DEVELOPPEMENT MATHEMATIQUE ET APPLICATIONS DE LA GRAVITATION QUANTIQUE A BOUCLES. Thesis (PDF Available) · January. Des chercheurs de l’Institut Périmètre travaillent activement sur un certain nombre d’approches de ce problème, dont la gravitation quantique à boucles, les . 19 avr. A quantum theory of gravitation aims at describing the gravitational La gravité quantique à boucles étant toujours une théorie en cours de.

Author: Zulkitaur Tygoramar
Country: Syria
Language: English (Spanish)
Genre: Software
Published (Last): 4 November 2012
Pages: 359
PDF File Size: 20.89 Mb
ePub File Size: 15.82 Mb
ISBN: 386-4-42097-605-2
Downloads: 19800
Price: Free* [*Free Regsitration Required]
Uploader: Voodoor

The Hamiltonian comes with a continuum action adapted to a fixed simplicial discretisation of spacetime. Devenez un soutien sur Patreon! With the use of Poisson brackets, the Hamilton’s equations can be rewritten as. LQG offers a geometric explanation of quatique finiteness of the entropy and of the proportionality of the area of the horizon.


This is the second result. International Journal of Modern Physics D. Jorge Pullin and Jerzy Lewandowski understood that the intersections of the loops are essential for the consistency of the theory, and the theory should be formulated in terms of intersecting loops, or graphs. It appears, then, that one can violate the second law of thermodynamics by dropping an object with nonzero entropy into a black hole. As such it can be applied at the spatially diffeomorphism-invariant level.

Solving the Hamiltonian constraint should tell us how quantum states voucles in ‘time’ from an initial spin network state to a final bucles network state.

Older attempts at this calculation had difficulties. Les physiciens nous donnent raison. Correspondence principle and classical limit. In contrast, loop quantum gravity, like general relativity, is manifestly background independent, eliminating the background required in string theory. There are however severe difficulties with this particular approach, for example the Hamiltonian operator is not self-adjoint, in fact it is not even a normal operator i.

Contrary to this, LQG is based only on quantum theory and general relativity and its scope is limited to understanding the quantum aspects of the gravitational interaction. Progress has been made in calculating background independent scattering amplitudes this way with the use of spin foams.


We now move on to demonstrate an important aspect of the quantum constraints. This is our final result.

Loop quantum gravity – Wikipedia

It turns out there are alternative routes to formulating the path integral, however their connection to the Hamiltonian formalism is less clear. The reason for this is that the smearing functions are not functions of the canonical variables and so the spatial diffeomorphism does not generate diffeomorphims on them. La nuit, tous les arbres sont-ils gris? Any collection of non-intersecting Wilson loops satisfy Ashtekar’s quantum Hamiltonian constraint. It was in particular the inability to have good control over the space of solutions to the Gauss’ law and spatial diffeomorphism constraints that led Rovelli and Smolin to consider a new representation — the loop representation in gauge theories and quantum gravity.

The action of the spatial diffeomorphism on the Gauss law is. Its greatest consequence sees the evolution of the universe continuing beyond the Big Bang called the Big Bounce. These come about from the fact that Wilson loops are based on matrices the holonomy and these matrices satisfy identities. Because of its significance this is known as the master equation. LQG grravitation related research programs. As Wilson loops form a basis we can formally expand any Gauss gauge invariant function bouclfs.

Classical theories of gravitation Quantum gravity Theory of everything. From these relationships one can form a notion of matter being located with respect to the gravitational field, or vice versa. Here we just mention issues that arises with the Hamiltonian constraint. The no hair conjecture of general relativity states that a black hole is characterized only by its massits chargeand its angular momentum ; hence, it has no entropy. This means it gragitation unproven that LQG’s description of spacetime at the Planck scale has the right continuum limit described by general relativity with possible quantum corrections.


HolonomyWilson loopand Knot invariant. Proponents of string theory will often point to the fact that, among other things, it demonstrably reproduces the established theories of general relativity and quantum field theory in the appropriate limits, which Loop Bouclss Gravity has struggled to do.

We consider the action of the constraints on arbitrary phase space functions. Thus Wilson loops are gauge invariant. This is a simpler theory than general relativity, it has no local degrees of freedom and as such depends only on topological qantique of the fields.

The principle was formulated by Niels Bohr in[24] though he had previously made use of it as early as in developing his model of the atom. Inclusion of distortion and rotation”. This defines the loop representation. In other words, it says that for large orbits and for large energiesquantum calculations must agree with classical calculations.


There are a number of particular difficulties in establishing the semiclassical limit:. The same idea is true for the other constraints. We need the quantque of a holonomy.

The problem was that although Loop quantum gravity predicted that the entropy of a black hole is proportional to the area of the event horizon, the result depended on a crucial free parameter in the theory, the above-mentioned Immirzi parameter. Ben, euh, il vient de la cosmologie aussi, donc je sais pas exactement…. Non, enfin moi, non.

Here, we develop the generalisation to SL 2,Cthat is we use twistors to parametrise the phase space of self-dual holonomy-flux variables. The Guass law and the spatial diffeomorphism constraints are the same. Je te laisse reprendre la main, euh… David:

Related Posts