Glossary (designed by E.T. Lefèvre)

Gravitational Lenses

Effect in which a visible or invisible mass acts as a lens to "focalize" the light coming from a background source. (see bending of light) On the image above, arcs are images distorted and demultiplied, by the galaxy cluster, of more distant objects.




Bending of light rays
When in classical mecanics one considers light as a material object and not only as a wave, one can show that (the trajectories followed by a body in the gravity field of a much more massive body do not depend on its mass) a light ray passing at a distance r of a body of mass M undergoes a deviation of angle

.

In general relativity, light follows the curvature of Space-Time induced by the mass M and undergoes a deviation of angle

.

This effect has been verified by Eddington in 1919 during an eclipse. The measurement of the deviation angle predicted by GR constituted the first experimental verification of Einstein's theory.




Planck length
Length obtained by combining the fundamental constants (where h is Planck's constant), c (vacuum speed of light) and G (gravitation or Newton constant) to obtain a quantity having the dimension of a length.

This microscopic length constitutes in ScR an unexceedable, unreachable (it is an asymptot, an horizon) and invariant under dilation, scale (or resolution). Even if it is only very small, it has all the physical properties of an infinitely small!

It is the smallest scale of Nature. The fact that it is not null has enormous repercussions on physics, like the finiteness of the speed of light.

The Planck mass MP and Planck Energy associated to it, EP = MP c2, are also computed from the 3 fundamental constants G, h and c: MP= (hbar c / G)^(1/2)




Cosmological length
length linked to the cosmological constant by:

Second length invariable under dilation that appears in ScR. It is the counterpart of the Planck length at large scale.

Is is the largest scale of Nature




Fractal Curve
Let's consider a continuous but non-differentiable curve (function). In general these two limits are even not defined, i.e. one cannot define the slope of the curve in any point.

An example of topological dimension 1 is the curve:

5th iteration from the generator

BE CAREFUL!: a (too) common error is to define a fractal curve or object as an object possessing the property to keep the same appearance under successive zooms. It applies only to self-similar fractals like the preceeding curve!

The word fractal refers, in ScR, to the appearance of a priori new structures along successive zooms toward small or large scales, which leads to a divergence for resolutions tending towards zero (towards Planck's scale in special ScR) and the infinity (cosmological scale in SScR).




Space-Time

A physical definition of Space-Time could take an entire book! However, giving a mathematical definition is relatively more simple.

In relativity and quantum mechanics, an event involving 1 body is characterized by 4 and only 4 coordinates (x,y,z,t). One puts apart properties like charge, spin, etc. and it does not mean that knowing only one (x,y,z,t) is sufficient to determine the evolution of a system but that the necessary quantities only depend on x, y, z, and t.

Space-Time constitutes the set of all possible (x,y,z,t) quadruplets and their transformations

Relativity's Space-Time is continuous and curved (the case were it is flat being not excluded a priori) and differentiable. This kind of Space cannot account for the quantum properties of matter.

Quantum Mechanics' Space-Time is in principle flat, minkovskian and differentiable. The contradiction with relativity as well as other considerations leads to attempts at including another kind of Space-Time in quantum mechanics, that have been up to now unfruitful..

In Scale Relativity, a criticism of measurement theory in physics, in particular of the role played by the resolutions, (c.f. the importance of the analysis of how we make measures of length and instant in the premisses of Einstein's theory) led L. Nottale to give up the (implicit) hypothesis of the differentiability of Space-Time, which implies its fractal and curved nature. The fractal Space-Time, explicitely dependent on resolutions, can be reduced to the definition of a "Space-Time-Zoom" with 5 dimensions (x,y,z,t,D). It is the fractal dimension, became a variable, which plays the role of a 5th dimension for scale laws (just as relativistic motion laws are implemented by the interpretation of time as a 4th dimension).

The concept of fractal space-time has also been independently introduced by Garnet Ord as a geometric analogue of relativistic quantum mechanics.



Chaos time
A chaotic system can be characterized by the behaviour of the separation between 2 of its trajectories. They are in general solutions of a system of deterministic differential equations describing the evolution of the system. When the system is chaotic, 2 solutions corresponding to 2 infinitely close initial conditions exponentially diverge one from another. One speaks of an extreme sensibility to initial conditions.

The deviation follows an exponential law:

is called the chaos time of the system. The inverse of the chaos time is the Lyapunov exponent. If, having measured as precisely as we want (but not enough to distinguish between the 2 initial conditions) the system's parameters (initial conditions) at a time t0, we try to determine its state after a time interval much greater than , we realize that the deviation between the 2 solutions is now so big that one cannot say anything on the state in which the system really is: knowing that there are, in fact, an infinity of possible initial conditions between the two that we have considered, the system can lie in an infinity of states very different one from another. One has a sort of predictibility horizon which, like the one we are familiar with (due to the roundness of the Earth), is not absolute: short term prediction (before the horizon) remains entirely possible!

Remarks:

Covariant derivative


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