TY - JOUR
T1 - Quantum di usion during in ation and primordial black holes
AU - Pattison, Chris
AU - Vennin, Vincent
AU - Assadullahi, Hooshyar
AU - Wands, David
N1 - Publisher Copyright:
© 2017 IOP Publishing Ltd and Sissa Medialab.
PY - 2017/1/1
Y1 - 2017/1/1
N2 - We calculate the full probability density function (PDF) of in ationary curvature perturbations, even in the presence of large quantum backreaction. Making use of the stochastic-δN formalism, two complementary methods are developed, one based on solving an ordinary differential equation for the characteristic function of the PDF, and the other based on solving a heat equation for the PDF directly. In the classical limit where quantum diffusion is small, we develop an expansion scheme that not only recovers the standard Gaussian PDF at leading order, but also allows us to calculate the first non-Gaussian corrections to the usual result. In the opposite limit where quantum diffusion is large, we find that the PDF is given by an elliptic theta function, which is fully characterised by the ratio between the squared width and height (in Planck mass units) of the region where stochastic effects dominate. We then apply these results to the calculation of the mass fraction of primordial black holes from inflation, and show that no more than ~ 1e-fold can be spent in regions of the potential dominated by quantum diffusion. We explain how this requirement constrains inflationary potentials with two examples.
AB - We calculate the full probability density function (PDF) of in ationary curvature perturbations, even in the presence of large quantum backreaction. Making use of the stochastic-δN formalism, two complementary methods are developed, one based on solving an ordinary differential equation for the characteristic function of the PDF, and the other based on solving a heat equation for the PDF directly. In the classical limit where quantum diffusion is small, we develop an expansion scheme that not only recovers the standard Gaussian PDF at leading order, but also allows us to calculate the first non-Gaussian corrections to the usual result. In the opposite limit where quantum diffusion is large, we find that the PDF is given by an elliptic theta function, which is fully characterised by the ratio between the squared width and height (in Planck mass units) of the region where stochastic effects dominate. We then apply these results to the calculation of the mass fraction of primordial black holes from inflation, and show that no more than ~ 1e-fold can be spent in regions of the potential dominated by quantum diffusion. We explain how this requirement constrains inflationary potentials with two examples.
KW - Inflation
KW - Physics of the early universe
KW - Primordial black holes
U2 - 10.1088/1475-7516/2017/10/046
DO - 10.1088/1475-7516/2017/10/046
M3 - Article
AN - SCOPUS:85040191403
SN - 1475-7516
VL - 2017
JO - Journal of Cosmology and Astroparticle Physics
JF - Journal of Cosmology and Astroparticle Physics
IS - 10
M1 - 046
ER -