canonical structure of tetrad bigravity sergei alexandrov laboratoire charles coulomb montpellier...
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Canonical structure of Tetrad Bigravity
Sergei Alexandrov
Laboratoire Charles CoulombMontpellier
S.A. arXiv:1308.6586
1. Introduction: massive and bimetric gravitty in the metric and tetrad formulations
2. Canonical structure of GR in the Hilbert-Palatini formulation
3. Canonical structure of tetrad bigravity
4. Conclusions
Plan of the talk
Massive gravity
The idea: to give to the graviton a non-vanishing mass
At the linearized level ― Fierz-Pauli theory
(In vacuum) is transverse and traceless and carries 5 d.o.f.
breaks gauge invariance
At the non-linear level ― Einstein-Hilbert action plus a potential
an extra fixed metric• has the flat space as a solution
• reduces to for and Diffeomorphism symmetry is broken
Bimetric gravity
Two dynamical metrics coupled by a non-derivative interaction term
Diffeomorphism symmetry:
• diagonal ― preserved by the mass term
• off-diagonal ― broken by the mass term
The theory describes one massless and one massive gravitons
In fact, not only…
Boulware-Deser ghost
Massive gravity describes a theory with 6 d.o.f.Boulware,Deser ’72 :
The trace becomes dynamical and describes a scalar ghost ― the Hamiltonian is unbounded from below
In the canonical language: The lapse and shift do not enter linearly and
therefore are not Lagrange multipliers anymore
(In the FP Lagrangian generates a second class constraintremoving one d.o.f.)
Is it possible to find an interaction potential which is free from the
ghost pathology?
Ghost-free potentials
The ghost is absent because the lapse appears again as Lagrange multiplier and generates a (second class) constraint
Symmetric polynomials:
deRham,Gabadadze,Tolley ’10 : There is a three-parameter family of ghost-free potentials
Hassan,Rosen ’11
How to deal with the awkward square root structure?
Tetrad reformulation
The idea: to reformulate the theory using tetrads
Hinterbichler,Rosen ’12
The important property:
• The symmetricity constraint follows from e.o.m. • The model should be absent from the BD ghost
The mass term in the tetrad formalism (in 4d):
=Symmetricity condition
=
antisymmetricityof the wedge product
linear in linear in
The model
The Hilbert-Palatini action:
The mass term:
Cartan equations Bimetric gravity in the tetrad formulation
Hilbert-Palatini action
3+1 decomposition:
the phase space the primary constraints
Non-covariant description
Solve constraints explicitly
primary constraints
secondary constraints
The kinetic term:
where
Covariant description
The symplectic structure is given by Dirac brackets
Don’t solve constraints explicitly
secondary constraints
We also need
Tetrad bigravity: phase spaceThe second class constraints of
the two HP actions are not affected by the mass term
does not depend on
Covariant description
Phase space:
+ s.c. constraints
Symplectic structure:
Dirac brackets
Non-covariant description
Phase space:
Symplectic structure:
canonical Poisson brackets
+ constraints
affected by the mass term
Tetrad bigravity: primary constraints
Decomposition of the mass term:
where
not expressible in terms of
The total set of primary constraints:
diagonal sector off-diagonal sector
weakly commute with all primary constraints
It remains to analyze the stability of
Tetrad bigravity: symmetricity condition
Stabilization of :
Crucial property:
mixed metric
where
secondary constraint
condition on Lagrange multipliers Symmetricity condition
Tetrad and metric formulations are indeed equivalent on-shell
Tetrad bigravity: constraint algebra
secondary constraintfixing Lagrange multipliers
are second class
Tetrad bigravity: secondary constraint
where
One can compute explicitly
Stability condition for
fixes or are second class
secondary constraint stability condition for
Summary of the phase space structure
+ 2×(9+9+3+3) = 48
• Phase space (in non-covariant description):
• Second class constraints:
– (6+3+3+1+1) = –14
• First class constraints:
– 2×(6+3+1) = –20
The BD ghost is absent!
2 ― massless graviton5 ― massive graviton
14 dim. phase space spaceor
7 degrees of freedom
Open problems• Superluminality, instabilities, tachyonic modes…
• Partially massless theory
• Degenerate sectors
What happens with the theory for configurations where some of the invertibility properties fail?Detailed study of the stability condition for
Additional gauge symmetry reducing the number of d.o.f. of the massive graviton from 5 to 4.Is it possible?