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#### Manifestly Gauge-Invariant General Relativistic Perturbation Theory: I. Foundations

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0711.0115v1.pdf

(Preprint), 793KB

CQG_27_055005.pdf

(Any fulltext), 674KB

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##### Citation

Giesel, K., Hofmann, S., Thiemann, T., & Winkler, O. (2010). Manifestly Gauge-Invariant
General Relativistic Perturbation Theory: I. Foundations.* Classical and quantum gravity,*
*27*(5): 055005. doi:10.1088/0264-9381/27/5/055005.

Cite as: https://hdl.handle.net/11858/00-001M-0000-0013-5FE0-D

##### Abstract

Linear cosmological perturbation theory is pivotal to a theoretical understanding of current cosmological experimental data provided e.g. by cosmic microwave anisotropy probes. A key issue in that theory is to extract the gauge invariant degrees of freedom which allow unambiguous comparison between theory and experiment. When one goes beyond first (linear) order, the task of writing the Einstein equations expanded to n'th order in terms of quantities that are gauge invariant up to terms of higher orders becomes highly non-trivial and cumbersome. This fact has prevented progress for instance on the issue of the stability of linear perturbation theory and is a subject of current debate in the literature. In this series of papers we circumvent these difficulties by passing to a manifestly gauge invariant framework. In other words, we only perturb gauge invariant, i.e. measurable quantities, rather than gauge variant ones. Thus, gauge invariance is preserved non perturbatively while we construct the perturbation theory for the equations of motion for the gauge invariant observables to all orders. In this first paper we develop the general framework which is based on a seminal paper due to Brown and Kuchar as well as the realtional formalism due to Rovelli. In the second, companion, paper we apply our general theory to FRW cosmologies and derive the deviations from the standard treatment in linear order. As it turns out, these deviations are negligible in the late universe, thus our theory is in agreement with the standard treatment. However, the real strength of our formalism is that it admits a straightforward and unambiguous, gauge invariant generalisation to higher orders. This will also allow us to settle the stability issue in a future publication.