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Updated in November 2005
The
articles that follow were presented for the first time on the occasion
of International Conferences and were published in the volumes of
proceedings of these meetings, in particular:
- The
P.I.R.T MEETING (Physical Interpretations of Relativity Theory) held
every two years at the Imperial College of London, sponsored by the
British Society for the Philosophy of Science, Michael C. Duffy
Chairman.
- Geometrization of Physics meeting, held every two years in Kazan
State University, Russia, Victor Bashkov Chairman
- Meetings organized by Franco Selleri and published in collective
books:
- Advances in Fundamental Physics
-
Open Questions in Relativistic Physics
The
articles are directly available by the buttons placed below.
The main ideas of these manuscripts were registered at the French
Society of authors.
The versions presented in this web site were slightly modified in
regard to the original ones, by taking account of new theoretical or
experimental data. But the guiding line remains unchanged. (Most of the
references quoted in the bibliography of our articles are present in
this web site in updated form.)
The ideas developed in these texts rest on theoretical and experimental
bases. They call into question some dogmas and lead to really new
concepts in Physics. The basic concepts
are presented in a synthetic form in a book entitled "From Galileo to
Lorentz and beyond", published by Apeiron. Email Apeiron@vif.com, web
site http://redshift.vif.com. For further information click here The book
can be ordered at the publisher's adress, or at the adresses of the
great distributors (Amazon, Blackwell, Garner, etc).
- Let us first bear in mind some of the principles
considered as basic in conventional physics that will be called into
question and criticized subsequently.
1-
Special relativity assumes the existence of "inertial" frames. All
these frames are therefore considered equivalent for the description of
the physical laws (Relativity Principle).We will endeavour to verify if
the structure of the physical world enables the existence of frames
really inertial (which implies the nonexistence of an aether drift)*
From 1905 to 1916, the aether was considered as inexistent by most
relativists, but from 1916 Einstein reconsidered his initial position
and formulated a new concept of aether (required by General
Relativity). According to him, “this aether may not be
thought of as endowed with the quality of ponderable media, as
consisting of parts which may be tracked through time. The idea of
motion may not be applied to it”. We will verify if this new
concept of aether is compatible with other well founded data
2- According to special relativity, the kinetic energy is assumed to
take the form in all
"inertial" frames. It reduces to in all
cases when V<<C.
3- The real one way speed of light is considered as identical and equal
to C in all directions of space (isotropic) and independent of the
"inertial" frame in which it is measured. The methods of measurement of
C are not called into question.
4- The simultaneity of two events is viewed as relative to the observer.
5- The interval of time between two instantaneous distant events is
considered as relative and dependent on the speed of the observer who
measures it.
6- The space-time transformations which connect any two "inertial"
frames are assumed to take the form of the Lorentz-Poincaré
transformations in all cases.
7- According to conventional relativity the contraction of moving
bodies is observational and reciprocal, (which implies that there is no
real contraction).
8- Speeds are considered only relative: there is no absolute velocity.
9- The rest mass of a body is assumed to be the same in all "inertial"
frames. Thus, the law applies
identically from all of them.
10- The method of slow clock transport is supposed to enable exact
synchronization of clocks.
- Criticism of the above-mentioned principles.
Most of
these statements follow from measurement distortions.
In effect when we measure the length and the time, we make systematic
errors because we use contracted meter sticks and retarded clocks. In
addition, as we will see, we make systematic errors in synchronizing
the clocks.
The simultaneity of two distant events is also falsely estimated.
In answer to the10 above mentioned statements we will demonstrate that:
1.
Several experimental and theoretical arguments speak in favour of the
existence of an aether frame in a state of absolute rest (cosmic
substratum) which is not compatible with the strict application of the
relativity principle.
The new concept of aether published by Einstein after 1916 is
demonstrated to be at variance with the experimental facts.
See the articles “Critique
of some assumptions of special relativity and arguments in favour of an
aether frame”
chapters I and III, “Extended
space-time transformations for a fundamental aether theory ”
and “Is the
relativity principle an unquestionable concept of physics”.
2. The conventional expression of the kinetic energy is completely
exact exclusively when it is measured from the aether frame.
See the article “Extended
space time transformations for a fundamental aether theory”
Chapter IV
(conclusion).
3. The speed of light is isotropic and equal to C exclusively in the
aether frame. But because of the systematic measurement distortions due
to length contraction, clock retardation and unreliable clock
synchronization, it is found equal to C in any "inertial" frame.
See the article “How
the apparent speed of light invariance follows
from Lorentz contraction” , and "Extended
space-time transformations for a fundamental aether theory ”.

4. The simultaneity of two distant events is absolute. It only seems to
be relative because we make a confusion between the instantaneous
events as such and the light signals issued from them Consult “Critique
of some assumptions of special relativity and arguments in favour of an
aether frame” chapter II and “Is
simultaneity relative or absolute”.
5. Clocks in motion are slowed down with respect to clocks at rest in
the aether frame. The real interval of time between two events does not
depend on the speed of the observer, but as a result of clock
retardation it seems to be modified when this speed is changed.
(In effect suppose that an event is simultaneous with the indication of
a clock showing 8h and that another is
simultaneous with a clock showing 10h, both
clocks being at rest in the aether frame. As far as the simultaneity is
absolute the real time of the events will be 8h
and 10h for all observers, at rest or in motion
with respect to the aether frame. So the real
interval of time appears to be absolute).
Consult “Critique
of some assumptions of special relativity and arguments in favour of an
aether frame” chapter II and “Is
simultaneity relative or absolute”.
