy energy conservation, it is necessary to look at the contribution
of decay of a portion of the compound nucleus mass.
In
reference (9), Table I, TAB=176.6o, p|=230+-20 MeV/c for 40 MeV proton
bombarding energy. Supposing that all the p| are produced by the two fission
fragments with equal mass of 119 MU, the kinetic energy is 135.6 MeV.
With TAB=175.9, p|=265+-20 MeV/c the kinetic energy is 123.81 MeV. The
first energy is 3.8 times bigger than the bombarding proton's, but in
the last case the energy is less than the projectile's. Evidently, there
is a question of performance (Ref. 9 Fig. 3 and 4, ref. (7) page 629).
A more realistic feature is what follows. We will only take for FF 25
% of p| value with the other 75 % produced by compound nucleus fission
residues. The reaction will produce two FF of 85 MU, 2 N14, 2 9Be, 2 alpha
particles, 2 tritons, 2 deuteriums, and 5 protons or neutrons. The fission
residue energies will be taken from experimental results. With conservative
values, the energy sum is bigger than the two cases calculated above.
With Ea>30 MeV (Ref. (12) fig 1 and 2), Ea>10 MeV (Ref. (15) fig
8 with T= 78o-156o and Ea>15 MeV with T=15o-68o, Ed>5 MeV fig.7
with T=78o-156o and Ed>10 MeV with T=15o-68o, Ep>5 MeV and Ep>10
MeV in Fig 6 with the same criteria. In Table I (ref.(15)) there are kinetic
energy averages for p, d, t, a and HI (heavy ions) that are bigger than
the above references cited. In many other experimental results the values
are even bigger. For the first case, with ref. (12) values, the ratio
is 4.3 times and, in the second case, the ratio gives 1.13 times the projectile
energy. If we take averages cited above, the ratios are 6.1 times and
1.6 times greater energy than the proton bombarding energy.
A
totally different situation is given in ref. (6) fig. 17 where P|R=1120
MeV/c (FF) and P|3=1520 MeV/c (9Be), and the energies of FF plus FR are
bigger than the projectile energy. The average excitation energy in table
I, of the same reference, is illustrative with respect to performance,
because the ratio is inversely proportional to projectile energy, even
though the connection between compound nucleus excitation energy and FF
and FR energies is unknown.
As
said before it is necessary to study this very carefully, but especially
by experiment.
Nuclear Waste
In
a meeting with Hans Kautzky, from Fermilab, to discuss a new experiment
with RaE(2) and a new theory of universal gravitation founded on interstellar
quanta of energy in the form of gravitons or neutrinos (17), he proposed
a new use for nucleus-nucleus collision: to bombard commercial and military
nuclear waste to transform these dangerous materials into nonradioactive
nuclei.
Conclusion
It
is necessary to perform new experiments to test concurrent fission residues,
that is to say, all compound nucleus residues, produced simultaneously
(prompt events), measuring the parameters in such a way as to make it
possible to calculate values that allow comparison of special relativity
predicted kinetic energies and momenta with those of autodynamics. As
a result of experiments already done, such information may have been recorded.
Obviously, this permits easy re-calculation using autodynamics equations,
and thus allows comparison of values. Researchers can take advantage of
this situation.
Acknowledgment
The
author thanks James M. Gavin for assistance in preparing the English language
version of this paper. Thanks the reviewer for his interesting comments
and suggestions.
TABLE I
CENTER OF MASS VALUES
Proj. C.N. F.A F.B B1 B2 Be1 Be2 a1 a2 N1 N2 N3 N4 N5 N6 ------------------------------------------------------ m 16 254 101 101 10 10 9 9 4 4 1 1 1 1 1 1 ER 315 20 225 225 200 200 125 125 80 80 55 55 60 60 55 55 EA 315 19 225 225 200 200 125 125 80 80 55 55 60 60 55 55 MR 3080 3080 6510 6510 1940 1940 1453 1453 776 776 324 324 339 330 324 324 MA 3016 3016 6487 6487 1878 1878 1420 1420 751 751 296 296 307 307 296 296 theta 90 270 315 135 15 195 10 190 5 185 355 175 8 188 ------------------------------------------------------
SMR 23339 SMA 22879 PMAMR 98.02 ET 1600 MT 254
LABORATORY VALUES
F.A.R 158.79 F.A.A 159.04 LMTR 3080 LMTA 2710 PLMTAR 88 PLMTR 100 PLMTA 89.86
Horizontal
Abbreviations
Proj. = Bombarding projectile, C.N. = Compound
nucleus, F.A = Fission Fragment A, F.B. = Fission Fragment B, B = Boron,
Be = Beryllium, a = Alpha particle, N = Neutron or proton particle.
