Next-to-next-to-leading order post-Newtonian spin(1)-spin(2) Hamiltonian for self-gravitating binaries
Corresponding Author
J. Hartung
Theoretisch–Physikalisches Institut, Friedrich–Schiller–Universität, Max-Wien-Platz 1, 07743 Jena, Germany
Phone: +49 3641 947 106, Fax: +49 3641 947 102
Theoretisch–Physikalisches Institut, Friedrich–Schiller–Universität, Max-Wien-Platz 1, 07743 Jena, GermanySearch for more papers by this authorJ. Steinhoff
Theoretisch–Physikalisches Institut, Friedrich–Schiller–Universität, Max-Wien-Platz 1, 07743 Jena, Germany
Centro Multidisciplinar de Astrofísica (CENTRA), Departamento de Física, Instituto Superior Técnico (IST), Universidade Técnica de Lisboa, Avenida Rovisco Pais 1, 1049-001 Lisboa, Portugal
Search for more papers by this authorCorresponding Author
J. Hartung
Theoretisch–Physikalisches Institut, Friedrich–Schiller–Universität, Max-Wien-Platz 1, 07743 Jena, Germany
Phone: +49 3641 947 106, Fax: +49 3641 947 102
Theoretisch–Physikalisches Institut, Friedrich–Schiller–Universität, Max-Wien-Platz 1, 07743 Jena, GermanySearch for more papers by this authorJ. Steinhoff
Theoretisch–Physikalisches Institut, Friedrich–Schiller–Universität, Max-Wien-Platz 1, 07743 Jena, Germany
Centro Multidisciplinar de Astrofísica (CENTRA), Departamento de Física, Instituto Superior Técnico (IST), Universidade Técnica de Lisboa, Avenida Rovisco Pais 1, 1049-001 Lisboa, Portugal
Search for more papers by this authorAbstract
We present the next-to-next-to-leading order post-Newtonian (PN) spin(1)-spin(2) Hamiltonian for two self-gravitating spinning compact objects. If both objects are rapidly rotating, then the corresponding interaction is comparable in strength to a 4PN effect. The Hamiltonian is checked via the global Poincaré algebra with the center-of-mass vector uniquely determined by an ansatz.
References
- [1]J. Hartung and J. Steinhoff, Ann. Phys. (Berlin) 523, 783–790 (2011).
- [2]P.D. D'Eath, Phys. Rev. D 12, 2183–2199 (1975).
- [3]B.M. Barker and R.F. O'Connell, Phys. Rev. D 12, 329–335 (1975).
- [4]B.M. Barker and R.F. O'Connell, Gen. Relativ. Gravit. 11, 149–175 (1979).
- [5]J. Steinhoff, G. Schäfer, and S. Hergt, Phys. Rev. D 77, 104018 (2008); J. Steinhoff, S. Hergt, and G. Schäfer, Phys. Rev. D 77, 081501(R) (2008).
- [6]J. Hartung and J. Steinhoff, Phys. Rev. D 83, 044008 (2011).
- [7]R.L. Arnowitt, S. Deser, and C.W. Misner, The Dynamics of General Relativity, in: Gravitation: An Introduction to Current Research, edited by L. Witten, (John Wiley, New York, 1962) pp. 227–265; republication: Gen. Relativ. Gravit. 40, 1997–2027 (2008).
10.1007/s10714-008-0661-1 Google Scholar
- [8]J. Steinhoff and G. Schäfer, Europhys. Lett. 87, 50004 (2009).
- [9]J. Steinhoff, Ann. Phys. (Berlin) 523, 296–353 (2011).
- [10]R.A. Porto and I.Z. Rothstein, Phys. Rev. D 78, 044012 (2008); 81, 029904(E) (2010).
- [11]M. Levi, Phys. Rev. D 82, 064029 (2010).
- [12]R.A. Porto and I.Z. Rothstein, Phys. Rev. Lett. 97, 021101 (2006).
- [13]A. Buonanno and T. Damour, Phys. Rev. D 59, 084006 (1999).
- [14]A. Buonanno and T. Damour, Phys. Rev. D 62, 064015 (2000).
- [15]T. Damour, B.R. Iyer, and A. Nagar, Phys. Rev. D 79, 064004 (2009).
- [16]T. Damour and A. Nagar, Phys. Rev. D 79, 081503(R) (2009).
- [17]A. Buonanno et al., Phys. Rev. D 79, 124028 (2009).
- [18]Y. Pan et al., Phys. Rev. D 81, 084041 (2010).
- [19]T. Damour, Phys. Rev. D 64, 124013 (2001).
- [20]T. Damour, P. Jaranowski, and G. Schäfer, Phys. Rev. D 78, 024009 (2008).
- [21]E. Barausse and A. Buonanno, Phys. Rev. D 81, 084024 (2010).
- [22]A. Nagar, arXiv:1106.4349 [gr-qc] (2011).
- [23]E. Barausse and A. Buonanno, arXiv:1107.2904 [gr-qc] (2011).
- [24]E. Barausse, É. Racine, and A. Buonanno, Phys. Rev. D 80, 104025 (2009).
- [25]M. Levi, arXiv:1107.4322 [gr-qc] (2011).
- [26]S. Wolfram, The Mathematica Book, 5th edition (Wolfram Media, Champaign, IL, 2003).
- [27]J.M. Martín-García, xAct: Efficient Tensor Computer Algebra, URL: http://www.xact.es/.
- [28]J.M. Martín-García, Comput. Phys. Commun. 179, 597–603 (2008).
- [29]D. Brizuela, J.M. Martín-García, and G.A. Mena Marugán, Gen. Relativ. Gravit. 41, 2415–2431 (2009).
- [30]T. Damour, P. Jaranowski, and G. Schäfer, Phys. Lett. B 513, 147–155 (2001).
- [31]T. Damour, P. Jaranowski, and G. Schäfer, Dimensional Regularization of the Gravitational Interaction of Point Masses in the ADM Formalism, in: Proceedings of the 11th Marcel Grossmann Meeting on General Relativity, edited by H. Kleinert, R. T. Jantzen, and R. Ruffini, (World Scientific, Singapore, 2008) p. 2490, arXiv:0804.2386 [gr-qc].
- [32]T. Damour, P. Jaranowski, and G. Schäfer, Phys. Rev. D 77, 064032 (2008).
- [33]T. Damour, P. Jaranowski, and G. Schäfer, Phys. Rev. D 62, 021501(R) (2000).
- [34]J. Steinhoff and H. Wang, Phys. Rev. D 81, 024022 (2010).