- Access by Xinjiang University
CMB polarization power spectra contributions from a network of cosmic strings
Phys. Rev. D 76, 043005 – Published 24 August, 2007
DOI: https://doi.org/10.1103/PhysRevD.76.043005
Abstract
We present the first calculation of the possible (local) cosmic string contribution to the cosmic microwave background polarization spectra from simulations of a string network (rather than a stochastic collection of unconnected string segments). We use field-theory simulations of the Abelian Higgs model to represent local U(1) strings, including their radiative decay and microphysics. Relative to previous estimates, our calculations show a shift in power to larger angular scales, making the chance of a future cosmic string detection from the B-mode polarization slightly greater. We explore a future ground-based polarization detector, taking the CLOVER project as our example. In the null hypothesis (that cosmic strings make a zero contribution) we find that CLOVER should limit the string tension to (where is the gravitational constant), above which it is likely that a detection would be possible.
Article Text
References (75)
- A. Vilenkin and E. P. S. Shellard, Cosmic Strings and Other Topological Defects (Cambridge University Press, Cambridge, U.K., 1994).
- M. B. Hindmarsh and T. W. B. Kibble, Rep. Prog. Phys. 58, 477 (1995).
- R. Jeannerot, J. Rocher, and M. Sakellariadou, Phys. Rev. D 68, 103514 (2003).
- E. J. Copeland, R. C. Myers, and J. Polchinski, J. High Energy Phys. 06 (2004) 013.
- S. Sarangi and S. H. H. Tye, Phys. Lett. B 536, 185 (2002).
- N. T. Jones, H. Stoica, and S. H. H. Tye, Phys. Lett. B 563, 6 (2003).
- G. Dvali and A. Vilenkin, J. Cosmol. Astropart. Phys. 03 (2004) 010.
- N. Bevis, M. Hindmarsh, M. Kunz, and J. Urrestilla, arXiv:astro-ph/0702223.
- M. Wyman, L. Pogosian, and I. Wasserman, Phys. Rev. D 72, 023513 (2005).
- R. A. Battye, B. Garbrecht, and A. Moss, J. Cosmol. Astropart. Phys. 09 (2006) 007.
- M. Kamionkowski, A. Kosowsky, and A. Stebbins, Phys. Rev. D 55, 7368 (1997).
- U. Seljak and A. Slosar, Phys. Rev. D 74, 063523 (2006).
- N. Bevis, M. Hindmarsh, M. Kunz, and J. Urrestilla, Phys. Rev. D 75, 065015 (2007).
- T. W. B. Kibble, Nucl. Phys. B252, 227 (1985).
- A. Albrecht and N. Turok, Phys. Rev. D 40, 973 (1989).
- D. P. Bennett and F. R. Bouchet, Phys. Rev. D 41, 2408 (1990).
- B. Allen and E. P. S. Shellard, Phys. Rev. Lett. 64, 119 (1990).
- G. Vincent, N. D. Antunes, and M. Hindmarsh, Phys. Rev. Lett. 80, 2277 (1998).
- J. N. Moore, E. P. S. Shellard, and C. J. A. P. Martins, Phys. Rev. D 65, 023503 (2002).
- C. J. A. P. Martins and E. P. S. Shellard, Phys. Rev. D 73, 043515 (2006).
- C. Ringeval, M. Sakellariadou, and F. Bouchet, J. Cosmol. Astropart. Phys. 02 (2007) 023.
- G. R. Vincent, M. Hindmarsh, and M. Sakellariadou, Phys. Rev. D 56, 637 (1997).
- R. A. Battye J. Wellerand , Phys. Rev. D 61, 043501 (2000).
- A. Albrecht, R. A. Battye, and J. Robinson, Phys. Rev. Lett. 79, 4736 (1997).
- C. Contaldi, M. Hindmarsh, and J. Magueijo, Phys. Rev. Lett. 82, 679 (1999).
- K. D. Olum and J. J. Blanco-Pillado, Phys. Rev. D 60, 023503 (1999).
Beyond , a string network could not be formed and studied in the scaling regime for a sufficient range in for the required data to be extracted from the simulations.
- U.K. National Cosmology Supercomputer: SGI Altix 3700 containing Intel Itanium II CPUs, URL www.damtp.cam.ac.uk/cosmos/.
- U.-L. Pen, U. Seljak, and N. Turok, Phys. Rev. Lett. 79, 1611 (1997).
- R. Durrer, M. Kunz, and A. Melchiorri, Phys. Rep. 364, 1 (2002).
In fact remains important, setting the overall normalization of and is used in the conversion between and .
- N. Turok, Phys. Rev. D 54, R3686 (1996).
- M. Doran, J. Cosmol. Astropart. Phys. 10 (2005) 011.