Vertical Abbreviations
m = mass(MU), ER = Relativity kinetic energy(MeV),
EA = Autodynamics kinetic energy(MeV), MR = Special relativity momentum(MeV/c),
MA = Autodynamics momentum(MeV/c), theta = Angles(degree), SMR = Special
relativity momentum sum(MeV/c), SMA = Autodynamics momentum sum(MeV/c),
PMAMR = Percent of momentum A respect to momentum R(%), ET = Kinetic energy
sum(MeV), MT = Mass sum(MU).
Laboratory Value Abbreviations
F.A.R = Relativity folding angle(degree), F.A.A
= Autodynamics folding angle(degree), LMTR = Linear Momentum Transfer,
Relativity(MeV/c), LMTA = Linear Momentum Transfer, Autodynamics(MeV),
PLMTAR = Percent of Linear Momentum Transfer Autodynamics respect to Relativity(%),
PLMTR = Percent Linear Momentum Transfer, Relativity, respect to projectile
momentum(%), PLMTA = Percent Linear Momentum Transfer, Autodynamics, respect
to projectile(%).
TABLE II
CENTER OF MASS VALUES
Proj. C.N. F.A F.B B1 B2 Be1 Be2 a1 a2 N1 N2 N3 N4 N5 N6 ---------------------------------------------------------------- m 16 254 80 120 10 10 9 9 4 4 1 1 1 1 1 1
ER 315 20 200 200 210 235 125 160 85 90 65 105 70 90 60 75 EA 315 19 200 200 210 235 125 160 85 90 65 105 70 90 60 75
MR 3080 3080 5463 6689 1989 2105 1453 1645 800 823 354 454 367 419 339 381 MA 3016 3016 5441 6671 1922 2026 1420 1598 773 794 318 381 327 360 307 336
theta 96 264 315 135 15 195 10 190 5 185 355 175 8 188
SMR 23287 SMA 22681 PMAMR 97.4 ET 1770 MT 252
LABORATORY VALUES
F.A.R 169.31 F.A.A 169.71 LMTR 1301 LMTA 1018 PLMTAR 78 PLMTR 42 PLMTA 33
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L. Carezani. Physics Essays, 1. 269(1988)
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H. Kanna, H. H. Marshall. Phy. Rev., 57, 372(1940)
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L. Carezani. Physics Essays, 5, 19(1992)
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B. Back et al., Phy. Rev., 22, 1927(1980)
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PĒter et al., Nuc. Phy., A519, 611(1990)
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Walz, H.P. Noyes, R.L. Carezani. Phys. Rev. A,29,2110(1984).
The conclusion espoused in the paper by H.P. Noyes is irrelevant because
the electrons receive external energy from the klystrons' electromagnetic
field, confirming the Bertozzi experiment(14) and the special relativity
equation for kinetic energy. It is impossible then to compare one equation
with the other because autodynamics applies for decay cases.
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Fatyga, K. Kwiatkowski, H. J. Karwowski, L. W. Woo and V. E. Viola,
Phys.. Rev. C, 32, 1496(1985)
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K. Gelbke et al., Physic Report 42C, 311(1978)
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G. Sobotka et al., Phys. Rev. Lett. 51, 2187(1983)
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Bini et al., Phys. Rev. C, 22, 1945(1980)
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Berthier et al., Phys. Lett B, 193, 417(1987)
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Bertozzi, Am. J. Phys. 32, 551 (1964)
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Chbihi et al., Phys. Rev. C, 43, 652(1991)
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Mordhorst et al., Phys. Rev. C, 43, 716(1991)
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the gravitational quantum of energy seems to be very close to the neutrino
hypothesis, the author gives to this graviton the name of neutrino.
Addendum
In
a very interesting reviewer's report on this paper, the following comments
were made: "On the face of it, this claim (momentum conservation violated)
by the author is not very convincing to me because the conservation of
linear momentum is one of the most thoroughly tested laws in physics.
To abrogate it on just the basis of ad hoc experimental evidence cannot
be allowed. (There is always the possibility of error in the experiments)",
and "what I would suggest to increase the plausibility of the author's
arguments, would be to show that the use of his autodynamics is equivalent
to there existing some sort of "extra" (as yet unknown) physical process
with- in the collision event that absorbs the momentum discrepancy. He
should describe at least the rough nature of this "extra" physical process
(even if it is highly speculative). Thus he would stop intimating the
violation of momentum conservation.
However,
the author didn't abrogate the violation of momentum conservation on the
basis of ad hoc experimental evidence. He doesn't know the exactly number
of experiments carried out, but he can say that more than two hundred
were performed, and all of them confirm the violation of momentum conservation!!!.
