Journals / Turkish Journal of Physics / 2019 / Cilt: 43 - Sayı: 5

Second-order gauge-invariant perturbation theory and conserved charges in cosmological Einstein gravity

Pages
493–501
Publication Date
2022-11-04
DOI
—
🏛️Bibliographic metadata and full text access for this article are provided via DergiPark.
DergiPark Record ↗
✨

AI Summary & Key Takeaways

AI Insight
⚡ TL;DR(Too Long; Didn't Read)

This method depends on the assumption that the first-order metric perturbation can be decomposed intogauge-variant and gauge-invariant parts and the gauge-variant parts do not contribute to physical quantities.

📌 3 Key Takeaways

🎯
Objective & Hypothesis:Recently a new approach in constructing the conserved charges in cosmological Einstein gravity was given.In this new formulation, instead of using the explicit form of the field equations, a covariantly conserved rank-four tensorwas used.
📊
Key Findings & Data:In the resulting charge expression, instead of the first derivative of the metric perturbation, the linearizedRiemann tensor appears along with the derivative of the background Killing vector fields.
💡
Conclusion & Impact:This method depends on the assumption that the first-order metric perturbation can be decomposed intogauge-variant and gauge-invariant parts and the gauge-variant parts do not contribute to physical quantities.
🔬Design:Research Article
📍Scope:Comprehensive Sample
⚙️Variables:Domain Parameters

Abstract

Recently a new approach in constructing the conserved charges in cosmological Einstein gravity was given.In this new formulation, instead of using the explicit form of the field equations, a covariantly conserved rank-four tensorwas used. In the resulting charge expression, instead of the first derivative of the metric perturbation, the linearizedRiemann tensor appears along with the derivative of the background Killing vector fields. Here we give a detailed analysisof the first-order and the second-order perturbation theory in a gauge-invariant form in cosmological Einstein gravity.The linearized Einstein tensor is gauge-invariant at the first order but it is not so at the second order, which complicatesthe discussion. This method depends on the assumption that the first-order metric perturbation can be decomposed intogauge-variant and gauge-invariant parts and the gauge-variant parts do not contribute to physical quantities.

🔖

Cite This Article

ALTAŞ, E. (2022). Second-order gauge-invariant perturbation theory and conserved charges in cosmological Einstein gravity. Turkish Journal of Physics, Cilt: 43 - Sayı: 5, 493–501. https://ajindex.com/articles/614136

📄 Full Text PDF Viewer

📄

PDF görüntüleyici hazırlanıyor...

References (12)

  1. Abbott LF, Deser S. Stability of gravity with a cosmological constant. Nuclear Physics B 1982
  2. doi: 10.1016/0550-3213(82)90049-9 [2] Deser S, Tekin B. Energy in generic higher curvature gravity theories. Physical Review D 2002
  3. 084009. doi: 10.1103/PhysRevD.67.084009 [3] Arnowitt R, Deser S, Misner CW. Canonical variables for general relativity. Physical Review 1960
  4. doi: 10.1103/PhysRev.117.1595 [4] Taub AH. Variational principles in general relativity. In: Cattaneo C (editor). Relativistic Fluid Dynamics. Berlin, Germany: Springer, 1970, pp. 205-300. doi: 10.1007/978-3-642-11099-3_3 [5] Deser S, Brill D. Instability of closed spaces in general relativity. Communications in Mathematical Physics 1973
  5. doi: 10.1007/BF01645610 [6] Deser S, Choquet-Bruhat Y. On the stability of flat space. Annals of Physics 1973
  6. doi: 10.1016/0003- 4916(73)90484-3 [7] Fischer AE, Marsden JE. Linearization stability of the Einstein equations. Bulletin of the American Mathematical Society 1973
  7. doi: 10.1090/S0002-9904-1973-13299-9 [8] Fischer AE, Marsden JE, Moncrief V. The structure of the space of solutions of Einstein’s equations. I. One Killing field. Annales de l’I.H.P. Physique th￿orique 1980
  8. Marsden JE. Lectures on Geometric Methods in Mathematical Physics. CBMS-NSF Regional Conference Series in Applied Mathematics. Philadelphia, PA, USA: SIAM, 1981. [10] Moncrief V. Spacetime symmetries and linearization stability of the Einstein equations I. Journal of Mathematical Physics 1975
  9. doi: 10.1063/1.522572 [11] Arms JM, Marsden JE. The absence of Killing fields is necessary for linearization stability of Einstein’s equations. Indiana University Mathematics Journal 1979
  10. doi: 10.1512/iumj.1979.28.28008 [12] Choquet-Bruhat Y. General Relativity and the Einstein Equations. Oxford, UK: Oxford University Press, 2009. [13] Girbau J, Bruna L. Stability by Linearization of Einstein’s Field Equation. Berlin, Germany: Springer, 2010. [14] Altas E, Tekin B. Linearization instability for generic gravity in AdS spacetime. Physical Review D 2018
  11. 024028. doi: 10.1103/PhysRevD.97.024028 [15] Altaş E. Linearization instability in gravity theories. PhD, Middle East Technical University, Ankara, Turkey, 2018. arXiv: 1808.04722 [hep-th]. [16] Altas E, Tekin B. Linearization instability of chiral gravity. Physical Review D 2018
  12. 124068. doi: 10.1103/Phys- RevD.97.124068 [17