Abstract

We show that intrinsic (not lensing-induced) correlations between galaxy shapes offer a new probe of primordial non-Gaussianity and inflationary physics which is complementary to galaxy number counts. Specifically, intrinsic alignment correlations are sensitive to an anisotropic squeezed limit bispectrum of the primordial perturbations. Such a feature arises in solid inflation, as well as more broadly in the presence of light higher spin fields during inflation (as pointed out recently by Arkani-Hamed and Maldacena). We present a derivation of the all-sky two-point correlations of intrinsic shapes and number counts in the presence of non-Gaussianity with general angular dependence, and show that a quadrupolar (spin-2) anisotropy leads to the analog in galaxy shapes of the well-known scale-dependent bias induced in number counts by isotropic (spin-0) non-Gaussianity. Moreover, in the presence of non-zero anisotropic non-Gaussianity, the quadrupole of galaxy shapes becomes sensitive to far superhorizon modes. These effects come about because long-wavelength modes induce a local anisotropy in the initial power spectrum, with which galaxies will correlate. We forecast that future imaging surveys could provide constraints on the amplitude of anisotropic non-Gaussianity that are comparable to those from the Cosmic Microwave Background (CMB). These are complementary as they probe different physical scales. The constraints, however, depend on the sensitivity of galaxy shapes to the initial conditions which we only roughly estimate from observed tidal alignments.

Highlights

  • We show that intrinsic correlations between galaxy shapes offer a new probe of primordial non-Gaussianity and inflationary physics which is complementary to galaxy number counts

  • Alignments are typically regarded as a contaminant to ‘cosmic shear’, and they can contribute significantly to the correlation of galaxy shapes with the weak lensing of the Cosmic Microwave Background (CMB) [15, 16]

  • We have shown that the intrinsic alignment of red galaxies will become an interesting probe of inflationary physics in the future

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Summary

Large-scale non-Gaussianity

When computing two-point correlations of large-scale structure in the large-scale limit, the leading relevant non-Gaussian statistic is the squeezed-limit potential bispectrum Bφ(k1, k2, kL), where kL ≪ k1, k2. We will only consider one of those terms, which in the squeezed limit can be written in general as. With “beyond-squeezed limit” terms suppressed by (kL/kS)2 These are negligible when considering large-scale correlations, and we will not consider them here. Standard local non-Gaussianity corresponds to L = 0 and A0 = 4fNloLc. We are interested in the two lowest order contributions: a monopole A0, and a quadrupole A2, which corresponds to the anisotropic shape generated, for example, by solid inflation [34] or spin-2 particles [26].

Intrinsic alignments and non-Gaussianity
Observed shape and number count correlations
Projection
Intrinsic shape correlations
Signatures of non-Gaussianity
Lensing shear
Modeling the red galaxy population and alignments
Fisher matrix analysis
Constraining non-Gaussianity with clustering and shapes
Discussion and conclusions
B Renormalized shape biases
Non-Gaussian initial conditions
C Non-Gaussian contributions to weak lensing shear
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