Lets look at what Einstein had to say about it shall we?
From an address delivered on May 5th, 1920, at the University of Leyden:
How does it come about that alongside of the idea of ponderable matter, which is derived by abstraction from everyday life, the physicists set the
idea of the existence of another kind of matter, the aether? The explanation is probably to be sought in those phenomena which have given rise to the
theory of action at a distance, and in the properties of light which have led to the undulatory theory. Let us devote a little while to the
consideration of these two subjects.
Outside of physics we know nothing of action at a distance. When we try to connect cause and effect in the experiences which natural objects afford
us, it seems at first as if there were no other mutual actions than those of immediate contact, e.g. the communication of motion by impact, push and
pull, heating or inducing combustion by means of a flame, etc. It is true that even in everyday experience weight, which is in a sense action at a
distance, plays a very important part. But since in daily experience the weight of bodies meets us as something constant, something not linked to any
cause which is variable in time or place, we do not in everyday life speculate as to the cause of gravity, and therefore do not become conscious of
its character as action at a distance. It was Newton's theory of gravitation that first assigned a cause for gravity by interpreting it as action at
a distance, proceeding from masses. Newton's theory is probably the greatest stride ever made in the effort towards the causal nexus of natural
phenomena. And yet this theory evoked a lively sense of discomfort among Newton's contemporaries, because it seemed to be in conflict with the
principle springing from the rest of experience, that there can be reciprocal action only through contact, and not through immediate action at a
distance.
It is only with reluctance that man's desire for knowledge endures a dualism of this kind. How was unity to be preserved in his comprehension of the
forces of nature? Either by trying to look upon contact forces as being themselves distant forces which admittedly are observable only at a very small
distance and this was the road which Newton's followers, who were entirely under the spell of his doctrine, mostly preferred to take; or by assuming
that the Newtonian action at a distance is only apparently immediate action at a distance, but in truth is conveyed by a medium permeating space,
whaether by movements or by elastic deformation of this medium. Thus the endeavor toward a unified view of the nature of forces leads to the
hypothesis of an aether. This hypothesis, to be sure, did not at first bring with it any advance in the theory of gravitation or in physics generally,
so that it became customary to treat Newton's law of force as an axiom not further reducible. But the aether hypothesis was bound always to play some
part in physical science, even if at first only a latent part.
When in the first half of the nineteenth century the far-reaching similarity was revealed which subsists between the properties of light and those of
elastic waves in ponderable bodies, the aether hypothesis found fresh support. 1t appeared beyond question that light must be interpreted as a
vibratory process in an elastic, inert medium filling up universal space. It also seemed to be a necessary consequence of the fact that light is
capable of polarization that this medium, the aether, must be of the nature of a solid body, because transverse waves are not possible in a fluid, but
only in a solid. Thus the physicists were bound to arrive at the theory of the ``quasi-rigid'' luminiferous aether, the parts of which can carry out
no movements relatively to one another except the small movements of deformation which correspond to light-waves.
This theory also called the theory of the stationary luminiferous aether moreover found a strong support in an experiment which is also of fundamental
importance in the special theory of relativity, the experiment of Fizeau, from which one was obliged to infer that the luminiferous aether does not
take part in the movements of bodies. The phenomenon of aberration also favored the theory of the quasi-rigid aether.
The development of the theory of electricity along the path opened up by Maxwell and Lorentz gave the development of our ideas concerning the aether
quite a peculiar and unexpected turn. For Maxwell himself the aether indeed still had properties which were purely mechanical, although of a much more
complicated kind than the mechanical properties of tangible solid bodies. But neither Maxwell nor his followers succeeded in elaborating a mechanical
model for the aether which might furnish a satisfactory mechanical interpretation of Maxwell's laws of the electro-magnetic field. The laws were
clear and simple, the mechanical interpretations clumsy and contradictory. Almost imperceptibly the theoretical physicists adapted themselves to a
situation which, from the standpoint of their mechanical program, was very depressing. They were particularly influenced by the electro-dynamical
investigations of Heinrich Hertz. For whereas they previously had required of a conclusive theory that it should content itself with the fundamental
concepts which belong exclusively to mechanics (e.g. densities, velocities, deformations, stresses) they gradually accustomed themselves to admitting
electric and magnetic force as fundamental concepts side by side with those of mechanics, without requiring a mechanical interpretation for them. Thus
the purely mechanical view of nature was gradually abandoned. But this change led to a fundamental dualism which in the long-run was insupportable. A
way of escape was now sought in the reverse direction, by reducing the principles of mechanics to those of electricity, and this especially as
confidence in the strict validity of the equations of Newton's mechanics was shaken by the experiments with b-rays and rapid cathode rays.