The systematic application of momentum and energy conservation to all
phenomena of decay, from the RaE to proton-proton annihilation (including
the Compton effect) confirms that the autodynamics equations match the
experimental results obtained. The author come upon the autodynamics equations,
at the beginning, through a systematic discussion of systems (frames)
in relative movement. This was the foundation of a new theory of relativity
called autodynamics. But it is easy to demonstrate that the autodynamics
kinetic energy equation is general, that is to say, it can represent the
case where a particle receives energy from the external medium. (Special
relativity equation). We can write the autodynamics equation as follows:
Ec
= M [1 - (1 -B^2)^1/2 ]
If
M = mo c^2 we have the autodynamics kinetic energy equation. If M = mo
c^2 + Ec (rest mass energy plus kinetic energy from the external medium)
we have the special relativity kinetic energy equation:
1
Ec = mo c^2 [ ------------ - 1 ]
(1 - B^2)^1/2
From
the scientific view-point it has sometimes been possible to have two different
explanations of the same phenomenon (wave-particles, for example), but
"to invent something "extra" and "highly speculative" (in the words of
the reviewer) to explain the violation of momentum conservation in nucleus-nucleus
collision alone is to create another problem because the solution for
it cannot be used on *other* phenomena. The author's original discovery
was precisely that *all* phenomena have in common the violation of momentum
conservation, and these momenta violations come about from the systematic
application of special relativity kinetic energy equations, which are
inadequate in describing a decay phenomenon. We don't need to invent anything
new! A lot of new "particles", "forces", "physical process" were created
to explain new phenomena without success. Even Einstein's "cosmological
constant" was later considered by him "his greatest mistake". No, simplicity
is the rule in nature, and autodynamics is very simple! The explanation
is general, universal, and therefore applicable to all phenomena!
The
following is the complete second report by the same reviewer. I want to
publish the whole report because it is a very interesting analysis of
the matter and the answer permit to clarified many aspect of the problem.
"Actually,
I do not see that the treatment that he gives now has changed in any significant
way from the one given in the first manuscript. He is still opting for
the use of "autodynamics" kinematics in place of special relativity kinematics
in nuclear decay processes almost entirely on the basic of experimental
data. (He has rejected my suggestion of invoking "extra" physical processes.)"
"once
again, I cannot go along with this hypothesis since, in my view, special
relativity is one of the most established disciplines of modern physics.
Moreover, in the manuscript he advocates two additional "revisions" of
established modern physics that are completely "unpalatable" to me. He
rejects Pauli's theory of the existence of neutrinos and, what is even
more unlikely, he maintains that the charge of the electron is not constant
but decrease its value with velocity."
"As
I said before, in as much as I am not very familiar with the work that
has been done in experimental nuclear physics, I feel that it would be
inappropriate to make professional recommendations as to whether you should
publish this article or not. However, my personal opinion (for what it
is worth) is that you should publish it. As far as I can see, the article
is not blatantly "crackpot" and it does not have any readily demonstrable
errors in development. Not having these two failings and having (what
one must admit it) a novel approach, a journal such as yours, which does
not at all object to completely novel approaches, must be inclined to
publish this article."
"An
other consideration might be mentioned here. After all, the author has
discovered in his "autodynamics" formulas a mathematical format which
is able to fit all of the experimental data. (I am taking the authors
word that it is so). This in itself is worthy of notice. Both Galileo
and Kepler really did not do any more than this. It is just that he has
actually not provided a physical basis for using these "autodynamics"
formulas (at least in my opinion). I hope that my comments have been of
use to you."
The
author's answer is the following:
Thank
you very much for your new comment on my paper (N-N collision and A.),
especially for your last words.
I
beg your pardon, but I am not "still opting for the use of "autodynamics"
kinematics in place of special relativity kinematics in nuclear processes
................"
The
special relativity approach - its equations - were applied to all the
experimental results obtained up to now, from the first RaE, through 238U
decay, neutron decay, Cl38 decay, 7Be decay and similar, muon decay and
similar, nucleus-nucleus collision, anomalous mean pass, electron-electron
and proton-proton annihilation, but the experimental values found are
not explained by special relativity's equations. The first failure was
in the historical RaE (210Bi83) experiment. Calculating kinetic energy
with the velocity at the end point of the electron spectrum, the value
is 1.16 MeV, but the experimental value found is 0.36 MeV. Pauli invented
a "new particle" ( a ghost particle ) called neutrino by Fermi. Autodynamics
kinetic energy explains perfectly this experimental value of .36 MeV.
Einstein's equation fails but not Autodynamics. I am not "opting": I only
have autodynamics' equations, which can explain this phenomenon and in
fact all decay phenomena, indeed !!!.
I
am not rejecting your suggestion about an "extra" physical process !!.
Autodynamics doesn't need it because autodynamics explains all decay phenomena.
