Dark Coupling and Gauge Invariance

We study a coupled dark energy-dark matter model in which the energy-momentum exchange is proportional to the Hubble expansion rate. The inclusion of its perturbation is required by gauge invariance. We derive the linear perturbation equations for the gauge invariant energy density contrast and velocity of the coupled fluids, and we determine the initial conditions. The latter turn out to be adiabatic for dark energy, when assuming adiabatic initial conditions for all the standard fluids. We perform a full Monte Carlo Markov Chain likelihood analysis of the model, using WMAP 7-year data.

[1]  The Cosmon model for an asymptotically vanishing time dependent cosmological 'constant' , 1994, hep-th/9408025.

[2]  Isocurvature fluctuations in tracker quintessence models , 2001, astro-ph/0108081.

[3]  J. P. Huchra,et al.  Final Results from the Hubble Space Telescope Key Project to Measure the Hubble Constant , 1998, astro-ph/9801080.

[4]  Bin Wang,et al.  Stability of the curvature perturbation in dark sectors' mutual interacting models , 2008, 0807.3471.

[5]  M. B. Gavela,et al.  Dark coupling , 2009, 0901.1611.

[6]  The theory of CMB anisotropies , 2001, astro-ph/0109522.

[7]  Hume A. Feldman,et al.  Theory of cosmological perturbations , 1992 .

[8]  R. Maartens,et al.  Dynamics of interacting dark energy , 2008, 0812.1827.

[9]  C. Wetterich,et al.  Gauge-invariant initial conditions and early time perturbations in quintessence universes , 2003, astro-ph/0304212.

[10]  R. Nichol,et al.  Cosmological constraints from the SDSS luminous red galaxies , 2006, astro-ph/0608632.

[11]  F. Atrio-Barandela,et al.  Dynamics of interacting quintessence models: Observational constraints , 2007, 0706.3860.

[12]  H. Kodama,et al.  Cosmological Perturbation Theory , 1984 .

[13]  R. Maartens,et al.  The growth of structure in interacting dark energy models , 2009, 0905.0492.

[14]  Constraints on the redshift dependence of the dark energy potential , 2004, astro-ph/0412269.

[15]  D. Pavón,et al.  Interacting models of soft coincidence , 2006, astro-ph/0606520.

[16]  Gibbons,et al.  Dark matter, time-varying G, and a dilaton field. , 1990, Physical review letters.

[17]  C. Baccigalupi,et al.  Early time perturbations behavior in scalar field cosmologies , 1998, astro-ph/9811156.

[18]  Roy Maartens,et al.  Large-scale instability in interacting dark energy and dark matter fluids , 2008 .

[19]  S. Carroll Quintessence and the rest of the world , 1999 .

[20]  Coupled Quintessence , 1999, astro-ph/9908023.

[21]  Interacting Quintessence , 2001, astro-ph/0105479.

[22]  Edward J. Wollack,et al.  SEVEN-YEAR WILKINSON MICROWAVE ANISOTROPY PROBE (WMAP) OBSERVATIONS: POWER SPECTRA AND WMAP-DERIVED PARAMETERS , 2010, 1001.4635.

[23]  Edward J. Wollack,et al.  FIVE-YEAR WILKINSON MICROWAVE ANISOTROPY PROBE OBSERVATIONS: COSMOLOGICAL INTERPRETATION , 2008, 0803.0547.

[24]  Roy Maartens,et al.  Adiabatic initial conditions for perturbations in interacting dark energy models , 2009, 0907.4981.

[25]  Roy Maartens,et al.  Velocities as a probe of dark sector interactions , 2009, 0907.2126.

[26]  IMPROVING COSMOLOGICAL CONSTRAINTS WITH NEW AND COMBINED SUPERNOVA DATASETS , 2008 .

[27]  Sean M. Carroll QUINTESSENCE AND THE REST OF THE WORLD : SUPPRESSING LONG-RANGE INTERACTIONS , 1998 .

[28]  A. Berera,et al.  On the large-scale instability in interacting dark energy and dark matter fluids , 2009, 0901.3272.

[29]  A. Liddle,et al.  Evolution of large-scale perturbations in quintessence models , 2002, astro-ph/0208562.

[30]  Edmund Bertschinger,et al.  Cosmological Perturbation Theory in the Synchronous and Conformal Newtonian Gauges , 1995 .

[31]  Superacceleration as the signature of a dark sector interaction , 2005, astro-ph/0510628.

[32]  Interacting Chaplygin gas , 2005, astro-ph/0509895.

[33]  A. Lewis,et al.  Cosmological parameters from CMB and other data: A Monte Carlo approach , 2002, astro-ph/0205436.

[34]  Damour,et al.  Nucleosynthesis constraints on an extended Jordan-Brans-Dicke theory. , 1991, Physical review. D, Particles and fields.

[35]  M. Trodden,et al.  The adiabatic instability on cosmology's dark side , 2007, 0709.1124.

[36]  A. Lewis,et al.  Efficient computation of CMB anisotropies in closed FRW models , 1999, astro-ph/9911177.

[37]  Roy Maartens,et al.  Quintessence with quadratic coupling to dark matter , 2009, 0911.3089.

[38]  P. Peebles,et al.  Interacting Dark Matter and Dark Energy , 2003, astro-ph/0307316.

[39]  Roy Maartens,et al.  Observational constraints on an interacting dark energy model , 2009, 0907.4987.

[40]  Topological Defects in Gravitational Lensing Shear Fields , 2009, 0906.0124.

[41]  E. Majerotto,et al.  Large-scale instability in interacting dark energy and dark matter fluids , 2008, 0804.0232.

[42]  J. Bardeen,et al.  Gauge Invariant Cosmological Perturbations , 1980 .