This dualism still confronts us in unextenuated form in the theory of Hertz, where matter appears not only as the bearer of velocities, kinetic
energy, and mechanical pressures, but also as the bearer of electromagnetic fields. Since such fields also occur in vacuo i.e. in free aether the
aether also appears as bearer of electromagnetic fields. The aether appears indistinguishable in its functions from ordinary matter. Within matter it
takes part in the motion of matter and in empty space it has everywhere a velocity; so that the aether has a definitely assigned velocity throughout
the whole of space. There is no fundamental difference between Hertz's aether and ponderable matter (which in part subsists in the aether).
The Hertz theory suffered not only from the defect of ascribing to matter and aether, on the one hand mechanical states, and on the other hand
electrical states, which do not stand in any conceivable relation to each other; it was also at variance with the result of Fizeau's important
experiment on the velocity of the propagation of light in moving fluids, and with other established experimental results.
Such was the state of things when H. A. Lorentz entered upon the scene. He brought theory into harmony with experience by means of a wonderful
simplification of theoretical principles. He achieved this, the most important advance in the theory of electricity since Maxwell, by taking from
aether its mechanical, and from matter its electromagnetic qualities. As in empty space, so too in the interior of material bodies, the aether, and
not matter viewed atomistically, was exclusively the seat of electromagnetic fields. According to Lorentz the elementary particles of matter alone are
capable of carrying out movements; their electromagnetic activity is entirely confined to the carrying of electric charges. Thus Lorentz succeeded in
reducing all electromagnetic happenings to Maxwell's equations for free space.
As to the mechanical nature of the Lorentzian aether, it may be said of it, in a somewhat playful spirit, that immobility is the only mechanical
property of which it has not been deprived by H. A. Lorentz. 1t may be added that the whole change in the conception of the aether which the special
theory of relativity brought about, consisted in taking away from the aether its last mechanical quality, namely, its immobility. How this is to be
understood will forthwith be expounded.
The space-time theory and the kinematics of the special theory of relativity were modeled on the Maxwell-Lorentz theory of the electromagnetic field.
This theory therefore satisfies the conditions of the special theory of relativity, but when viewed from the latter it acquires a novel aspect. For if
K be a system of coordinates relatively to which the Lorentzian aether is at rest, the Maxwell-Lorentz equations are valid primarily with reference to
K. But by the special theory of relativity the same equations without any change of meaning also hold in relation to any new system of coordinates K'
which is moving in uniform translation relatively to K. Now comes the anxious question: Why must I in the theory distinguish the K system above all
K' systems, which are physically equivalent to it in all respects, by assuming that the aether is at rest relatively to the K system? For the
theoretician such an asymmetry in the theoretical structure, with no corresponding asymmetry in the system of experience, is intolerable. If we assume
the aether to be at rest relatively to K, but in motion relatively to K', the physical equivalence of K and K' seems to me from the logical
standpoint, not indeed downright incorrect, but nevertheless unacceptable.
The next position which it was possible to take up in face of this state of things appeared to be the following. The aether does not exist at all. The
electromagnetic fields are not states of a medium, and are not bound down to any bearer, but they are independent realities which are not reducible to
anything else, exactly like the atoms of ponderable matter. This conception suggests itself the more readily as, according to Lorentz's theory,
electromagnetic radiation, like ponderable matter, brings impulse and energy with it, and as, according to the special theory of relativity, both
matter and radiation are but special forms of distributed energy, ponderable mass losing its isolation and appearing as a special form of energy.
