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Pathologies of dimension-zero scalar fields

James M. Cline, Anamaria Hell

Abstract

It has been claimed in a series of papers that scalar fields with a fourth-order Lagrangian $\sim(\Box\varphi)^2$ can solve the cosmological constant problem by canceling the loop contributions from standard model fields, and that their fluctuations can be the source of the primordial density perturbations of the Universe, without the need for inflation. We dispute these claims. The spectrum of the theory includes a ghost, which leads to classical instabilities and quantum violation of unitarity. We show that the new scalar particles cannot cancel the standard model contributions to the cosmological constant, unless they include a unitarity-violating ghost at the quantum level. Further, the coupling of such scalars to the particles of the standard model induces a confining fifth force which rules it out as a source of density perturbations in the early Universe.

Pathologies of dimension-zero scalar fields

Abstract

It has been claimed in a series of papers that scalar fields with a fourth-order Lagrangian can solve the cosmological constant problem by canceling the loop contributions from standard model fields, and that their fluctuations can be the source of the primordial density perturbations of the Universe, without the need for inflation. We dispute these claims. The spectrum of the theory includes a ghost, which leads to classical instabilities and quantum violation of unitarity. We show that the new scalar particles cannot cancel the standard model contributions to the cosmological constant, unless they include a unitarity-violating ghost at the quantum level. Further, the coupling of such scalars to the particles of the standard model induces a confining fifth force which rules it out as a source of density perturbations in the early Universe.
Paper Structure (18 sections, 79 equations, 3 figures)

This paper contains 18 sections, 79 equations, 3 figures.

Figures (3)

  • Figure 1: Left: $c_1$ coefficient for scalar perturbations, Eq. (\ref{['scalar-pert']}), versus dimensionless wave number squared, $\hat{k}^2 = k^2 t^2$, in the cosmological background $a(t)\sim t^{2/3}$, $\phi(t)\sim t$. For small $\hat{k}$, it is negative, indicating that the perturbations are ghosts. Right: squared group and phase velocities of the perturbations in this case.
  • Figure 2: Magnitude of phase and group velocities for scalar ghost perturbations around the inflationary background with $a\sim e^{Ht}$ and $\varphi\sim 1/a$.
  • Figure 3: Left: hypothetical loop contribution to $\psi$-Higgs scattering, that violates unitarity because of the wrong-sign $\psi$ propagator. Right: analogous unavoidable contribution to graviton-$\psi$ scattering, that similarly violates unitarity.