Autodynamics does not have any "extra" physical processes - at this level
- because it was developed with the classical relativistic conception
(Poincare-Einstein). Autodynamics' general theory about mass-energy-mass
transformation in the Universe, explains the perpetual changes, the perpetual
transformation of mass-energy as the most basic principle for the universal
evolution of matter (At this level the "extra" is relevant. You will see
it). The Compton effect, the canon ball, particles moving in an accelerator,
are all, basically, intrinsically, phenomena of decay. The canon ball's
chemical energy and the accelerator's electromagnetic energy come, originally,
from decay, from transformation of mass into energy.
I
agree with you: "Special relativity is one of the most established disciplines
of modern physics". But, I am sorry, with a condition: *until now, or
until 30 years ago, more or less*. Special relativity cannot explain any
decay phenomena. *It is useless in particle and nuclear physics*!! To
save special relativity it was necessary to create a lot of ad-hoc theory
for each phenomenon. Pauli's hypothesis has reached a crazy state: *neutrino's
delirium tremens. There are more than 40 or 50 different "qualities" for
neutrinos, all of them as "extra qualities", and most of them very frustrating,
indeed, and truly fantasies, really. Attached to this letter there is
a list that I prepared for another reason. I am not rejecting Pauli's
theory. Whether I reject it or not is irrelevant! *It is rejected by itself*!!
It is rejected by Autodynamics. The special relativity equations don't
apply to decay phenomena. Special relativity equations apply only when
the particles receive energy from the external medium. It is not my fault
if the wrong equation is applied to a decay case !!
I
"maintain that the charge of the electron is not constant ........." But
I maintain this only when the electron (particles in general) is going
through a process of decay!!! In the RaE decay, as example, the electron
doesn't decay!!! The neutron decay in an electron, and a proton, providing
the kinetic energy to both particles. This kinetic energy come from the
energy (mass transformation) that maintain bound the proton and electron,
in what we call the neutron - the sum of proton and electron mass is less
than the neutron mass. The electron here is "an electron", a normal electron,
"an entire" electron, and its electric charge is the total electric charge,
equal in movement to the value at rest!!! There is no electron decay,
there is no electron mass transformation into kinetic energy, and there
is no charge variation!!! The RaE is a decay process because the neutron
decay and the RaE lose the electron. But this electron didn't decay. It
is a formal electron. You can apply the electric charge variation equation
when the phenomenon exist, but the phenomenon doesn't exist because the
equation exist!!!.
The
"physical basis" of my theory is in the paper entitled "Fundamental Basis
for a New Relativistic Mechanics. Autodynamics". The ideas are very simple!
Please, find it enclosed. The English is not perfect but you will understand
the ideas. Please, improve it and let me know.
Regarding
your expression "is worthy of notice " I can tell you that my theory is
being taught in a Chinese University and it is receiving constantly more
support. If you are a professor you could start teaching Autodynamics
for the next generation. The principal reason why I am sending you the
paper is because in it, in section 13.- SO FAR AND BEYOND, you will find
"your" "invoking "extra" physical processes". You are going in the right
direction, I hope. I also hope Autodynamics will be the next paradigm
in the relativity field, particle, nuclear and plasma physics.
Your
comments are very important to me because I can test if my theory can
explain all the question!
Thank
you very much for your collaboration.
The
list about neutrinos mentioned above is the following:
Neutrino
Delirium Tremens
This
section comes from section 14 of the general Autodynamics theory paper
(not yet published):
14.- SO FAR AND BEYOND
14.1.-
Philosophy
Discussing
autodynamics' philosophical implications with a scientist, with regard
to the universal transformation of mass into energy, and vice versa, I
arrived at the conclusion that is possible to explain all phenomena as
decay process. When we are talking about external energy we think of something
striking the particle to increase its kinetic energy. But, another picture
is possible: the external energy - generally as an electromagnetic field
- is absorbed by the particle, it decaying later. The increasing kinetic
energy is a consequence of a decay process.
Whether
the total energy absorbed is converted into kinetic energy or part of
it is kept by the particle to increase its mass, will be a matter of discussion
in another paper about proton-proton annihilation. Actually, it is only
interesting that this accelerating process by external energy could be
interpreted as a decay phenomenon. The Compton effect was explained by
autodynamics as a decay phenomenon.
14.2.- Beyond
If
part of the energy is taken by the particle "without increasing its mass"
we will have "mass without weight", "mass without inertia", which will
be transformed in "inertial mass" at fission time, after the fusion of
the particles at collision time (annihilation)
To
special relativity, Newton's universe is relevant, but to autodynamics
a new different universe is opening. The fundamental "action" in the universe
is alternatively given by decay process and energy absorption.
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