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.

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The constraints define a constraint surface in the original phase space. Ben, euh, il vient de la cosmologie aussi, donc je sais pas exactement… David: This makes the AQG semiclassical analysis superior over that of LQG, and suantique has fravitation made in establishing it has the correct semiclassical limit and providing contact with familiar low energy physics. Theory of quantum gravity, merging quantum mechanics and general relativity. Recent research by Chris Duston and Matilde Marcolli introduces topology change via topspin networks.

Podcast Science — Faut-il manger moins de produits animaux? Hamiltonian constraint of LQG.

Consequently, not just matter, but space itself, prefers an atomic structure. In the Hamiltonian formulation of ordinary classical mechanics the Poisson bracket is an important concept.

Specifically, the dynamics of the theory are encoded in the Hamiltonian constraintbut there is no candidate Hamiltonian. InRovelli and Smolin showed that the quantum operators of the theory associated to area and volume have bouccles discrete spectrum.

It is possible to extend mainstream LQG formalism to higher-dimensional supergravity, general relativity with supersymmetry and Kaluza—Klein extra dimensions should experimental evidence establish their existence. HolonomyWilson loopand Knot invariant. One can employ the idea of the delta function to impose the condition that the Hamiltonian constraint should vanish.


The sum over rerouting are chosen as such to make the form of the intertwiner invariant under Gauss gauge transformations.

The Chiral Structure of Loop Quantum Gravity

Before we move on to the constraints of LQG, lets us consider certain cases. We consider the action of the constraints on arbitrary phase space functions. This means that one cannot just solve the spatial diffeomorphism constraint and then the Gravitayion constraint.

This theory is thus described as background dependent. In fact a series of recent papers have been published attempting just this. LQG differs from string theory in that it is formulated in 3 and 4 dimensions and without supersymmetry or Kaluza-Klein extra dimensions, while the latter requires both to be true.

According to Einstein, gravity is not a force — it is a property of spacetime itself. Given that the anti-symmetric summation is taken over in the formula for the volume we would need at least intersections with three non- coplanar lines. Cette condition sur l’absence de torsion est en fait une contrainte secondaire de l’analyse canonique.

Il a, il a, … depuis quelques jours. The theory gives a physical picture of spacetime where space and time are granular and discrete directly because of quantization just like photons in the quantum theory of electromagnetism and the discrete energy levels of atoms.

Just as different phases are physically different, so are different sectors of a quantum field theory. Views Read Edit View history.

As Carlo Rovelli puts it: Bosonic string theory M-theory Supergravity Superstring theory. From these relationships one can form a notion of matter being located with respect to the gravitational field, or vice versa.

Bonsoir tous le monde Johan: The Guass law and the spatial diffeomorphism constraints are the same. Let us go back to the connection representation. Actually it turns out that one needs at least four-valent vertices for the volume operator to be non-vanishing. Because of its significance this is known as the master equation.



Canonical general relativity was originally formulated in terms of metric variables, but there seemed to be insurmountable mathematical difficulties in promoting the constraints to quantum operators because of their highly non-linear dependence on the canonical variables. A very important aspect of the Hamiltonian operator is that it only acts at vertices a consequence of this is that Thiemann’s Hamiltonian operator, like Ashtekar’s operator, annihilates non-intersecting loops except now it is not just formal and has rigorous mathematical meaning.

Je sais pas comment se porte les ventes, est ce que tu. Salut tous le monde Johan: The quantization of the volume proceeds the same way as with the area. Oui, bien sur, bien sur.

Loop quantum gravity – Wikipedia

There is the consistent discretizations approach. The Gauss law has vanishing Poisson bracket with the Hamiltonian constraint. General covariancebackground independenceand diffeomorphism.

Difficulties with the Barrett—Crane vertex”. The Consistent Discretizations approach to LQG, [46] [47] is an application of the master constraint program to construct the physical Hilbert space of the canonical theory. Ca fait parti de ces qiantique qui sont ces avocats?