6. The space-time transformations connecting two "inertial" frames take
the form of those of Lorentz-Poincaré exclusively when one
of them is at rest in the cosmic substratum. In all other cases they
take a different form.
The space-time transformations conceal hidden variables which are
nothing other than the Galilean transformations. Consult the papers “Extended
space-time transformations for a fundamental aether theory”
and “Hidden
variables in Lorentz transformations”.
For more detailed explanations consult “Relativity
and Cosmic substratum”.
7. As we have already seen, the real value of the speed of light is
equal to C exclusively in the aether frame. Contrary to what is often
believed, this is confirmed by a number of experimental facts. In all
other frames it is equal to (where is the speed of the frame
with respect to the cosmic substratum).
Assuming this result and the equality of the two way transit time of
light along the two arms of Michelson's interferometer, (a fact more
and more confirmed by the modern versions of Michelson’s
experiment) we demonstrate that length contraction, real and non
reciprocal becomes an unquestionable fact.
Consult the article “How
the apparent speed of light invariance follows
from Lorentz contraction”.
8. The existence of an absolute aether frame implies the existence of
absolute speeds.
See the articles “Critique
of some assumptions of special relativity and arguments in favour of an
aether frame” , chapter III and “Is the
relativity principle an unquestionable concept of physics”.
9. The rest mass of a body is different in the different "inertial"
frames. The law is
completely exact exclusively when the observer makes the measurement
from the aether frame. From all other "inertial" frames, it takes a
different form.
Since the Earth frame moves at low speed with respect to the aether
frame , the law appears approximatively exact
in the Earth frame.
The mass depends not only on the quantity of matter but also on the
relation of matter and aether.
Consult “Mass
and energy in the fundamental theory of space and time”. and “Critique
of some assumptions of special relativity and arguments in favour of an
aether frame” 
10. The method of slow clock transport does not allow exact
synchronization of clocks. It is equivalent to the
Einstein-Poincaré procedure which makes use of light
signals. Both methods, when they are used to measure the speed of
light, give (erroneously) the values C in all inertial frames.
Consult “Synchronization
procedures and light velocity”.
For
more detailed explanations the reader can consult “Some
important questions regarding Lorentz-Poincaré’s
theory and Einstein’s relativity I and “Some
important questions regarding Lorentz-Poincaré’s
theory and Einstein’s relativity II”.
* In all the articles presented in this
web site, we call "inertial" the frames in which a body at rest is not
submitted to perceptible external forces, a term sanctionned by
use.Yet, we must be aware that, insofar as an aether drift exists, real
frames cannot be perfectly inertial, which means that the relativity
principle does not strictly apply. The
implications for fundamental physics are shown to be far-reaching.
Important note
Some of
the papers presented in this web site have been slightly modified in
regard to the originals, (in particular those published before 1988);
in effect at that time we had not yet found the decisive arguments
calling into question the application of the relativity principle. So
we could suppose that the law (which
is usually derived from this principle) was at variance with the other
postulates of Lorentz (aether, length contraction). This result (if
confirmed) appeared at first sight, as an important objection against
the postulates of Lorentz.
But since then, we have found a number of arguments demonstrating that
the relativity principle is not an unquestionable concept of physics
(since it does not strictly apply in the physical world) and that the
law can be derived without its help provided that be the rest mass in the
fundamental frame and not in any inertial frame. In consequence of
which the law does no longer appear in disagreement with the other
postulates of Lorentz.
Acknowledgements
We are
grateful to the colleagues who have supported a part or the whole of
our work, in particular
Pr V. Bashkov, Chairman of the International conference Geometrization
of physics, Kazan State University, Russia.
Dr M-C Duffy, Chairman of the International Conference, Physical
Interpretations of Relativity Theory (PIRT), Imperial College London.
Pr B. Grossetete, Head of the Laboratory of Nuclear Physics and high
Energy, Universities of Paris VI and Paris VII.
Pr P. Marmet, University of Ottawa, Canada.
Pr F. Selleri, University of Bari Italy, Organizer of several
International Conferences dealing with Relativity and Quantum physics.
Pr J.P. Vigier, Laboratory of Relativist Gravitation and Cosmology
University of Paris VI, who, as a referee of our book, gave complete
support to the essentials of our work.
Pr H. Puthoff, Institute for Advanced Studies, Austin, Texas, USA. Pr
M. Jammer, Bar Illan University, Israel. Pr R.M. Santilli, Institut for
Basic Research, Palm Harbor, USA. Dr W. Cantrell, "Infinite Energy"
(Bimonthly Magazine of the New Energy Foundation), Concord, USA, for
the review of our book " From Galileo to Lorentz and beyond" he has
written in this journal.
We
would like to also thank the colleagues who have sent us letters of
encouragement on the occasion of one or several of our publications, in
particular: Dr R. Hock, Institut Laüe Langevin, Grenoble, Dr
P. Huber, University of Heidelberg, Germany, M.B. Guy, Ecole des Mines
St Etienne, France, M. V. Makarov, Paris, France, Dr G. Margalhaes Sao
Paulo, Brazil, Pr A. Peres, Israël Institute of Technology
(Technion), Haïfa, Pr T. E Phipps Jr, USA, or with whom we had
interesting exchanges of views, such as Pr H. Hayden, University of
Connecticut USA, Dr Y. Pierseaux, University of Bruxelles, Belgium, Pr
M. Sachs, University of New-York at Buffalo, Pr J. P Wesley, Blumberg,
Germany. We are grateful to late Pr S. Prokhovnik, University of New
south Wales, Australia with whom we have kept up a regular
correspondence during more than two years.
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