New first order Lagrangian for General Relativity

In summary, the new action principle described in this paper leads to a simpler Lagrangian for gravitons than the metric one, and can be used to compute graviton scattering amplitudes.
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http://arxiv.org/abs/1503.08640

New first order Lagrangian for General Relativity

Yannick Herfray, Kirill Krasnov
(Submitted on 30 Mar 2015)
We describe a new BF-type first-order in derivatives Lagrangian for General Relativity. The Lagrangian depends on a connection field as well as a Lie-algebra valued two-form field, with no other fields present. There are two free parameters, which translate into the cosmological constant and the coefficient in front of a topological term. When one of the parameters is set to zero, the theory becomes topological. When the other parameter is zero, the theory reduces to the (anti-) self-dual gravity. Thus, our new Lagrangian interpolates between the topological and anti-self-dual gravities. It also interprets GR as the (anti-) self-dual gravity with an extra quadratic in the auxiliary two-form field term added to the Lagrangian, precisely paralleling the situation in Yang-Mills theory.

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"Our work is also of relevance for the spin foam approach to quantum gravity [15]. The spin foam description of the topological theory, whose Lagrangian is (2) with α = 0, is considered to be understood. Thus, if it was possible to give a spin foam description of the ASD gravity (2) with λ = 0, then it would perhaps be also possible to combine the two and obtain full GR. Given that the theory with α = 0 is believed to give rise to the quantum group SUq(2), our description thus points in the direction of full GR being about ”q-deformed instantons”, whatever that may be."
 
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This is the master thesis of the co author Yannick Herfray:

Study of a family of modifications of General Relativity, supervised by Kiril Krasnov:

http://www.ens-lyon.fr/DSM/SDMsite/M2/stages_M2/Herfray2014.pdf

Now he is a PhD leaded by Kiril Kranikov:

http://www.digt.org/group-members/
 
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Other papers by Krasnov which led directly to this results are :

http://arxiv.org/pdf/1103.4498.pdf
New Action Principle for General Relativity
General Relativity can be reformulated as a diffeomorphism invariant SU(2) gauge theory. A new action principle for this ”pure connection” formulation of GR is describedhttp://arxiv.org/pdf/1101.4788.pdf
Gravity as a diffeomorphism invariant gauge theory

A general diffeomorphism invariant SU(2) gauge theory is a gravity theory with two propagating polarizations of the graviton. We develop this description of gravity, in particular for future applications to the perturbative quantization. Thus, the linearized theory, gauge symmetries, gauge fixing are discussed in detail, and the propagator is obtained. The propagator takes a simple form of that of Yang-Mills theory with an additional projector on diffeomorphism equivalence classes of connections inserted. In our approach the gravitational perturbation theory takes a rather unusual form in that the Planck length is no longer fundamental.

http://arxiv.org/pdf/1205.7045.pdf
Pure Connection Formalism for Gravity: Linearized Theory

Abstract We give a description of gravitons in terms of an SL(2, C) connection field. The gauge-theoretic Lagrangian for gravitons is simpler than the metric one, in particular because the Lagrangian only depends on 8 components of the field per spacetime point as compared to 10 in the Einstein-Hilbert case. Particular care is paid to the treatment of the reality conditions that guarantee that one is dealing with a system with a hermitian Hamiltonian. We give general arguments explaining why the connection cannot be taken to be real, and then describe a reality condition that relates the hermitian conjugate of the connection to its (second) derivative. This is quite analogous to the treatment of fermions where one describes them by a second-order in derivatives Klein-Gordon Lagrangian, with an additional first-order reality condition (Dirac equation) imposed. We find many other parallels with fermions, e.g. the fact that the action of parity on the connection is related to the hermitian conjugation. Our main result is the mode decomposition of the connection field, which is to be used in forthcoming works for computations of graviton scattering amplitudes.
 

1. What is a first order Lagrangian in General Relativity?

A first order Lagrangian in General Relativity is a mathematical function that describes the dynamics of a system in terms of its kinetic and potential energies. In the context of General Relativity, it is used to describe the motion of particles and fields in curved spacetime.

2. Why is a new first order Lagrangian needed for General Relativity?

The standard first order Lagrangian for General Relativity, known as the Hilbert action, has some limitations and is not suitable for certain applications. A new first order Lagrangian has been proposed to overcome these limitations and provide a more comprehensive description of the dynamics of General Relativity.

3. How does the new first order Lagrangian differ from the Hilbert action?

The new first order Lagrangian takes into account additional terms that were not included in the Hilbert action, such as the cosmological constant and higher order curvature terms. It also introduces new variables that allow for a more complete description of the gravitational field.

4. What are the implications of the new first order Lagrangian for our understanding of General Relativity?

The new first order Lagrangian has the potential to provide a more accurate and comprehensive understanding of the dynamics of General Relativity. It may also lead to new insights and predictions that were not possible with the Hilbert action.

5. Has the new first order Lagrangian been tested or confirmed by experiments?

At this point, the new first order Lagrangian is still a theoretical proposal and has not been directly tested or confirmed by experiments. However, it is based on well-established principles and has been extensively studied and debated by physicists. Further research and experimentation will be needed to fully evaluate its validity and implications.

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