Pileup Subtraction for Jet Shapes

Physical Review Letters American Physical Society (APS) 110:16 (2013) 162001

Authors:

Gregory Soyez, Gavin P Salam, Ji-Hun Kim, Souvik Dutta, Matteo Cacciari

Signal-background interference effects for $gg \to H \to W^+ W^-$ beyond leading order

(2013)

Authors:

Marco Bonvini, Fabrizio Caola, Stefano Forte, Kirill Melnikov, Giovanni Ridolfi

Vacuum Varieties, Holomorphic Bundles and Complex Structure Stabilization in Heterotic Theories

(2013)

Authors:

Lara B Anderson, James Gray, Andre Lukas, Burt Ovrut

The Cosmophenomenology of Axionic Dark Radiation

ArXiv 1304.1804 (2013)

Authors:

Joseph P Conlon, MC David Marsh

Abstract:

Relativistic axions are good candidates for the dark radiation for which there are mounting observational hints. The primordial decays of heavy fields produce axions which are ultra-energetic compared to thermalised matter and inelastic axion-matter scattering can occur with $E_{CoM} \gg T_{\gamma}$, thus accessing many interesting processes which are otherwise kinematically forbidden in standard cosmology. Axion-photon scattering into quarks and leptons during BBN affects the light element abundances, and bounds on overproduction of $^4$He constrain a combination of the axion decay constant and the reheating temperature. For supersymmetric models, axion scattering into visible sector superpartners can give direct non-thermal production of dark matter at $T_{\gamma} \ll T_{freezeout}$. Most axions --- or any other dark radiation candidate from modulus decay --- still linger today as a Cosmic Axion Background with $E_{axion} \sim \mathcal{O}(100) eV$, and a flux of $\sim 10^6 cm^{-2} s^{-1}$.

The Cosmophenomenology of Axionic Dark Radiation

(2013)

Authors:

Joseph P Conlon, MC David Marsh