Abstract

Neutron stars are sensitive laboratories for testing general relativity, especially when considering deviations where velocities are relativistic and gravitational fields are strong. One such deviation is described by dynamical, Chern-Simons modified gravity, where the Einstein-Hilbert action is modified through the addition of the gravitational parity-violating Pontryagin density coupled to a field. This four-dimensional effective theory arises naturally both in perturbative and non-perturbative string theory, loop quantum gravity, and generic effective field theory expansions. We calculate here Chern-Simons modifications to the properties and gravitational fields of slowly spinning neutron stars. We find that the Chern-Simons correction affects only the gravitomagnetic sector of the metric to leading order, thus introducing modifications to the moment of inertia but not to the mass-radius relation. We show that an observational determination of the moment of inertia to an accuracy of 10%, as is expected from near-future observations of the double pulsar, will place a constraint on the Chern-Simons coupling constant of \xi^{1/4} < 5 km, which is at least three-orders of magnitude stronger than the previous strongest bound.

Highlights

  • Even though it has been almost a century since its original proposal, general relativity (GR) remains only marginally tested in the strong, dynamical regime, where velocities are relativistic and gravitational fields are strong

  • With the imminent discovery of gravitational waves, new frameworks have been proposed that will allow us to search for GR deviations with gravitational waves in the strong, dynamical regime

  • GR tests with neutron stars appear a priori to be not as clean as solar system or binary pulsar tests

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Summary

INTRODUCTION

Even though it has been almost a century since its original proposal, general relativity (GR) remains only marginally tested in the strong, dynamical regime, where velocities are relativistic and gravitational fields are strong. The second group corrects the action by introducing higher-order curvature terms, which, by construction, do not modify the leading-order predictions of GR in the weak-field These theories do modify the strong-field regime of gravity, where neutron star observations can place stringent constraints. We concentrate here on tests of dynamical CS modified gravity, which is currently only weakly constrained by binary pulsar observations [45] This four-dimensional theory adds a certain contraction of two Riemann tensors and the Levi-Civita tensor to the Einstein-Hilbert action, coupled to a dynamical scalar field. We calculate the CS-modified gravitational field inside neutron stars and relate this to possible observables that would allow us to constrain the theory.

Basic Equations
Perturbative Constraints in Dynamical CS Modified Gravity
Zeroth-Order Field Equations
Zeroth-Order Scalar-Field Evolution Equation
First-Order Field Equations
First-Order Scalar Field Evolution Equation
Second-Order Field Equations
Boundary Conditions
27 M 2 10 r2 θext
General Relativistic Solutions
First-Order CS Scalar Field Solution
CONNECTION TO OBSERVABLES
Findings
CONCLUSIONS

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