We show that consistent nonlinear partially massless models cannot be obtained starting from “f-g” massive gravity, with “f” the embedding de Sitter space. The obstruction, which is also the source of f-g acausality, is the very same fifth constraint that removes the notorious sixth ghost excitation. Here, however, it blocks extension of the gauge invariance (appearing for mass to de Sitter cosmological constant tunings) that removed the helicity-zero mode at linear level. Separately, our methods allow us to almost complete the proof that all f-g models are acausal
We exhibit novel effects (absent in GR) of sources in massive gravity. First, we show that removing ...
We explore the space of static solutions of the recently discovered three-dimensional "new massive g...
Motivated by the apparent dependence of string σ models on the sum of spacetime metric and antisymme...
We show that consistent nonlinear partially massless models cannot be obtained starting from “f-g” m...
We show, by analyzing its characteristics, that the ghost-free, 5 degree of freedom, Wess-Zumino mas...
Massive gravity is an old idea: trading geometry for mass. Much effort has been expended on establis...
The parameter space of the de Rham-Gabadadze-Tolley massive gravity ought to be constrained essentia...
We show that higher spin systems specific to cosmological spaces are subject to the same problems as...
The mass of the graviton can be generated using a Brout-Englert-Higgs mechanism with four scalar fie...
We perform a covariant constraint analysis of massive gravity valid for its entire parameter space, ...
We explore spherically symmetric stationary solutions, generated by ``stars'' with regular interiors...
Abstract. Non-linear partially massless (PM) gravity, if it exists, is a theory of massive gravity i...
AbstractIn this Letter we present a very simple and independent argument for the absence of the Boul...
In three dimensions, there are two distinct mass-generating mechanisms for gauge fields: adding the ...
We use conformal, but ghostful, Weyl gravity to study its ghost-free, second derivative, partially m...
We exhibit novel effects (absent in GR) of sources in massive gravity. First, we show that removing ...
We explore the space of static solutions of the recently discovered three-dimensional "new massive g...
Motivated by the apparent dependence of string σ models on the sum of spacetime metric and antisymme...
We show that consistent nonlinear partially massless models cannot be obtained starting from “f-g” m...
We show, by analyzing its characteristics, that the ghost-free, 5 degree of freedom, Wess-Zumino mas...
Massive gravity is an old idea: trading geometry for mass. Much effort has been expended on establis...
The parameter space of the de Rham-Gabadadze-Tolley massive gravity ought to be constrained essentia...
We show that higher spin systems specific to cosmological spaces are subject to the same problems as...
The mass of the graviton can be generated using a Brout-Englert-Higgs mechanism with four scalar fie...
We perform a covariant constraint analysis of massive gravity valid for its entire parameter space, ...
We explore spherically symmetric stationary solutions, generated by ``stars'' with regular interiors...
Abstract. Non-linear partially massless (PM) gravity, if it exists, is a theory of massive gravity i...
AbstractIn this Letter we present a very simple and independent argument for the absence of the Boul...
In three dimensions, there are two distinct mass-generating mechanisms for gauge fields: adding the ...
We use conformal, but ghostful, Weyl gravity to study its ghost-free, second derivative, partially m...
We exhibit novel effects (absent in GR) of sources in massive gravity. First, we show that removing ...
We explore the space of static solutions of the recently discovered three-dimensional "new massive g...
Motivated by the apparent dependence of string σ models on the sum of spacetime metric and antisymme...