More careful reflection teaches us, however, that the special theory of relativity does not compel us to deny aether. We may assume the existence of
an aether,; only we must give up ascribing a definite state of motion to it, i.e. we must by abstraction take from it the last mechanical
characteristic which Lorentz had still left it. We shall see later that this point of view, the conceivability of which shall at once endeavor to make
more intelligible by a somewhat halting comparison, is justified by the results of the general theory of relativity.
Think of waves on the surface of water. Here we can describe two entirely different things. Either we may observe how the undulatory surface forming
the boundary between water and air alters in the course of time; or else with the help of small floats, for instance we can observe how the position
of the separate particles of water alters in the course of time. If the existence of such floats for tracking the motion of the particles of a fluid
were a fundamental impossibility in physics if, in fact, nothing else whatever were observable than the shape of the space occupied by the water as it
varies in time, we should have no ground for the assumption that water consists of movable particles. But all the same we could characterize it as a
medium.
We have something like this in the electromagnetic field. For we may picture the field to ourselves as consisting of lines of force. If we wish to
interpret these lines of force to ourselves as something material in the ordinary sense, we are tempted to interpret the dynamic processes as motions
of these lines of force, such that each separate line of force is tracked through the course of time. It is well known, however, that this way of
regarding the electromagnetic field leads to contradictions.
Generalizing we must say this: There may be supposed to be extended physical objects to which the idea of motion cannot be applied. They may not be
thought of as consisting of particles which allow themselves to be separately tracked through time. In Minkowski's idiom this is expressed as
follows: Not every extended conformation in the four-dimensional world can be regarded as composed of worldthreads. The special theory of relativity
forbids us to assume the aether to consist of particles observable through time, but the hypothesis of aether in itself in conflict with the special
theory of relativity. Only we must be on our guard against ascribing a state of motion to the aether.
Certainly, from the standpoint of the special theory of relativity, the aether hypothesis appears at first to be an empty hypothesis. 1n the equations
of the electromagnetic field there occur, in addition to the densities of the electric charge, only the intensities of the field. The career of
electromagnetic processes in vacuo appears to be completely determined by these equations, uninfluenced by other physical quantities. The
electromagnetic fields appear as ultimate, irreducible realities, and at first it seems superfluous to postulate a homogeneous, isotropic
aether-medium, and to envisage electromagnetic fields as states of this medium.
But on the other hand there is a weighty argument to be adduced in favor of the aether hypothesis. To deny the aether is ultimately to assume that
empty space has no physical qualities whatever. The fundamental facts of mechanics do not harmonize with this view. For the mechanical behavior of a
corporeal system hovering freely in empty space depends not only on relative positions (distances) and relative velocities, but also on its state of
rotation, which physically may be taken as a characteristic not appertaining to the system in itself. In order to be able to look upon the rotation of
the system, at least formally, as something real, Newton objectifies space. Since he classes his absolute space togaether with real things, for him
rotation relative to an absolute space is also something real. Newton might no less well have called his absolute space ``aether''; what is
essential is merely that besides observable objects, another thing, which is not perceptible, must be looked upon as real, to enable acceleration or
rotation to be looked upon as something real.
It is true that Mach tried to avoid having to accept as real something which is not observable by endeavoring to substitute in mechanics a mean
acceleration with reference to the totality of the masses in the universe in place of an acceleration with reference to absolute space. But inertial
resistance opposed to relative acceleration of distant masses presupposes action at a distance; and as the modern physicist does not believe that he
may accept this action at a distance, he comes back once more, if he follows Mach, to the aether, which has to serve as medium for the effects of
inertia. But this conception of the aether to which we are led by Mach's way of thinking differs essentially from the aether as conceived by Newton,
by Fresnel, and by Lorentz. Mach's aether not only conditions the behavior of inert masses, but is also conditioned in its state by them.
Mach's idea finds its full development in the aether of the general theory of relativity. According to this theory the metrical qualities of the
continuum of space-time differ in the environment of different points of space-time, and are partly conditioned by the matter existing outside of the
territory under consideration. This space-time variability of the reciprocal relations of the standards of space and time, or, perhaps, the
recognition of the fact that ``empty space'' in its physical relation is neither homogeneous nor isotropic, compelling us to describe its state by
ten functions (the gravitation potentials g), has, I think, finally disposed of the view that space is physically empty. But therewith the conception
of the aether has again acquired an intelligible content, although this content differs widely from that of the aether of the mechanical undulatory
theory of light. The aether of the general theory of relativity is a medium which is itself devoid of all mechanical and kinematical qualities, but
helps to determine mechanical (and electromagnetic) events.