- W. Hu and M. J. White, Phys. Rev. D 56, 596 (1997).
- A. Lewis, A. Challinor, and A. Lasenby, Astrophys. J. 538, 473 (2000).
- C.-l. Kuo et al. (ACBAR Collaboration), Astrophys. J. 600, 32 (2004).
- W. C. Jones et al. (BOOMERANG Collaboration), Astrophys. J. 647, 823 (2006).
- A. C. S. Readhead et al. (CBI Collaboration), Science, 306, 836 (2004).
- K. Grainge et al., Mon. Not. R. Astron. Soc. 341, L23 (2003).
- G. Hinshaw et al., arXiv:astro-ph/0603451 [Astrophys. J. (to be published)].
Parameters obtained from a fit to CMB data are: , , , , and , with zero running of and spatial flatness assumed.
- W. L. Freedman et al., Astrophys. J. 553, 47 (2001).
- D. Kirkman, D. Tytler, N. Suzuki, J. M. O’Meara, and D. Lubin, Astrophys. J. Suppl. Ser. 149, 1 (2003).
- R. A. Knop et al. (Supernova Cosmology Project), Astrophys. J. 598, 102 (2003).
- S. M. Leach, A. R. Liddle, J. Martin, and D. J. Schwarz, Phys. Rev. D 66, 023515 (2002).
- The primordial scalar mode can give rise to very small vector and tensor contributions in nonlinear perturbation theory and so create small BB spectrum contributions [47], but they will not be relevant unless cosmic strings have a very small contribution indeed, and the cosmic shear signal is successfully cleaned.
- N. Bartolo, S. Matarrese, S. Mollerach, and A. Riotto, arXiv:astro-ph/0703386.
In principle cosmic strings and the matter perturbations that they seed contribute to the lensing of the inflationary power spectra, and the string spectra are also lensed. As the string perturbations are subdominant we neglect the latter contributions here, but this is an approximation that should be tested.
- N. Bevis, M. Hindmarsh, and M. Kunz, Phys. Rev. D 70, 043508 (2004).
- D. P. Bennett, Phys. Rev. D 33, 872 (1986).
- C. J. A. P. Martins and E. P. S. Shellard, Phys. Rev. D 54, 2535 (1996).
- L. Pogosian, I. Wasserman, and M. Wyman, arXiv:astro-ph/0604141.
- R. Durrer, M. Kunz, and A. Melchiorri, Phys. Rev. D 59, 123005 (1999).
- U. Seljak, U.-L. Pen, and N. Turok, Phys. Rev. Lett. 79, 1615 (1997).
- E. M. Leitch et al. (DASI Collaboration), Astrophys. J. 624, 10 (2005).
- T. E. Montroy et al. (BOOMERANG Collaboration), Astrophys. J. 647, 813 (2006).
- J. L. Sievers et al. (CBI Collaboration), arXiv:astro-ph/0509203 [Astrophys. J. (to be published)].
- P. Oxley et al. (EBEX Collaboration), Proc. SPIE Int. Soc. Opt. Eng. 5543, 320 (2004).
- A. C. Taylor (CLOVER Collaboration), New Astron. Rev. 50, 993 (2006).
- W. H. Kinney, Phys. Rev. D 58, 123506 (1998).
- L. Knox, Phys. Rev. D 52, 4307 (1995).
- W. Hu and T. Okamoto, Astrophys. J. 574, 566 (2002).
- C. M. Hirata and U. Seljak, Phys. Rev. D 67, 043001 (2003).
- C. M. Hirata and U. Seljak, Phys. Rev. D 68, 083002 (2003).
- A. Achucarro and T. Vachaspati, Phys. Rep. 327, 347 (2000).
- M. Hindmarsh, Phys. Rev. Lett. 68, 1263 (1992).
- M. Hindmarsh, Nucl. Phys. B392, 461 (1993).
- J. Urrestilla, A. Achucarro, and A. C. Davis, Phys. Rev. Lett. 92, 251302 (2004).
- K. Dasgupta, J. P. Hsu, R. Kallosh, A. Linde, and M. Zagermann, J. High Energy Phys. 08 (2004) 030.
- A. Achucarro, P. Salmi, and J. Urrestilla, Phys. Rev. D 75, 121703(R) (2007).
- J. Urrestilla, N. Bevis, M. Hindmarsh, M. Kunz, and A. Liddle (unpublished).
- P. M. Saffin, J. High Energy Phys. 09 (2005) 011.
- J. Urrestilla and A. Vilenkin (unpublished).
- M. Hindmarsh and P. M. Saffin, J. High Energy Phys. 08 (2006) 066.
- K. Kajantie, M. Karjalainen, M. Laine, J. Peisa, and A. Rajantie, Phys. Lett. B 428, 334 (1998).