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.
|Published (Last):||18 February 2008|
|PDF File Size:||7.4 Mb|
|ePub File Size:||17.53 Mb|
|Price:||Free* [*Free Regsitration Required]|
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. Squaring the constraint is dangerous as it could lead to worsened ultraviolet behaviour of the corresponding operator boufles hence the master constraint programme must be approached with due bouclrs.
Les plantes dorment la nuit: Combining this identity with the simple identity. On part de physique des particules? Just as different phases are physically different, so are different sectors of a quantum field theory. The kinematic inner product structure is easily employed to provide the inner product structure after solving this first constraint; the new inner product is simply.
Catégorie:Gravitation quantique à boucles – Wikiwand
Since the action is a polynomial in the spinors, canonical quantisation is straightforward. Et donc il y a eu beaucoup de modifications depuis 30, euh 40 ans maintenant. This is not guaranteed because of a feature of quantum field quabtique which is that they have different sectors, these are analogous to the different phases that come about in the thermodynamical limit of statistical systems.
The reason is that the rescaled Hamiltonian constraint is a scalar density of weight two while it can be shown that only scalar densities of grzvitation one have a chance to result in a well defined operator.
GRAVITATION QUANTIQUE | Perimeter Institute
The master constraint see below does not suffer from these problems and as such offers a way of connecting the canonical theory to the path integral formulation.
As mentioned above the holonomy tells quntique how to propagate test spin half particles. English translation in Bohrpp. The corresponding phase space has a non-linear structure. Quantiquf like photons as well as changes in the spacetime geometry gravitons are both described as excitations on the string worldsheet.
Gravitatioj one quantizes the theory, it is difficult to ensure that one recovers real general relativity as opposed to complex general relativity. Loop quantum gravity LQG is a theory of quantum gravitymerging quantum mechanics and general relativitymaking it a possible candidate for a theory of everything.
The Chiral Structure of Loop Quantum Gravity
Classical and Quantum Gravity. According to Gravitatlon, gravity is not a force — it is a property of spacetime itself. Many of the technical problems in canonical quantum gravity revolve around the constraints.
The most fundamental representation being the Pauli matrices. Carlo Rovelli and Lee Smolin defined a nonperturbative and background-independent quantum theory of gravity in terms of these loop solutions.
Retranscription: la gravité quantique à boucles
To recover the real theory, one has to impose what are known as the “reality conditions. The use of Wilson loops explicitly solves the Gauss gauge constraint. The classical limit or correspondence limit is the ability of a physical theory to approximate or “recover” classical mechanics when considered over special values of its parameters.
The easiest geometric quantity is the area. This opens up a way of trying to directly link canonical LQG to a path integral description. In contrast, gravitons play a key role in string theory where they are among the first massless level of excitations of a superstring. Also, Pullin and Gambini provide a framework to connect the path integral and canonical approaches to quantum gravity. 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.
This is our final result. The quantization of the volume proceeds the same way as with the area. One approach to solving the Hamiltonian constraint starts with what is called the Dirac delta function. The essential idea is that coordinates are only artifices used in describing nature, and hence should play no role in the formulation of fundamental physical laws.
It appears, then, that one can violate the second law of thermodynamics by dropping an object with nonzero entropy into a black hole. The image of space given in LQG is similar.
List of unsolved problems in physics. For example, string theory also addresses unificationthe understanding of all known forces and particles as manifestations of a single entity, by postulating extra dimensions and so-far unobserved additional particles and symmetries. Black hole thermodynamics is the area of study that seeks to reconcile the laws of thermodynamics with the existence of black hole event horizons.
Formulating general relativity with triads instead of metrics was not new. Because of their resemblance to soap foams and the way they are labeled John Baez gave these ‘quantum space-times’ the name ‘spin foams’.
Enfin, si, un tout petit peu avant. The feature that distinguishes such different theories is the Hamiltonian constraint which is the only one that depends on the Lagrangian of the classical theory. This is what Einstein discovered: This page was last edited on 18 Decemberat The first attempt at this was the famous Barrett—Crane model. Let us move to LQG, additional complications will arise from that one cannot define an operator for the quantum spatial diffeomorphism constraint as the infinitesimal generator of finite diffeomorphism transformations and the fact the constraint algebra is not a Lie algebra due to the bracket between two Hamiltonian constraints.
That is, it is a sum over infinitesimal spatial diffeomorphisms constraints where the coefficients of proportionality are not constants but have non-trivial phase space dependence.
These identities can be combined with each other into further identities of increasing complexity adding more loops. These SU 2 variables are quatique derived from the Holst action, which contains the Barbero–Immirzi parameter as an additional coupling constant. LQG offers a geometric explanation of the finiteness of the entropy and of the proportionality of the area of the horizon.