What is fundamentally new in the aether of the general theory of relativity as opposed to the aether of Lorentz consists in this, that the state of
the former is at every place determined by connections with the matter and the state of the aether in neighboring places, which are amenable to law in
the form of differential equations,; whereas the state of the Lorentzian aether in the absence of electromagnetic fields is conditioned by nothing
outside itself, and is everywhere the same. The aether of the general theory of relativity is transmuted conceptually into the aether of Lorentz if we
substitute constants for the functions of space which describe the former, disregarding the causes which condition its state. Thus we may also say, I
think, that the aether of the general theory of relativity is the outcome of the Lorentzian aether, through relativation.
As to the part which the new aether is to play in the physics of the future we are not yet clear. We know that it determines the metrical relations in
the space-time continuum, e.g. the configurative possibilities of solid bodies as well as the gravitational fields; but we do not know whaether it has
an essential share in the structure of the electrical elementary particles constituting matter. Nor do we know whaether it is only in the proximity of
ponderable masses that its structure differs essentially from that of the Lorentzian aether; whaether the geometry of spaces of cosmic extent is
approximately Euclidean. But we can assert by reason of the relativistic equations of gravitation that there must be a departure from Euclidean
relations, with spaces of cosmic order of magnitude, if there exists a positive mean density, no matter how small, of the matter in the universe. In
this case the universe must of necessity be spatially unbounded and of finite magnitude, its magnitude being determined by the value of that mean
density.
If we consider the gravitational field and the electromagnetic field from the standpoint of the aether hypothesis, we find a remarkable difference
between the two. There can be no space nor any part of space without gravitational potentials; for these confer upon space its metrical qualities,
without which it cannot be imagined at all. The existence of the gravitational field is inseparably bound up with the existence of space. On the other
hand a part of space may very well be imagined without an electromagnetic field; thus in contrast with the gravitational field, the electromagnetic
field seems to be only secondarily linked to the aether, the formal nature of the electromagnetic field being as yet in no way determined by that of
gravitational aether. From the present state of theory it looks as if the electromagnetic field, as opposed to the gravitational field, rests upon an
entirely new formal motif, as though nature might just as well have endowed the gravitational aether with fields of quite another type, for example,
with fields of a scalar potential, instead of fields of the electromagnetic type.
Since according to our present conceptions the elementary particles of matter are also, in their essence, nothing else than condensations of the
electromagnetic field, our present view of the universe presents two realities which are completely separated from each other conceptually, although
connected causally, namely, gravitational aether and electromagnetic field, or as they might also be called space and matter.
Of course it would be a great advance if we could succeed in comprehending the gravitational field and the electromagnetic field togaether as one
unified conformation. Then for the first time the epoch of theoretical physics founded by Faraday and Maxwell would reach a satisfactory conclusion.
The contrast between aether and matter would fade away, and, through the general theory of relativity, the whole of physics would become a complete
system of thought, like geometry, kinematics, and the theory of gravitation. An exceedingly ingenious attempt in this direction has been made by the
mathematician H. Weyl,; but I do not believe that his theory will hold its ground in relation to reality. Further, in contemplating the immediate
future of theoretical physics we ought not unconditionally to reject the possibility that the facts comprised in the quantum theory may set bounds to
the field theory beyond which it cannot pass.
Recapitulating, we may say that according to the general theory of relativity space is endowed with physical qualities; in this sense, therefore,
there exists an aether. According to the general theory of relativity space without aether is unthinkable; for in such space there not only would be
no propagation of light, but also no possibility of existence for standards of space and time (measuring-rods and clocks), nor therefore any
space-time intervals in the physical sense. But this aether may not be thought of as endowed with the quality characteristic of ponderable media,
as consisting of parts which may be tracked through time. The idea of motion may not be applied to it.
--Albert Einstein
The problem is, dh, your scalar weapons theory are derived from the assumption that this aether is in fact endowed with qualities characteristic of
ponderable media. That is why the concept of scalar weapons is foolish